Poland-Vietnam Symposium on Natural Science, High Technologies and Humanities for Young Scientists
Hanoi, 16 th -18 th July 2018
Book of abstracts
Hoa Kim Ngan NHU-TARNAWSKA Magdalena KRUPSKA-KLIMCZAK
Poland-Vietnam Symposium on Natural Science, High Technologies and Humanities for Young Scientists
PolVietSym2018
Hanoi, 16 th – 18 th July 2018
Book of abstracts
Publikacja sfinansowane ze środków Uniwersytetu Pedagogicznego im. Komisji Edukacji Narodowej w Krakowie (UP).
Publication was financially supported by the Pedagogical University of Cracow (PUC).
Cover design/Projekt okładki Hoa Kim Ngan Nhu-Tarnawska Front cover photos/Zdj ęcie na okładce © Hoa Kim Ngan Nhu-Tarnawska
Editor/Redaktor Hoa Kim Ngan Nhu-Tarnawska, Magdalena Krupska-Klimczak
Copy right © by authors and editors/autorzy i redaktorzy Kraków 2018
ISBN 978-83-8084-162-8
Printing and Binding/Druk i oprawa Scientific Publisher of the Pedagogical University of Cracow Wydawnictwo Naukowe Uniwersytetu Pedagogicznego im. Komisji Edukacji Narodowej w Krakowie Pochor ąż ych 2, 30 084 Kraków tel./fax (+48) 12 6626383 tel. (+48) 12 6626756 Email: [email protected] Website: http://www.wydawnictwoup.pl
Contents/Spis tre ści/Nội dung
Symposium Aims and Scope...... 5 Cel i Zakres Sympozium ...... 6 Mục tiêu và Đề tài c ủa H ội th ảo ...... 7 Organizing Committee ...... 9 Program ...... 11 Scheme ...... 17
Plenary lecture
Zbigniew TARNAWSKI ...... 21 What do we know about Universe?
Session 1
PHAN Nguyen Duc Duoc ...... 27 Functional integral method in quantum field theory of plasmons in grapheme Fabrication of Graphene/DWCNTs hybrid film for Cholesterol Electrochemical Sensor Kamila KOM ĘDERA ...... 30 Mössbauer studies of iron-based superconductors HOANG Thu Trang ...... 31 Enhanced high-order resonant Q-factor with multiple coupled resonators in slotted two-dimensional photonic crystals for reduced optical switching intensity in bistable devices PHAM The Linh ...... 34 Suppression of photonic stopband reflection in metal-photonic structure Vo Van THIEP ...... 36 Mercury concentration in different parts of brain of big Sus srcofa from Małopolska region, Poland Jarosław INDYK ...... 38 Security dilemma of states in 21 st century on an example of Poland and Vietnam
Session 2
Tran Van PHUC ...... 43 Optical properties and chemical composition of transition layers formed in the process + + + + of irradiation by Ne , Ar , Kr and Xe ions of the multilayer TiO 2/SiO 2 system Sylwia SOWA ...... 44 Superconductivity and structure of U-based alloys with selected (3-5)d-metals and of their hydrides
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DINH Tien Hung ...... 46 Study of designing the scintillation detector using CsI(Tl) crystals and PIN photodiode for ambient gamma dose rate HOANG Huu Thang ...... 47 Synthesis and Characterization of NaLi 0.2 Mn 0.8 O2 Oxide as a Cathode Material for Sodium-ion Batteries Le Thi Thu PHUONG ...... 48 Levels of microelements (Cu, Zn, Fe) and macroelements (Mg, Ca) in organs of Mullet (Mugil cephalus Linnaeus, 1758) in coastal Vietnam Maria KOTKIEWICZ ...... 50 Social activity of NGO members as exemplified by scouts
Session 3
Magdalena KRUPSKA-KLIMCZAK ...... 53 + + + Intermixing in Fe 3O4 films induced by 1MeV Ar , Kr and Au ion irradiation PHAM Hoai Linh ...... 54 Study on fabrication of magnetic fluids based on spinel ferrite Fe 3O4 nanoparticles for applying in magnetic fluid hyperthermia cancer treatment Tomasz MRÓZ ...... 57 Reactor neutron activation analysis in studies of C3-CAM transition of Mesembryantheum crystallinum L Artur JACH-CHRZASZCZ ...... 58 The Treaty of Trianon: the politics of memory in contemporary Hungary
Session 4
NGUYEN Ngoc Anh ...... 63 Experimental study on nuclear level scheme, nuclear level density, and radiative strength function using the gamma–gamma coincidence spectrometer in Vietnam Maria PODGÓRNA ...... 65 Raman scattering investigations of phase transitions in the nanocrystals of PbZrO 3- BiFeO 3 system NGUYEN Minh Nguyet ...... 67 Impact of external factors on electromagnetic properties of metamaterial absorbers in THz region NGUYEN Thi Thu Ha ...... 70 Synthesis the series of compounds Sr 2MO 3FeAs (M = V, Cr) VU Hoang Anh ...... 71 Assessment of impacts to biodiversity forest in Dong Chau forest - Nuoc Trong stream, Kim Thuy commune, Le Thuy district, Quang Binh province Anna MICHNIEWSKA ...... 72 Khan Academy - a platform supporting the teaching and learning process in Poland
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Session 5
PHAM Van Phuc ...... 75 Fabrication of the MA/FA/Cs triple cation perovskite solar cells using one-step and two-step approaches MAI Thi Ly ...... 76 DFT study of electronic structure properties of SrAFe 4As 4 (A = Rb and Cs) superconductors TRAN Van Hau ...... 78 Functional integral method in quantum field theory of Dirac fermions in graphene NGUYEN Viet Dung ...... 79 Effects of filler surface on molecular mobility and resulting deformation and fracture behaviour of thermoplastic polymer composites TRUONG Van Canh ...... 81 Provincial spatial distribution of Gini coefficient in Vietnam Malwina KOSTRZEWSKA-OBERTANIEC ...... 83 Trust of Youth to the local government
Session 6
Mirosław KULIK ...... 87 Effects of high temperature annealing on optical properties of ions implanted GaAs near surface layers Depth profile of atoms and optical properties of near surface layers of implanted semiconductors Cao Van HIEP ...... 90 Simulate Compton suppression spectrometer in Dalat research reactor by using Monte Carlo method KHUONG Viet Hoang ...... 91 Synthesis of ultra-small TiO 2 nanowire/nanorod arrays by hydrothermal method for application to photodetectors NGUYEN Hoai Nam ...... 92 Preparation of Fe 3O4 based drug delivery system loading doxycycline Michał APOLLO ...... 93 Short-Term Impacts of Livestock Grazing on Vegetation and Track Formation in a High Mountain Environment: A Case Study from the Himalayan Miyar Valley (India) Dorota KONIECZNA ...... 94 Asperger’s syndrome as a civilization phenomenon
Session 7
DINH Chi Linh ...... 97 Na-doped La 0.7 Ca 0.3 MnO 3 compounds exhibiting a large magnetocaloric effect near room temperature
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NGUYEN Hong Nhung ...... 99 Preparation of cobalt nanoparticles and effects of rhizome pre-treatment by cobalt on grow and yield of tumeric (curcuma longa l.) DAO Chi Tue ...... 100 Characterization of Pt/Ir diffusion bond-coating for gas turbine
List of participants ...... 103
Map of Hanoi, IMS-VAST ...... 111
Additional information for participant of PolVietSym2018
Cracow ...... 119 Hanoi ...... 123 Halong bay ...... 131 Phong Nha-Ke Bang national park ...... 133 Hoian ...... 134
Post-deadline abstract
Peter MASSANYI ...... 137 Innovative technological and methodological processes in teaching subject “biology of animal production”
Opening and welcoming speeches
Opening speech of Prof. Nguyen Van Hieu ...... 141 Welcoming speech of Prof. Doan Dinh Phuong ...... 143 Welcoming speech of Prof. Robert Stawarz...... 145 Welcoming speech of Mr. Szymon Wudarski ...... 147
Statistics of PolVietSym2018
Summary of Prof. Hoa Kim Ngan Nhu-Tarnawska ...... 153
Updated program PolVietSym2018
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Symposium Aims and Scope Dear Colleagues, Young Scientists and Students, We are glad to welcome you in Hanoi at Poland-Vietnam Symposium on Natural Science, High Technologies and Humanities for Young Scientists (PolVietSym2018) held on 16 th – 18 th July, 2018 at the Insti tute of Materials Science (IMS), Vietnam Academy of Science and Technology (VAST), Hanoi, Vietnam. The symposium is jointly organized by the Pedagogical University of Cracow (PUC) and IMS-VAST, within the scope of the formal bilateral cooperation between PUC and VAST, and of our cooperation with Advanced Center for Physics, Institute of Physics (IOP)-VAST as well as with Institute for European Studies (IES), Vietnam Academy of Social Science (VASS) in Hanoi. The aim of the symposium is to offer an opportunity for students, Ph.D. students and young scientists to meet in an informal environment to discuss the current issues and the latest advances in their research fields, to present their activities as well as to make connections and to initiate cooperation. The symposium topics will be covered are all domains of natural sciences, technology, social sciences and humanities. To encourage the participation of young scientists and especially Ph.D. students and students, no conference fee is required. PolVietSym2018 will be attended by 52 participants (23 from Poland) among which 37 young scientists, Ph.D. students and students from 14 scientific institutions will present their work in the symposium. We feel as a suc cess, since it takes place for the first time and in Hanoi. We would like to express our deep thanks to the Rector and Vice -Rectors of Pedagogical University of Cracow for their financial support for the Ph.D. students and young scientists of PUC to participate to PolVietSym2018, and to the Directors of IMS-VAST and Head of Advanced Center for Physics-IOP-VAST for their financial support and great help in organizing the symposium and extra common activities for the participants during the symposium. We thank the PhD students’ Union of PUC for organizing the trip of participants of PUC to Hanoi. We are particularly grateful to Prof. Nguyen Van Hieu for his unconditional su pport and his valuable and constructive suggestions during the planning and realization of the symposium. We wish to thank the support from the Dea n of Faculty of Mathematics , Physics and Technical Science-PUC. We gratefully acknowledge the support from Embassy of Poland in Hanoi. We wish you a fruitful and enjoyable time at the symposium and in Hanoi. Magdalena Krupska-Klimczak, Nhu-Tarnawska Hoa Kim Ngan, Vu Dinh Lam On behalf of Organizing Committee of PolVietSym2018
Trung Tâm Tiên Ti ến về Vật Lý VIÊ Ṇ VÂ Ṭ LY ́ 5
Cel i Zakres Sympozjum Drodzy koledzy, młodzi naukowcy, doktoranci i studenci, Cieszymy si ę, że mo żemy powita ć wszystkich w Hanoi podczas „sympozjum Polsko-Wietnamskiego Nauk Przyrodniczych, Technologii i Nauk Humanistycznych dla Młodych Naukowców” (PolVietSym2018) odbywaj ącego si ę w dniach 16- 18.07.2018r. w Instytucie Nauk o Materiałach (IMS) Wietnamskiej Akademii Nauk i Technologii (VAST) w Hanoi, Wietnam. Sympozjum to jest organizowane wspólnie przez Uniwersytet Pedagogiczny w Krakowie (PUC) oraz IMS-VAST w ramach współpracy dwustronnej pomi ędzy PUC i VAST, oraz w ramach współpracy z Zaawansowanym Centrum Fizyki Instytutu Fizyki (IOP)-VAST i z Instytutem Europeistyki (IES) Wietnamskiej Akademii Nauk Społecznych (VASS) w Hanoi. Celem sympozjum jest zaoferowanie studentom, doktorantom i młodym naukowcom okazji do spotkania si ę w przyjaznej atmosferze, aby omówi ć bie żą ce zagadnienia i najnowsze osi ągni ęcia w swoich dziedzinach nauki, przedstawi ć swoje wyniki bada ń oraz nawi ąza ć kontakty i zainicjowa ć współprac ę. Przedmiotem sympozjum b ędą wszystkie dziedziny nauk przyrodniczych, technologii, nauk społecznych i humanistycznych. Aby zach ęci ć do udziału studentów, doktorantów i młodych naukowców, opłata konferencyjna nie jest wymagana. Udział w PolVetSym2018 we źmie 52 uczestników (23 z Polski), w śród których 37 młodych naukowców, doktorantów i studentów (z 14 instytucji naukowych) zaprezentuje swoj ą prac ę na sympozjum. Cieszymy si ę sukcesem, poniewa ż odbywa si ę to po raz pierwszy i w Hanoi. Pragniemy wyrazi ć gł ębok ą wdzi ęczno ść Rektorowi i Prorektorom Uniwersytetu Pedagogicznego w Krakowie za wsparcie finansowe udziału doktorantów i młodych naukowców w PolVietSym2018 oraz Dyrektorom IMS-VAST i Kierownikowi Zaawansowanego Centrum Fizyki-IOP-VAST za wsparcie finansowe i pomo ć w zorganizowaniu sympozjum oraz współnych działa ń dla uczestników podczas sympozjum. Chcemy podzi ękowa ć Samorz ądów Doktorantów PUC za pomoc w zorganizowaniu wyjazdu do Hanoi. Jeste śmy szczególnie wdzi ęczni prof. Nguyen Van Hieu, za jego bezwarunkowe wsparcie oraz cenne i konstruktywne sugestie podczas planowania i realizacji sympozjum. Wyra żamy podzi ękowanie Dziekanowi Wydziału Matematyczno-fizyczno-Technicznego-PUC za wsparcie. Serdecznie dzi ękujemy Polskiej Ambasadzie w Hanoi za udzielenie nam wsparcia.
Życzymy owocnego i przyjemnego sp ędzania czasu na sympozjum oraz w Hanoi.
Magdalena Krupska-Klimczak Nhu-Tarnawska Hoa Kim Ngan Vu Dinh Lam W imieniu Komitetu Organizacyjnego PolVietSym2018
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Mục tiêu và Đề tài c ủa Hội th ảo Các đồng nghi ệp, các cán b ộ khoa h ọc tr ẻ và các em sinh viên thân m ến, Nhi ệt li ệt chào đón toàn th ể đại bi ểu tham d ự hội th ảo Ba lan-Vi ệt Nam v ề khoa h ọc t ự nhiên, công ngh ệ, khoa h ọc xã h ội và nhân v ăn, t ổ ch ức vào ngày 16-18 tháng 7 n ăm 2018 t ại Vi ện Khoa H ọc V ật Li ệu (IMS) thu ộc Vi ện Hàn Lâm Khoa H ọc và K ỹ Thu ật Vi ệt Nam (VAST) t ại thành ph ố Hà n ội. Hội th ảo do tr ường Đại H ọc S ư Ph ạm t ại thành ph ố Cracow ở Ba lan (PUC) và vi ện IMS-VAST ph ối h ợp t ổ ch ức, trên c ơ s ở hi ệp định h ợp tác song ph ươ ng gi ữa PUC và VAST, và h ợp tác v ới Trung tâm tiên ti ến v ề Vật lý-Vi ện V ật lý(IOP)-VAST và với Vi ện Nghiên c ứu châu Âu (IES) Vi ện Hàn Lâm Khoa H ọc Xã H ội Vi ệt nam (VASS) tại Hà n ội. Mục tiêu c ủa h ội th ảo là t ạo c ơ h ội cho đại bi ểu tham d ự, đặc bi ệt là các sinh viên, nghiên c ứu sinh và nh ững cán b ộ khoa h ọc tr ẻ được g ặp g ỡ trong không khí thân mật để th ảo lu ận các v ấn đề hi ện t ại, nh ững ti ến b ộ mới nh ất trong l ĩnh v ực nghiên cứu c ủa mình, trình bày các ho ạt động c ủa b ản thân, c ũng nh ư được ti ếp xúc trao đổi và đặt n ền móng h ợp tác. Các ch ủ đề trong h ội th ảo s ẽ được đề cập t ới là t ất c ả các lĩnh v ực khoa h ọc t ự nhiên, công ngh ệ, khoa h ọc xã h ội và nhân v ăn. Để khuy ến khích s ự tham gia c ủa cán b ộ tr ẻ, đặc bi ệt là nghiên c ứu sinh và sinh viên, h ội th ảo không yêu c ầu các đại bi ểu đóng góp ti ền h ội ngh ị phí. Có 52 đại bi ểu tham d ự PolVietSym2018 (23 đại bi ểu t ừ Ba Lan) trong đó có 37 cán b ộ khoa h ọc tr ẻ, nghiên c ứu sinh và sinh viên (t ừ 14 viện khoa h ọc/tr ường đại học) trình bày báo cáo trong h ội th ảo. Chúng tôi đánh giá đó là m ột thành công, nh ất là vì h ội th ảo này di ễn ra l ần đầu tiên và tại Hà N ội. Chúng tôi bày t ỏ lòng bi ết ơn sâu s ắc t ới Hi ệu tr ưởng và các Phó Hi ệu tr ưởng tr ường Đại h ọc S ư ph ạm t ại Cracow đã h ỗ tr ợ tài chính cho các nghiên c ứu sinh và ti ến s ĩ tr ẻ của tr ường tham d ự PolVietSym2018, t ới ban lãnh đạo IMS-VAST và lãnh đạo Trung tâm tiên ti ến v ề Vật lý-IOP-VAST đã h ỗ tr ợ tài chính và công s ức t ổ ch ức hội th ảo c ũng nh ư các ho ạt động chung cho các đại bi ểu tham gia h ội th ảo. Chúng tôi cảm ơn H ội Đồng Nghiên C ứu Sinh c ủa tr ường PUC đã giúp đỡ tổ ch ức chuy ến đi c ủa đoàn tr ường PUC đến Hà N ội. Chúng tôi xin bày t ỏ sự bi ết ơn đặc bi ệt đến Giáo s ư Vi ện S ĩ Nguy ễn V ăn Hi ệu đã dành cho chúng tôi s ự hỗ tr ợ vô biên và l ời ch ỉ d ẫn h ữu ích trong quá trình l ập k ế ho ạch và th ực hi ện hi ện t ổ ch ức h ội th ảo này. Chúng tôi trân tr ọng cảm ơn sử ủng h ộ và h ỗ tr ợ c ủa Tr ưở ng Khoa khoa Toán-Vật lý-Kỹ thu ật-PUC. Chúng tôi chân thành cảm ơn sự hỗ tr ợ của Đại s ứ quán Ba Lan t ại Hà N ội.
Chúc toàn th ể đại bi ểu có được th ời gian hi ệu qu ả và thú v ị tại h ội th ảo c ũng nh ư t ại Hà N ội.
Magdalena Krupska-Klimczak Nhu-Tarnawska Hoa Kim Ngan Vu Dinh Lam Thay m ặt ban t ổ ch ức PolVietSym2018
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ORGANIZING COMMITTEE
Patron/Honorary chairman Nguyen Van Hieu (VAST, Hanoi) Kazimierz Karolczak (Rector of PUC, Krakow)
Advisory Committee Nguyen Thanh Binh (IOP-VAST, Hanoi) Nguyen An Ha (IES-VASS, Hanoi) Magdalena Krupska-Klimczak (PUC, Krakow) Vu Dinh Lam (IMS-VAST, Hanoi) Peter Massanyi (SUA, Nitra) Hoa Kim Ngan Nhu-Tarnawska (PUC, Krakow) Katarzyna Potyrała (PUC, Krakow) Bogusław Skowronek (PUC, Krakow) Robert Stawarz (PUC, Krakow) Mariurz Wołos (PUC, Krakow)
Organizing Committee Vu Dinh Lam (IMS-VAST, Hanoi, chairman) Hoa Kim Ngan Nhu-Tarnawska (PUC, Krakow, co-chairwoman) Magdalena Krupska-Klimczak (PUC, Krakow) Sylwia Sowa (PUC, Krakow) Kamila Kom ędera (PUC, Krakow)
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VENUE Institute of Materials Science (IMS), Vietnam Academy of Science and Technology (VAST), 18 Hoang Quoc Viet Road, Cau Giay District, Hanoi, Vietnam.
CONTACT ADDRESSES in Hanoi: Institute of Materials Science, VAST, 18 Hoang Quoc Viet Road, Cau Giay District, Hanoi, Vietnam. Phone: (+84) 948288776 (Vu Dinh Lam) Fax: (+84-4) 38360705 E-mail: [email protected] Website: http://www.polvietsym2018.ac.vn
in Poland: Nanostructure Laboratory, Institute of Physics, Pedagogical University of Cracow, Podchor ąż ych 2, 30 084 Kraków, Poland Phone: (+48) 12 6627801 (Kim Nhu-Tarnawska, Magdalena Krupska-Klimczak) E-mail: [email protected] Website: www.polvietsym2018.up.krakow.pl
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PROGRAM
Monday, 16 th July 2018
Registration Institute of Materials Science (IMS), Vietnam Academy of Science and 8:00-17:00 Technology (VAST), 18 Hoang Quoc Viet Road, Cau Giay district, Hanoi, Vietnam. Building B2.
S-O: Opening session
Chairman: Vu Dinh Lam, Nhu-Tarnawska Hoa Kim Ngan Welcome address Honorary guests of PolVietSym2018: Prof. Nguyen Van Hieu, patron/honorary chairman of PolVietSym2018. Prof. Đoàn Đình Ph ươ ng, Director of IMS-VAST. Prof. Robert Stawarz, Vice-Rector of the Pedagogical University of 9:00-9:30 Cracow. Mr. Szymon Wudarski, chargé d'affaires ad interim of the Republic of Poland in the Socialist Republic of Vietnam. Dr. Nguyen Bich Ha, IMS-VAST, Deputy Editor-in-Chief of the journal Advances in Natural Sciences: Nanosci.&Nanotech. 9:30-10:15 Zbigniew Plenary What do we know about our Universe? TARNAWSKI Lecture 10:15 Symposium photo 10:15-11:00 Coffee/tea break Session 1
Chairman: Nguyen Thanh Binh Functional integral method in quantum field theory 11:00-11:15 PHAN Nguyen of plasmons in grapheme O-01 Duc Duoc Fabrication of Graphene/DWCNTs hybrid film for Cholesterol Electrochemical Sensor 11:15-11:30 Kamila Mössbauer studies of iron-based superconductors O-02 KOM ĘDERA Enhanced high-order resonant Q-factor with 11:30-11:45 HOANG Thu multiple coupled resonators in slotted two- O-03 Trang dimensional photonic crystals for reduced optical switching intensity in bistable devices 11:45-12:00 Suppression of photonic stopband reflection in PHAM The Linh O-04 metal-photonic structure 11
12:00-12:15 Mercury concentration in different parts of brain of Vo Van THIEP O-05 big Sus srcofa from Małopolska region, Poland 12:15-12:30 Security dilemma of states in 21 st century on an Jarosław INDYK O-06 example of Poland and Vietnam 12:30-14:00 Lunch break
Session 2
Chairman: Ryszard Radwa ński Optical properties and chemical composition of 14:00-14:15 transition layers formed in the process of irradiation Tran Van PHUC O-07 by Ne +, Ar +, Kr + and Xe + ions of the multilayer TiO 2/SiO 2 system 14:15-14:30 Superconductivity and structure of U-based alloys Sylwia SOWA O-08 with selected (3-5) d-metals and of their hydrides Study of designing the scintillation detector using 14:30-14:45 DINH Tien Hung CsI(Tl) crystals and PIN photodiode for ambient O-09 gamma dose rate Synthesis and Characterization of NaLi Mn O 14:45-15:00 HOANG Huu 0.2 0.8 2 Oxide as a Cathode Material for Sodium-ion O-10 Thang Batteries Levels of microelements (Cu, Zn, Fe) and 15:10-15:15 Le Thi Thu macroelements (Mg, Ca) in organs of Mullet (Mugil O-11 PHUONG cephalus Linnaeus, 1758) in coastal Vietnam 15:15-15:30 Maria Social activity of NGO members as exemplified by O-12 KOTKIEWICZ scouts
15:30-16:00 Coffee/tea break
Session 3
Chairman: Pham Duy Long Magdalena 16:00-16:15 Intermixing in Fe O films induced by 1MeV Ar +, KRUPSKA- 3 4 O-13 Kr + and Au + ion irradiation KLIMCZAK Study on fabrication of magnetic fluids based on 16:15-16:30 PHAM Hoai Linh spinel ferrite Fe O nanoparticles for applying in O-14 3 4 magnetic fluid hyperthermia cancer treatment Reactor neutron activation analysis in studies of C - 16:30-16:45 3 Tomasz MRÓZ CAM transition of Mesembryantheum crystallinum O-15 L 16:45-17:00 Artur JACH- The Treaty of Trianon: the politics of memory in O-16 CHRZASZCZ contemporary Hungary Group activity. Visit to One Pillar Pagoda. Walk to the West lake. 17:00-19.30 Dinner at Truc Bach lake. 12
Tuesday, 17 th July 2018
Session 4
Chairman: Andrzej Korna ś Experimental study on nuclear level scheme, 9:00-9:15 NGUYEN Ngoc nuclear level density, and radiative strength function O-17 Anh using the gamma–gamma coincidence spectrometer in Vietnam 9:15-9:30 Maria Raman scattering investigations of phase transitions O-18 PODGÓRNA in the nanocrystals of PbZrO 3-BiFeO 3 system 9:30-9:45 NGUYEN Minh Impact of external factors on electromagnetic O-19 Nguyet properties of metamaterial absorbers in THz region 9:45-10:00 NGUYEN Thi Synthesis the series of compounds Sr 2MO 3FeAs (M O-20 Thu Ha = V, Cr) Assessment of impacts to biodiversity forest in 10:00-10:15 VU Hoang Anh Dong Chau forest - Nuoc Trong stream, Kim Thuy O-21 commune, Le Thuy district, Quang Binh province 10:15-10:30 Anna Khan Academy - a platform supporting the teaching O-22 MICHNIEWSKA and learning process in Poland 10:30-11:00 Coffee/tea break
Session 5
Chairman: Tran Quoc Tien Fabrication of the MA/FA/Cs triple cation 11:00-11:15 PHAM Van Phuc perovskite solar cells using one-step and two-step O-23 approaches 11:15-11:30 DFT study of electronic structure properties of MAI Thi Ly O-24 SrAFe 4As 4 (A = Rb and Cs) superconductors 11:30-11:45 Functional integral method in quantum field theory TRAN Van Hau O-25 of Dirac fermions in grapheme Effects of filler surface on molecular mobility and 11:45-12:00 NGUYEN Viet resulting deformation and fracture behaviour of O-26 Dung thermoplastic polymer composites 12:00-12:15 TRUONG Van Provincial spatial distribution of Gini coefficient in O-27 Canh Vietnam 12:15-12:30 Malwina KOSTRZEWSKA- Trust of Youth to the local government O-28 OBERTANIEC 12:30-14:00 Lunch break
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Visit to Vietnam museum of Ethnology (at Nguyen Van Huyen Rd, 14:00-17.30 1.2km from IMS, see the map in page 113).
18:00-21:00 Symposium banquet
Wednesday, 18 th July 2018
Session 6
Chairman: Peter Massanyi Effects of high temperature annealing on optical properties of ions implanted GaAs near surface 9:00-9:15 Mirosław KULIK layers O-29 Depth profile of atoms and optical properties of near surface layers of implanted semiconductors 9:15-9:30 Simulate Compton suppression spectrometer in Cao Van HIEP O-30 Dalat research reactor by using Monte Carlo method Synthesis of ultra-small TiO nanowire/nanorod 9:30-9:45 KHUONG Viet 2 arrays by hydrothermal method for application to O-31 Hoang photodetectors 9:45-10:00 NGUYEN Hoai Preparation of Fe 3O4 based drug delivery system O-32 Nam loading doxycycline Short-Term Impacts of Livestock Grazing on 10:00-10:15 Vegetation and Track Formation in a High Michał APOLLO O-33 Mountain Environment: A Case Study from the Himalayan Miyar Valley (India) 10:15-10:30 Dorota Asperger’s syndrome as a civilization phenomenon O-34 KONIECZNA 10:30-11:00 Coffee/tea break Session 7
Chairman: Zbigniew Tarnawski 11:00-11:15 Na-doped La Ca MnO compounds exhibiting a DINH Chi Linh 0.7 0.3 3 O-35 large magnetocaloric effect near room temperature Preparation of cobalt nanoparticles and effects of 11:15-11:30 NGUYEN Hong rhizome pre-treatment by cobalt on grow and yield O-36 Nhung of tumeric (curcuma longa l.) 11:30-11:45 Characterization of Pt/Ir diffusion bond-coating for DAO Chi Tue O-37 gas turbine Summary (Nhu-Tarnawska Hoa KIM NGAN) Awards for the best presentations (Zbigniew 11:45-12:15 TARNAWSKI, Nguyen Thanh BINH) Closing (Vu Dinh LAM) 14
12:15-14:00 Lunch break
Visit to the Ancient University of Vietnam - Van Mieu-Quoc Tu Giam 14:00-17:30 (see page 127).
18:00-20:00 Group activity. Dinner in the old quarter.
Thursday, 19 th July 2018
Excursion to Halong bay including 4h excursion by boat around the 7:00-20:00 bay and visit of Heaven Palace Cave (see page 131).
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Monday, Tuesday, Wednesday, Thursday, 16 th July 2018 17 th July 2018 18 th July 2018 19 th July 2018 Welcome address O-17 Nguyen Ngoc Anh O-29 Mirosław Kulik
N.V. Hieu, D.D. Phuong, O-18 Maria Podgórna O-30 Cao Van Hiep R. Stawarz, Sz. Wudarski. O-19 Nguyen M. Nguyet O-31 Khuong Viet Hoang
S4 S6 S-O Plenary lecture: O-20 Nguyen T.T. Ha O-32 Nguyen Hoai Nam 9:00-10:30 9:00-10:30 9:00-10:30 9:00-10:15 9:00-10:15 Z. Tarnawski O-21 Vu Hoang Anh O-33 Michał Apollo Excursion O-22 A. Michniewska O-34 Dorota Konieczna to Halong bay 10:15-11:00: coffee/tea break 10:30-11:00: coffee/tea break 10:30-11:00: coffee/tea break including 4hrs boat-trip Vietnam. Vietnam. O-01 Phan Ng. Duc Duoc O-23 Pham Van Phuc O-35 Dinh Chi Linh around the bay O-02 Kamila Kom ędera O-24 Mai Thi Ly O-36 Nguyen H. Nhung and visit of
O-03 Hoang Thu Trang O-25 Tran Van Hau O-37 Dao Chi Tue Heaven Palace S7 S1 S5 O-04 Pham The Linh O-26 Nguyen Viet Dung Summary. Best Cave O-05 Vo Van Thiep O-27 Truong Van Canh Presentation Awards. 11:00-12:15 11:00-12:30 11:00-12:30 (see page 131).
my of Science and Technology (VAST), (VAST), Technology and of my Science O-06 Jarosław Indyk O-28 M. Kostrzewska-O Closing.
12:30-14:00 lunch break 12:30-14:00 lunch break 12:15-14:00 lunch break
Registration. O-07 Tran Van Phuc O-08 Syliwa Sowa
O-09 Dinh Tien Hung Visit to Vietnam Visit to Ancient University
S2 O-10 Hoang Huu Thang Museum of Ethnology of Vietnam - Van Mieu- 8:00-17:00 8:00-17:00 O-11 Le Thi Thu Phuong (at Nguyen Van Huyen Quoc Tu Giam (see page 14:00-15:40 O-12 Maria Kotkierwicz Rd, 1.2km from IMS- 127). 15:30-16:00 coffee/tea break VAST, see the map in page 113). O-13 M. Krupska-Klimczak 14:00-17.30 14:00-17.30
O-14 Pham Hoai Linh 18 Hoang Quoc Viet Road, Cau Giay district, Hanoi, district, Hanoi, Giay Cau Road, Viet 18Quoc Hoang 17:00 S3
- O-15 Tomasz Mróz
16 O-16 A. Jach-Chrzaszcz
Group-activity. Group-activity. One Pilar Pogoda. Dinner at Symposium banquet. Dinner in the old quater. Institute of Materials Science (IMS), Vietnam Acade Vietnam (IMS), Science Materials of Institute from 17:00 Truc Bach lake. from 18:00 from 18:00
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18
Plenary Lecture
Zbigniew Tarnawski What do we know about Universe?
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20
What do we know about Universe?
Zbigniew TARNAWSKI 1,2 AGH University of Science and Technology, Faculty of Physics and Applied Computer Science 1 and Academic Centre for Materials and Nanotechnology 2, al. Mickiewicza 30, 30-059 Kraków, Poland *Email: [email protected]
One thing we know about the Universe is that it is really big, possibly infinite, without an edge. The story of our Universe energy and matter evolution since a fraction of a second after Big Bang is well described [1]. Most cosmologists accept the Inflationary Universe model (Fig. 1), which brings us closer to the Beginning [2, 3] – the spontaneous creation from the so-called false vacuum. This model could solve some problems (Horizon, Flatness, Homogeneity, Isotropy of the Universe), which are not explained well enough in the standard Bing Bang model. The most important ingredients of both models is Einstein’s General Relativity (GR) and Standard Model of elementary particles, which is the quantum field theory combining Quantum Chromo-Dynamics (QCD) and Quantum Electro-Dynamics (QED) into one mathematical scheme of electro-weak and strong interactions – the Grand Unified Theory (GUT). The current structure of Universe, abundance of every element, and the whole “Zoo” of every possible Star or Black Hole, is known to us. We know as well “our place” on the Earth located in the Solar system which locates in the galaxy that we call Milky Way. Milky Way is part of the Local Group of galaxies, which is a component of still bigger structures in the Universe. We can be proud of ourselves as Human who discovered and understand almost everything about Universe.
Fig.1. Illustration of Inflationary Universe model (Image source [4]).
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But… 1/ Where did the Life and Human Intelligence come from? Which physical law brings to the existence of the Intelligence who can pose all questions, look for answers and draw a picture of our Universe as well as of every possible universe? If physicists believe that the Intelligence is a product of evolution in accordance to the physical laws, they should be the ones who give the answers and proofs. 2/ If there will be Theory of Everything (TOE)? The two basic theories GR and GUT are not compatible and the dream of combining them together into TOE is still a dream. It is commonly accepted that it would be Quantum Gravity theory and the search for it brings us to the next question. 3/ Why we have to assume the existence of unobservable objects? Physics is an experimental science and physicists always look for experimental proofs. They should avoid to postulate existence of things, objects, entities which cannot be confirmed experimentally. However, even our current and well-established theories assume the existence of not observed (yet) beings. One example is Dark Matter and Dark Energy, which are introduced as necessary ingredients to understand the current behavior of Universe. The elementary particles’ existence (protons, neutrons, electrons and photons) is an indirect proof that vacuum is filled in by quantum fields (field of electroweak forces, quark-antiquark condensate, weak superconducting condensate and Higgs field, quantum fluctuations…) with a huge energy density beyond the imagination. Assuming the existence of unobservable beings is like opening “Pandora box” for physicists. Multiple theories based on unobservable mathematical objects, treated as real and as the source of our material world, were developed. A wide spectrum of String theories in multiple dimensions (M-theories), many versions of quantum gravity theories starting from the so-called Planck Scale, has engaged thousands of best brains in physics for many years. Combination of these ideas with the science of Black Holes and Quantum Physics brought the ideas of holographic universe or multiverse [5]. We cannot chose which one gives hope for TOE and which direction is the future solution. 4/ If we have reached the finish line of our understanding? Well established physics theory-Quantum Mechanics (QM) has been used in practice for about 100 years and applied in every piece of electronic equipment, but its understanding is still doubtful. In order to feel more comfortable with it, physicists were ready to re-define the meaning of the word “understanding”. According to R. Feynman, nobody understand QM. Especially its nonlocality was so strongly opposed by Einstein, although it was confirmed experimentally. This is why there are many interpretations of QM and the discussions is ongoing until now. In spite of all we know, it is considered that there is a crisis in physics and thus some ingenuous breakthrough is necessary to overcome it [6]. It looks like we are at the beginning, not at the finish line of our understanding what is really going on with our reality. 5/ Is the space quantized? It is worth to mention here the ideas of Digital Universe, which came from the computer scientists, e.g. Alan Turing, Konrad Zuse, Edward Fredkin and latelly Stephen Wolfram, which are taken more and more seriously by physisists. The question is that if the Universe is an universal Turing machine or cellural automata 22
obeying certain rules? If it can be explained by Quantum Gravity theories, which deal with the space(time) structure on the Planck scale. The actual question is if space itself is quantised? It would not be possible to understand the structure of vacuum (space) and the Universe, before accepting its granularity. It reminds the story of atoms. Namely, it was not possible to discover and understand the structure of atoms, before that, the existence of atoms was accepted. Indeed, the atomic theory of matter has been obvious for some philosophers since 500BC and for some chemists since begining of 19th century. But many physicists have refused to consider the existence of atoms, which existence could not be then proved experimentally. Even now physicists officially accept the year 1905 (when Einstein’s work explaining Brownian motion appeared) as the date of the first theoretical proof of atom existence. 7/ Is there ether or else? The concept of ether has been existed for thousands years. The physisists have emptied the space to nothingness after 1905 (the year of Einstein Special Relativity (SR)). Nowedays, we are slowly filling this nothigness again with virtual particles and fields (Fig. 2).
Fig. 2. Suggestion a structure for the vacuum (Image source [7]).
But we are not able to accept, that space itself is built of quanta and has the energy density possibly in the range of 10 112 J/m 3. The first candidate for space quanta is the extended quantum foam model proposed in 1955 by J.A. Wheeler, in which the gravity meets quantum physics, and in which at the Planck length (10 -34 m) the space curvature forms the space-time metric. There is a common agreement and understanding that the really empty space/vacuum/void/nothingness is unstable. Some believes that the unstable vacum can produce Universes [2,3]. Others think that it spontaneously forms quantum condensates of Standard Model of elementary particles (Fig. 3) [8]. Someone may claim and prove that all can happens simultaneously: the empty space condensates into atoms of space of the size of Planck length (Planck quanta which are fermionic black holes rotating with the speed of light and possessing spin of ½ ħ). The process of collapsing of the flat space into quantum crystal (cellular automata) may give the energy necessary to produce all the matter and energy, as well as all quantum fields. All of them being the excitations of the space fabric. 23
Fig. 3. Deep structure of the quantum grid – typical pattern of activity in the gluon fields of QCD [8].
We are living in quantum world. Planck constant observed in every quantum process is arising from the property of space itself. Quantized Space is an Universal Computer and Universe is a computing process, as it was summarized by J.A. Wheeler with his words: It from Bit [9].
Acknowledgements This work was supported by the AGH UST statutory task No.11.11.220.01/6 within subsidiary of the Ministry of Science and Higher Education.
References [1] S. Weinberg, The First Three Minutes: A Modern View of the Origin of the Universe , Basic Books (1977). [2] A.H. Guth, The Inflationary Universe: A Possible Solution to the Horizon and Flatness Problems , Phys. Rev. D, 23 , 347 (1981). [3] A.D. Linde, A New Inflationary Universe Scenario: A Possi6le Solution to the Horizon, Flatness, Homogeneity, Isotropy, and…problems” , Physics Letters, 108B , 389 (1982). [4] Just Science, http://www.justscience.in/articles/dark-energy-really-know- universe-live/2017/12/27 [5] Scientific American, Is Our Universe a Hologram? Video produced by Eric R. Olson, 2014. https://www.scientificamerican.com/video/is-our-universe-a-hologram-video/ [6] Lee Smolin, Time reborn. From the crisis in physics to the future of the universe. Mariner Books (2013). [7] Resonance Science Foundation, New insights suggesting a structure for the vacuum , https://resonance.is/new-insights-suggesting-structure-vacuum/ [8] F. Wilczek, The lightness of being. Mass, Ether and the unification of forces. Basic Books (2008). [9] J.A. Wheeler, Information , Physics, Quantum: the Search for Links. http://cqi.inf.usi.ch/qic/wheeler.pdf
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Session 1
O-01 PHAN Nguyen Duc Duoc Functional integral method in quantum field theory of plasmons in graphene Fabrication of Graphene/DWCNTs hybrid film for Cholesterol Electrochemical Sensor
O-02 Kamila KOM ĘDERA Mössbauer studies of iron-based superconductors
O-03 HOANG Thu Trang Enhanced high-order resonant Q-factor with multiple coupled resonators in slotted two-dimensional photonic crystals for reduced optical switching intensity in bistable devices
O-04 PHAM The Linh Suppression of photonic stopband reflection in metal-photonic structure
O-05 Vo Van THIEP Mercury concentration in different parts of brain of big Sus srcofa from Małopolska region, Poland
O-06 Jarosław INDYK Security dilemma of states in 21 st century on an example of Poland and Vietnam
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26
Functional integral method in quantum field theory of plasmons in graphene
PHAN Nguyen Duc Duoc 1,2,* , Nguyen Van Hieu 1,2 1Institute of Materials Science, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet,Cau Giay, Hanoi, Vietnam 2VNU-University of Engineering and Technology, 144 Xuan Thuy, Cau Giay, Hanoi, Vietnam *Email: [email protected]
In the present work we apply the functional integral method to the study of quantum field theory of collective excitations of spinless Dirac fermion in graphene at = vanishing absolute temperature and at Fermi level EF 0 . After introducing the Hermitian scalar field ϕ(x ) describing these collective excitations we establish the ϕ expression of the functional integral Z containing a functional series I[ϕ ] . The explicit expressions of several terms of this functional series were derived. Then we ϕ ϕ consider the functional series I[ ] in second order approximation and denote I0[ ] the corresponding approximate expression of I[ϕ ] . We shall demonstrate that in this approximation the scalar field ϕ(x ) can be devided into two parts: a background field ϕ ϕ ξ 0 (x ) corresponding to the extremum of I0[ ] and another scalar field (x ) ϕ ϕ ξ describing the fluctuation of (x ) around the background 0 (x ) . We call (x ) the fluctuation field. Then we establish the relationship between this fluctuation field ξ(x ) and the quantum field of plasmons in graphene. Considering some range of values of frequency (energy) and wave vector (momentum) of plasmons, when the analytical calculations can be performed, we derived the differential equation for the quantum field of graphene plasmons. From this field equation we establish the relation between frequency and wave vector of plasmons in the long wavelength limit.
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Fabrication of Graphene/DWCNTs hybrid film for Cholesterol Electrochemical Sensor
Nguyen Duc Duoc PHAN 1,2,* , Van Hau TRAN 1,2 , Thi Thanh CAO 1, Van Trinh PHAM 1, Hai Binh NGUYEN 1 and Van Chuc NGUYEN 1,* 1Institute of Materials Science, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet, Cau Giay, Hanoi, Vietnam 2VNU-University of Engineering and Technology, 144 Xuan Thuy, Cau Giay, Hanoi, Vietnam *Email: [email protected]; [email protected]
Graphene is a true two dimensional material with unique properties, such as very large surface to volume ratio, high conductivity and electron mobility at room temperature. While carbon nanotubes (CNTs) were discovered as an excellent material with one dimensional electrical conductivity, large surface area and high electron mobility. Therefore, it is believed that graphene and CNTs as sensor components can make sensors accurate, fast and increase ability of surface contact due to their remarkable properties. In this work, the graphene/double wall carbon nanotubes (G/DWCNTs) hybrid film was fabricated by low vacuum chemical vapour deposition (CVD) method, it was investigated by field emission scanning electron microscope (FE-SEM), Raman spectroscopy and electrical conductivity, the result shown that the multilayer graphene bonded DWCNTs was grown on the copper substrate (figure 1). Cholesterol Oxidase (ChOx) is immobilized on graphene and G/DWCNTs modified electrode to detect the cholesterol in solution. The FE-SEM, electrochemical impedance spectroscopy, square wave voltammetric (SWV) and CV techniques were used for characterizing the electrochemical biosensors. The current peak of G/DWCNTs modified electrode of cyclic voltammetric (CV) spectrum with 5 mM potassium ferricyanide in 0.1M photphate buffer solutions (PBS) of pH 7 increased significantly comparing to graphene modified electrode (~ 2 times), the SWV current peaks increase linearly with the addition of cholesterol in the concentration range 2-10 mM with the low detection limit. Therefore, G/DWCNTs will be promised as a good sensing film and reliability for electrochemical biosensor applications.
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Figure 1: FE-SEM image of graphene (a) and graphene/DWCNTs hybrid film (b).
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Mössbauer studies of iron-based superconductors
Kamila KOM ĘDERA 1,* , Artur BŁACHOWSKI 1, Krzysztof RUEBENBAUER 1, Jan ŻUKROWSKI 2 1 Mössbauer Spectroscopy Division, Institute of Physics, Pedagogical University, 30 084 Krakow, Poland 2 Academic Centre for Materials and Nanotechnology, AGH University of Science and Technology, 30 059 Krakow, Poland *Email: [email protected]
Iron-based superconductors make four major families based on the corrugated nearly-two-dimensional sheets of either strongly bound iron-pnictogen or iron- chalcogen atoms. Usually, superconductivity is induced by doping or applying pressure to the parent compound, except the simplest compounds of the ‘11’ family. One can dope any kind of atom within the compound in isovalent, hole-doping or electrondoping fashion. Parent compounds exhibit itinerant magnetic order of the 3d (iron) character. It appears as spin density wave (SDW) of the antiferromagnetic type incommensurates with the respective lattice period and of the complex shape. For a majority of cases, it is a longitudinal SDW propagating along the a-axis of the orthorhombic unit cell being created at the magnetic order from the tetragonal cell – due to the magneto-elastic forces. On the other hand, the 3d magnetism and orthorhombic distortion are gone for superconductors as shown by the Mössbauer spectra obtained versus temperature, and by spectra obtained in the strong external magnetic field at low temperatures – stronger than the first critical field for these second kind superconductors. However, superconductivity is intimately related to these layered structures with the electronic charge modulation, leading to the charge density wave (CDW) on iron nuclei – observed as variation of the isomer shift. What is more, one observes closely related modulation of the electric field gradient on iron nuclei called electric field gradient wave (EFGW). The shape of these modulations changes rapidly at the superconducting gap: opening and relaxing back once the bosonic system of Cooper pairs is well separated from the rest of the electronic system. It was found that localized 4f magnetic moments order within the superconducting phase in a similar fashion as in the normal phase.
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Enhanced high-order resonant Q-factor with multiple coupled resonators in slotted two-dimensional photonic crystals for reduced optical switching intensity in bistable devices
Thu Trang HOANG 1,2,* , Quang Minh NGO 1,2 1Institute of Materials Science, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet, Cau Giay, Hanoi, Vietnam 2Graduate University of Science and Technology, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet, Cau Giay, Hanoi, Vietnam *Email: [email protected]
We review in part of our current study on the enhanced high-order resonant Q- factor with multiple coupled resonators by using coupled-mode theory (CMT) in time. Two types of coupled resonators under investigation are coupled resonator optical waveguides (CROWs) and side-coupled resonators with waveguide (SCREW). The number of resonators ( n) and the phase shift ( ϕ) between two adjacent resonators are examined due to their influences on the shapes and Q-factors of the spectral responses. The finite-difference time-domain (FDTD) method is used to perform the proposed designs for practical applications. The proposed coupled resonators in slotted two- dimensional (2D) photonic crystals (PhCs) are designed to enhance the electromagnetic intensity and to confine the light into small cross-sectional area with low refractive index of the nonlinear material so that the efficient optical bistable devices could be achieved. Optical resonant structures which are made by the coupling between 2D PhC cavities and waveguides have been of great interest to researchers in photonic fields. These structures can exhibit high quality ( Q) factors and small modal volumes ( V) , which are promising to be key platforms for the large-scale photonic integrated circuits (PICs) such as high-performance filters, all-optical analogue to electromagnetically induced transparency, and low-input-power nonlinear photonic devices. There is a demand for a less resonant wavelength shift during the switching operation of all-optical switching/bistable devices so that a sharp resonance feature of the resonator is preferable. In order to get the sharpness, it requires a high Q-factor of the spectral response. We can achieve a high Q-factor of a single resonator as well as multiple coupled resonators [1]. Numerous theoretical models and simulation methods [2], have been developed to realize the linear and nonlinear characteristics of the coupled resonators and the resonators coupled with waveguides in PhC structures. However, basic understanding of physics insight these structures is still an important issue for researchers working in the PhC-based PICs. In these two commonly used resonator geometries, the number of resonators ( n) and the phase shift ( ϕ) play an important role in the spectral responses. While the number of resonator n defines the order of the resonant structures and number of resonant peaks/dips, the phase shift ϕ will decide the position, symmetric or asymmetric lineshape, and Q-factor of resonances. These geometries are designed in slotted 2D PhCs filled with nonlinear
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organic materials for applications in the efficient third-order nonlinear process, especially in optical switching/bistability. For the slotted conventional geometry and the transverse-electric polarization, the light is not only guided but its magnitude also enhanced inside the slot. To enhance the magnitude of electric field in the slot, the high Q-factor resonance of cavity in the slotted PhC waveguide and the slow light enhanced optical nonlinear in PhC coupled - resonator waveguide have been studied. On the other hand, the side -coupled resonators and waveguide, which exhibits electromagnetically induced transparency (EIT) has also been proposed. These structures bring about strong light-matter interactions, which enables enhancement of optical nonlinearity. In this work, the CMT in time combined with the FDTD simulation is employed to analyze and evaluate the Q- factors of resonances of CROWs and SCREW in the slotted 2D PhCs of holes filled with low index material. The influences of the number of resonators n and the phase shift ϕ on the Q-factor of spectral response are discussed. Our analysis reveals that from the perspective of optical switching/bistability, the CRO Ws and SCREW structures are more advantageous than the single resonator with an equivalent enhancing the Q-factor of resonance. For illustration, the slotted 2D PhC structure [3] under consideration is started with a 2D triangular lattice PhC structure of holes with lattice constant a. The holes are inscribed through the silicon film (e.g. SOI platform) with radius of r. The slotted waveguide is formed by removing the center row of holes and inscribing with the rectangular slot of width d. The slotted PhC w aveguide is obtained by first producing the slotted PhC waveguide and then filling it with low index material (e.g. DDMEBT) of linear refractive index of 1.8 and third-order nonlinear coefficient of 1.7x10 -17 m2/W as shown in Fig. 1. The FDTD simulations have been performed by assuming the geometry is invariant in the x-y plane with effective refractive index of 2.98 at λ = 1550 nm for transverse electric mode.
Figure 1: Slotted 2D PhC waveguides: (a) and (b) are the designs of the fifth-order filter based on CROWs and two side-coupled resonators and waveguide, respectively. The details of the one resonator are shown in (c).
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Figures 1(a-b) show the 2D PhC structures of coupled five identical slotted cavities together through the waveguide and two identical side-coupled slotted cavities and slotted waveguide, respectively. Each cavity is formed by gradually changing the slotted width from 50 nm at the center to 120 nm of both sides as shown in Fig. 1(c). The increasing step of slotted width of cavity is 10 nm for each periodicity, whereas the slotted waveguide widths at the input and output ports are kept at 50 nm. The design of the cavity with a slotted width gradually increases to reduce the abrupt change of the intensity inside the resonator. In the context of the presentation, a general of enhancing high-order resonant Q-factor with multiple coupled resonators will be treated by using CMT in time, and then confirmed by the FDTD simulation for slotted 2D PhCs filled with a low refractive index nonlinear material for application of switching/bistability. This result might provide a guideline for all-optical signal processing on a PhC chip design.
Acknowledgment This research is funded by Vietnam National Foundation for Science and Technology Development (NAFOSTED) under grant number “103.03-2017.02”.
References [1] Q. M. Ngo, S. Kim, J. Lee, H. Lim, Journal of Lightwave Technology 30 , 3525- 3531 (2012). [2] H. A. Haus, Waves and Fields in Optoelectronics (Englewood Cliffs, NJ: Prentice-Hall, 1984). [3] T. T. Hoang, Q. M. Ngo, D. L. Vu, Q. K. Le, T. K. Nguyen, P. T. H. Nguyen, Journal of Nanophotonics 12 (1), 016014 (2018).
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Suppression of photonic stopband reflection in metal-photonic structure
The Linh PHAM 1, Hong Luu DANG 1, Minh Nguyet NGUYEN 1, Dac Tuyen LE 2, *, Dinh Lam VU 1, * 1Institute of Materials Science, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet, Hanoi, Vietnam 2Department of Physics, Hanoi University of Mining and Geology, 18 Pho Vien, Hanoi, Vietnam *Email: [email protected] ; [email protected]
The rapid development in micro and nano manufacturing allows people to fabricate more and more artificial materials with outstanding features. Artificial structures of highly ordered periodic nano/micro have been demonstrated unique properties in ability to control electromagnetic wave [1-3]. They are a new class of optical materials and can be gained properties rooted from their structures rather than directly from chemical composition. Therefore, by adjusting the shape, size, orientation and arrangement of the structures, we can obtain desired features. Photonic crystals (PhCs) or metamaterials (MMs) have proven their applications and are nowadays a familiar concept. PhCs can be used to manipulate the flow of light by photonic band gap effect [1]. In 2000, the MM of negative refractive index was observed for first time by Smith and coworkers [2]. Numerous fascinating applications of MMs have been demonstrated such as superlens, invisible cloaking, and perfect absorption. For the interest of optical materials with nanostructures, self-assembled dielectric arrays have been used as backbone to distribute noble metal nanoparticles [4]. In this work, we use SiO 2 opal photonic crystal as a template to corrugate golden film with nanometer size periodicity. Optical characterizations are investigated via reflection measurement. Figure 1(a) shows the scanning electron microscopy (SEM) image of the annealed golden film. We can clearly observe golden nanocaps on the top of each sphere. Figure 1(b) presents the reflection spectra of a pure opal substrate and its golden cap structure. The reflection peak of the pure opal is result from effect of opal photonic stop band associated Bragg diffraction. However, the reflection peak of golden cap structure is inversed. It indicates the interesting properties of golden caps which can be absorbed electromagnetic wave. We have demonstrated a simple and inexpensive method to fabricate metal-photonic structure working on visible region. The golden caps lead to enhance absorption of the structure.
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Figure 1. (a) SEM image of golden cap structure. (b) Reflection spectra of pure opal and golden cap structure.
Acknowledgement This research is funded by Vietnam National Foundation for Science and Technology Development (NAFOSTED) under grant number 103.02-2017.67.
References [1] M. Fujita, S. Takahashi, Y. Tanaka, T. Asano, and S. Noda, Science 308 , 1296 (2005) [2] D. Smith, W. J. Padilla, D. Vier, S. C. Nemat-Nasser, and S. Schultz, Phys. Rev. Lett . 84 , 4184 (2000) [3] N. Segal, S. Keren-Zur, N. Hendler and T. Ellenbogen, Nature Photonics 17 , 1 (2015) [4] L. D. Tuyen, et al. Opt. Express 20 , 29266 (2012) ơ
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Mercury concentration in different parts of brain of big Sus srcofa from Małopolska region, Poland
V.V. THIEP 1,2,* , M. BŁASZCZYK 1, R. STAWARZ 1, J.Ł. BINKOWSKI 1 1 Institute of Biology, Pedagogical University of Cracow, Podchorazych 2, 30-084 Krakow, Poland 2 Faculty of Agriculture, Forestry and Fisheries, Quang Binh University, 312 Ly Thuong Kiet Str, Dong Hoi, Quang Binh, Vietnam *Email: [email protected]
The parts of pig's brain (forebrain, midbrain, hindbrain, and brainstem) were collected in 2016 in the slaughterhouses located in Małopolska region, Poland. Total mercury (Hg) content was determined by cold-vapor atomic absorption spectrometer. The study indicated the mean concentrations of Hg were rather low (0.0055 µg g -1 w.w.). Mean Hg concentration in the hindbrain, forebrain, brainstem, and midbrain were 0.0056, 0.0056, 0.0054 and 0.0054 µg g -1 w.w., respectively (Table 1). There was no a significant difference in Hg concentrations between 4 sections of pig's brain (p > 0.05). The Hg concentration in the brain is approximately equal to the number of muscles, but lower than in liver and kidneys, compared to literature data (Table 2). In all tested samples, the Hg level was below the permissible Hg limits for food in Europe follow European Commission [1-4].
Table 1. Hg concentration (µg g -1 w.w.) in parts of the brain of pigs (N=28) in Małopolska region, Poland Material Mean SE SD Minimum Maximum hindbrain 0.0056 0.0007 0.0037 0.0012 0.0139 forebrain 0.0056 0.0006 0.0033 0.0010 0.0126 midbrain 0.0054 0.0005 0.0028 0.0013 0.0114 brainstem 0.0054 0.0006 0.0031 0.0012 0.0141
Table 2. Published data on Hg concentrations (µg g -1w.w.) in pig liver, kidney and muscle. Liver Kidney Muscle Country Reference - - 0.012 Ghana Nkansah and Ansah (2014) [8] 0.001 0.002 0.001 Spain López-Alonso et al. (2007) [7] - - 0.001 Poland Paulina et al. (2012) [11] 0.005 0.008 0.003 Poland Falandysz J., Gajda B., (1988) [5] 0.004 0.012 0.001 Czech Republic Ulrich et al. (2001) [13] - - 0.003 Czech Republic Raszyk et al. (1996) [12] 0.015 0.019 0.009 Sweden Jorhem et al. (1991) [6] - - 0.003 Croatia Nina et al. (2010) [10] 0.012 0.014 0.011 Finland Niemi et al. (1991) [9] 36
References [1] Agency for Toxic Substances and Disease Registry (ATSDR), 1999. Public Health Statement Mercury . Atlanta, GA: U.S. Department of Health and Human Services, Public Health Service. [2] AMAP/UNEP, 2008. Technical background report to the global atmospheric mercury assessment. Arctic Monitoring and Assessment Programme/UNEP Chemicals Branch, pp 1-159. [3] European Communities, 2005. Community Strategy Concerning Mercury— communication from the Commission to the Council and the European Parliament. Commission on the European Communities. [4] European Commission, 2017. Maximum residue levels for mercury compounds, Directorate-General for Health and Food Safety (https://ec.europa.eu/info/law/better-regulation/initiatives/ares-2017- 3117108_en) [5] Falandysz J., Gajda B., 1988. Mercury content in muscle, liver and kidneys of slaughtered and game animals from the northern part of Poland, 1985-1986. Roczniki Panstwowego Zakladu Higieny . 39:113-117 [6] Jorhem L., Slorach S., Sundström B., Ohlin B., 1991. Lead, cadmium, arsenic and mercury in meat, liver and kidney of Swedish pigs and cattle in 1984-88. Food Additives and Contaminants., 8, 201-211 [7] López-Alonso M., Miranda M., Castilo C., Hernández J., García M., Benedito J., 2007. Toxic and esentail metals in liver, kidney and muscle of pigs at slauggter in Galicia (NW Spain). Food Additives and Contaminants , p 39. [8] Nkansah M. A., Ansah J. K., 2014. Determination of Cd, Mercury, As, Cr and Pb levels in meat from the Kumasi Central Abattoir. International Journal of Scientific and Research Volume 4, Issue 8. [9] Niemi A., Venalainen E. R., Hirvi T., Hirn J., Karppanen E., 1991. The lead, cadmium and mercury concentrations in muscle, liver and kidney from Finnish pigs and cattle during 1987-1988. Zeitschrift fur Lebensmittl Untersuchung und Forschung . 192:427-429 [10] Nina B., Maja Đ., Marija S., 2010. Survey of Arsenic, cadmium, copper, mercury and lead in kidney of cattle, horse, sheep and pigs from rural areas in Croatia. Food Additives and Contaminants : Part B Surveillance. 3: 3, 172 — 177 [11] Paulina D., Małgorzata P. , Mariusz R., 2012. Zawarto ść metali ci ęż kich w wybranych produktach spo żywczych Województwa Podkarpackiego. Bromatologia i Chemia Toksykologiczna .N 1, str. 94–100 [12] Raszyk J., Nezveda K., Docekalová H., Salava J., Palác J., 1996. The presence of harmful chemical elements (Mercury, Cd, Pb) in the stable environment for pig herds (in Czech). Veterinarni Medicina- Czech. 41, 207-211 [13] Ulrich R., Raszyk J., Nápracník A., 2001. Variations in contamination by mercury, cadmium and lead on swine farms in the district of Hodonín in 1994 to 1999. Veterinarni Medicina- Czech. 46, (5): 132–139
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Security dilemma of states in 21 st century on an example of Poland and Vietnam
Jarosław Indyk Institute of Political Science, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland Email: [email protected]
Nowadays, as far as international relations are concerned, many countries face the security dilemma. This specially concerns developing countries such Vietnam and until recently Poland. Both countries have to, to large extent, balance their economies, in order to maintain continuous development, but on the other hand, their governments have to provide safety of their citizen in case of any threats. Despite the fact that these states are located on different continents and the distance between them is large, we can observe certain similarities such as: turbulent history, occupation by external states, and geopolitical situation [1]. Both Poland and Vietnam border countries that have great political, military, and economical resources. Due to the above, it is worth to discuss the dilemma of security that these both countries face, considering investments in atomic power technology and ballistic missiles, which, in the military aspect, gain importance every year. Many countries, especially those developing, faces so called security dilemma, which defines the level up to which and how a country should reinforce. In the 21 st century, along with the development of technology, the model of army based on a large number of soldiers, tanks or a military power measured by the number of armoured carriers is being discontinued. On the other hand, more significant are attacks using computers, the Internet, as well as the development of the technology ballistic missiles [2]. It is very visible in case of India, which invests in the development of technologies able to transport nuclear weapon [3], or USA, which, despite a reduction of conventional warfare means and nuclear bombs, still does not decrease the number of missiles for their transport. A similar trend can be noticed in case of states such as Israel, Russia, China, or North Korea. What is more, the international law states not much about the proliferation of the technology of ballistic missiles [4], thus, gives countries such as North Korea [5] or Iran free hand to conduct studies on development of weapons of such type. Due to the above, it seems very essential to analyse and discuss whether countries such as Poland and Vietnam should not revise their approaches to the issue of security and commonly, or individually, think about the possibility of investing in the development of own technologies being able to scare off potential enemies or to cause significant losses behind the enemy lines.
References [1] S. C. Tucker, The Encyclopedia of the Vietnam War: A Political, Social, and Military History , ABC-CLICO Ltd, 41-46 (2000)
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[2] M. Czajkowski Obrona przeciwrakietowa w stosunkach mi ędzynarodowych , Wydawnictwo Uniwersytetu Jagiello ńskiego (2013) [3] J. Berlinger, N. Kumar, India tests-fires Agni-V, a nuclear-capable ICBM , cnn.com (January 19, 2018) [https://edition.cnn.com/2018/01/18/asia/india-icbm- tests/index.html] [4] Columbia Peoples, Justifying Ballistic Missile Defence: Technology, Security and Culture , Cambridge University Press,215-248 (2010) [5] M. Dodge, Keeping Up With North Korea’s And Iran’s Bad Ballistic Missiles , Investors.com (November 11, 2017) [https://www.investors.com/politics/commentary/keeping-up-with-bad-ballistic- missiles/] [6] A. Antoszewski, R. Herbut, Systemy polityczne współczesnego świata , Arche, 166-182 (2001) [7] I. E. Rinehart, S. A. Hildreth, S. V. Lawrence, Ballistic Missile Defense in the Asia--Pacific Region: Cooperation and Opposition , Congressional Research Service, 3-25 (April 3, 2015) [8] K. Atherton, Is North Korea investing in a fundamentally useless weapon? , Defence News (December 29, 2017) [https://www.defensenews.com/global/asia-pacific/2017/12/29/is-north-korea- investing-in-a-fundamentally-useless-weapon/]
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40
Session 2
O-07 Tran Van PHUC Optical properties and chemical composition of transition layers formed in the process of irradiation by Ne +, Ar +, Kr + and Xe + ions of the multilayer TiO 2/SiO 2 system
O-08 Sylwia SOWA Superconductivity and structure of U-based alloys with selected (3-5)d-metals and of their hydrides
O-09 DINH Tien Hung Study of designing the scintillation detector using CsI(Tl) crystals and PIN photodiode for ambient gamma dose rate
O-10 HOANG Huu Thang Synthesis and Characterization of NaLi0.2Mn0.8O2 Oxide as a Cathode Material for Sodium-ion Batteries
O-11 Le Thi Thu PHUONG Levels of microelements (Cu, Zn, Fe) and macroelements (Mg, Ca) in organs of Mullet (Mugil cephalus Linnaeus, 1758) in coastal Vietnam
O-12 Maria KOTKIEWICZ Social activity of NGO members as exemplified by scouts
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42
Optical properties and chemical composition of transition layers formed in the process of irradiation by Ne +, Ar +, Kr + and Xe + ions of the multilayer TiO 2/SiO 2 system
M. Kulik 1,2 , D.E. Kołody ńska 3, H.M. Przewłocki 4, T.V. Phuc 1,5,* , Afag I. Madadzada1,6 , A.P. Kobzev 1, Z. Hubicki 3, J. Żuk 2 and K. Pyszniak 2 1Joint Institute for Nuclear Research, Dubna, Moscow reg. 141980, Russia 2Institute of Physics, Maria Curie-Skłodowska University, 20-031, Lublin Poland 3 Faculty of Chemistry, Maria Curie-Skłodowska University, 20-031, Lublin Poland 4 Institute of Electron Technology, 02-668,Warszawa Poland 5 Institute of Physics, Vietnamese Academy of Science and Technology, 10 Dao Tan, Ba Dinh, Hanoi, VietNam 6 National Nuclear Research Center JSC, 370143, Baku, Azerbaijan *Email: [email protected]
+ + + Four groups of TiO 2/SiO 2/TiO 2/Si samples were irradiated by Ne , Ar , Kr and Xe + ions with the same fluence of 3x10 16 cm -2. Each of these groups was divided into four subgroups containing samples implanted with the same kind of ions with incident energies of 100 keV, 150 keV, 200 keV and 250 keV. The implantation process was carried out at room temperature. Spectra of dielectric functions and depth distribution chemical compositions were taken by spectroscopic ellipsometry (SE) and X-ray photoelectron spectroscopy (XPS), both before and after the irradiation. The results of this research indicate the presence of transition layers between homogeneous TiO 2 and SiO 2 layers. It has been noticed that the thickness and chemical composition of these layers changes with the increasing energy and mass of implanted ions. The spectra of refraction and extinction coefficients of all the studied layers were calculated in the 250 nm to 1000 nm wavelength range. It was found that the spectra of refraction and extinction coefficients of the transition layers are efficiently found using the effective medium approximation (EMA). Using the ionic stripping of the TiO 2 surface layer and taking XPS spectra of Ti2 p and Ti3 p bounds it was found that concentration of Ti and TiO, TiO 2 and Ti 2O3 compounds changes with the increasing distance from the irradiated surface. Computer simulations conducted using the SRIM code have shown that these concentration changes of elements and chemical compounds can be attributed to the formation of vacancies and to the displacement of atoms in the investigated layers.
43
Superconductivity and structure of U-based alloys with selected (3-5) d-metals and of their hydrides
Sylwia SOWA 1,* , N.-T.H. KIM-NGAN 1, Magdalena KRUPSKA-KLIMCZAK 1, Mykhaylo PAUKOV 2, Volodymyr BUTURLIM 2, Ladislav HAVELA 2 1Nanostructure Laboratory, Institute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland 2Department of Condensed Matter Physics, Faculty of Mathematics and Physics, Charles University, Ke Karlovu 5, 12116 Prague, Czech Republic *Email: [email protected]
Uranium metal exists in three allotropic phases: α, β and γ. Using ultrafast- cooling (splat-cooling) with the cooling rate of 106 K/s helps to minimalize the T alloying concentration (T=Mo, Zr, Nb, Pt, Pd, Ti, Ru) necessary to retain the γ-U phase in U-T alloys down to low temperatures. The hydrogen absorption in U-T alloys at high hydrogen pressures leads to a formation of the hydrides implying a disappearance of the superconductivity and a formation of U magnetic moment [1]. The temperature dependences of electrical resistivity of selected splat-cooled U-T alloys are summarized in Fig. 1. U-T splats become superconductivity at low temperatures revealed by resistivity drops to zero. The sharpest drop and the highest Tc = 2.11 K was obtained for U-15at.% Mo, which is a conventional BCS superconductor. Additional information about the superconducting phase transition was provided by the temperature dependence of the specific heat, measured for some of splats down to 0.3 K (Fig. 2). For U-15at.% Mo and U-15at.% Ru splats a pronounced λ- type of anomaly was observed [2]. All the splats can absorb hydrogen when exposed to a high H 2 pressure forming hydrides of approximate stoichiometry (UH 3)1-xTx. A much larger volume expansion can be achieved by hydrogen absorption, yielding two structure variants of UH 3, namely α-UH 3 and β-UH 3, which become strong ferromagnets with TC ≈ 165 K [3].
Figure 1. Superconducting phase transition in U-T splats indicated by abrupt drops of the electrical resistivity to zero. All curves are normalized to the resistivity value at T = 4 K [2].
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Figure 2. Specific heat anomalies related to the superconducting phase transition for selected U-T splats. The vertical bars indicate theoretical BCS values.
In the present study we compare the structure and electronic properties of splat- cooled U-T alloys and their hydrides [2]. Analysis of XRD data for the hydrides with Nb and Ti reveals a mixture of α- and β-UH 3 hydrides for the 15% alloying level (Fig. 3). The hydride with composition (UH 3)0.85 Ru 0.15 exhibits a pattern similar to (UH 3)0.85 Mo 0.15 , although the average grains size is not as small as in the Mo alloying case. The peak broadening does not allow precise determination of lattice parameters, which, however, remain close to those of α- and β-UH 3 hydrides. The alloying increases the Curie temperature of UH 3 reaching over 190 K for UH 3 with 15% Ti. TC starts to decrease for the higher alloying levels.
Figure 3. Comparison of XRD patterns of selected hydrides with simulated patterns of α- and β- UH 3.
Acknowledgements This work was supported by the Czech Science Foundation under the Grant 15- 01100S and the Visegrad/V4EaP Scholarship-51600543. Experiments were partly performed at MLTL ( http://mltl.eu/ ), which is supported within the program of Czech Research Infrastructures (project No. LM2011025). References: [1] S. Sowa et al., Acta Phys. Pol. A , 130 , 521-526 (2016). [2] S. Sowa et.al., Physica B , Physica B , 536 , 546-552 (2018). [3] I. Tkach et al ., J. Alloys Comp ., 534 , 101-109 (2012). 45
Study of designing the scintillation detector using CsI(Tl) crystals and PIN photodiode for ambient gamma dose rate
D. T. Hung 1* , P. D. Khang 2 1Military Institute of Chemical and Environmental Engineering (MICEE), DCT08, Phu Vinh, An Khanh, Hoai Đuc, Hanoi, Vietnam 2Hanoi University of Science and Technology, 1 Dai Co Viet, Hanoi, Vietnam *Email: [email protected]
In Vietnamese weather conditions, it is difficult to use NaI(Tl) scintillation detector which combined PMTs for out-door real-time gamma spectrum monitoring purpose. Using this system, the gamma spectrum will be continuously shifted, because the light output and the photo-emission (in proportion to scintillator and PMTs) will be significantly changed by the environmental temperature. Therefore, designing others scintillation detector including CsI(Tl) crystals and PIN photodiode is ideal to replace NaI(Tl) and PMTs - the light output and electron emission in electronic components are constant when the environmental temperature changed. This paper shows some results with new detector (includes CsI(Tl) and PIN photodiode) for use in the measure of that type.
Acknowledgment This work was supported by the MICEE Research Project in KC.AT Program, No. 634/2017/HDKHCN.
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Synthesis and Characterization of NaLi 0.2 Mn 0.8 O2 Oxide as a Cathode Material for Sodium-ion Batteries
Huu Thang HOANG 1,2 , Nang Long PHUONG 1,2 , Van Nghia NGUYEN 3,* , Vu Chung HOANG 1 1Institute of Materials Science, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet Street, Hanoi, Vietnam 2 University of Engineering and Technology, 144 Xuan Thuy Street, Hanoi, Vietnam 3Hanoi Architectural University, Km10 Nguyen Trai Street, Thanh Xuan, Hanoi, Vietnam *Email: [email protected]
Recently, lithium ion batteries are commonly used in mobile electronic devices, electric vehicles, and energy storage systems. However, due to the limited resources and high production cost of lithium compounds, finding the new abundant and environmental friendly materials is desirable. Sodium ion batteries are attractive candidates for the energy storage on a large scale because of the sodium-rich resources and competitive production cost. Recently, the P2-layered structure compounds have been proposed and used as the cathode materials for the sodium-ion batteries. In this study, the NaLi 0.2 Mn 0.8 O2 oxide was successfully synthesized by a conventional solid state reaction method. The XRD analysis revealed that the NaLi 0.2 Mn 0.8 O2 material has the P2- layered structure, belonging to the space group P6 3/mmc , lattice parameters are a = 2.85995 Å, c = 11.06368 Å, and cell volume = 78.3697 Å 3. Coating carbon onto the NaLi 0.2 Mn 0.8 O2 material using different carbon compounds is reported as well. (1 blan
47
Levels of microelements (Cu, Zn, Fe) and macroelements (Mg, Ca) in organs of Mullet ( Mugil cephalus Linnaeus, 1758) in coastal Vietnam
L.T.T. PHUONG 1,* , V.V. THIEP 1,2 , N.T.Q. PHUONG 1, H.A. VU 1, L.K. VU 1, N.T.T. VAN 1 1 Faculty of Agriculture, Forestry and Fisheries, Quang Binh University, 312 Ly Thuong Kiet Str, Dong Hoi, Quang Binh, Vietnam 2 Institute of Biology, Pedagogical University of Cracow, Podchorazych 2, 30-084 Krakow, Poland *Email: [email protected]
Fish is not only a source of valuable proteins and specific n-3 and n-6 polyenoic fatty acids, but it also provides necessary mineral macroelements (calcium, magnesium) and microelements (copper, zinc, iron) [1-4]. Thus, in this study, the concentrations of calcium (Ca), magnesium (Mg), copper (Cu), zinc (Zn), and iron (Fe) in organs (muscle, gill, and liver) of Mullet ( Mugil cephalus Linnaeus, 1758) were investigated. Samples were collected in coastal Vietnam from July to October 2017. Total heavy metals concentration determined by the flame atomic absorption spectrometer [5-7]. The result showed that there was the significant difference in concentration of calcium, magnesium, copper, zinc, and iron in muscle, gill, and liver (p<0,05). Mean Cu concentration in muscle < gill < liver (0.041, 0.055 and 0.080 µg g - 1 d.w., respectively). Mean Fe concentration in muscle < liver < gill (2.225, 2.247 and 5.394 µg g -1 d.w., respectively). Mean Zn concentration in liver < gill < muscle (0.486, 0.664 and 1.093 µg g -1 d.w., respectively). Mean Mg concentration in liver < gill < muscle (0.082, 0.206 and 0.373 µg g -1 d.w., respectively). Mean Ca concentration in liver < gill < muscle (0.036, 1.651 and 2.096 µg g -1 d.w., respectively) (Table 1).
Table 1. Heavy metals concentration (µg g -1 d.w.) in organs of the Mullet (N=54) in coastal Vietnam Cu Fe Zn Mg Ca Mean ± 0.055 ± 5.394 ± 0.664 ± 0.206 ± 1.651 ± SD 0.034 2.891 0.249 0.084 0.669 Gill Min 0.018 1.383 0.169 0.069 0.547 Max 0.181 12.296 1.268 0.389 3.719 Mean ± 0.080 ± 2.247 ± 0.486 ± 0.082 ± 0.036 ± SD 0.033 1.327 0.172 0.018 0.052 Liver Min 0.025 0.485 0.220 0.047 -0.051 Max 0.140 5.817 0.900 0.111 0.189 Mean ± 0.041 ± 2.225 ± 1.093 ± 0.373 ± 2.069 ± SD 0.033 1.579 0.532 0.164 1.205 Muscle Min -0.022 0.186 0.297 0.065 0.017 Max 0.113 4.958 2.266 0.660 4.488
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The study results also showed that the bioaccumulation of these heavy metals also depends on fish weight and body length and age. The estimated levels of all metals in the present study were lower than the limits permitted by Food and Agriculture Organization of the United Nations/World Health Organization (FAO/WHO).
References [1] Ewa Brucka-Jastrz ębska, Dorota Kawaczuga, Monika Rajkowska, Mikołaj Protasowicki, 2009. Levels of microelements (Cu, Zn, Fe) and macroelements (Mg, Ca) in freshwater fish. J. Elementol. 14(3): 437-447 [2] Joanna Łuczy ńska, Kazimierz Markiewicz, Jan Jaworski, 2006. Interspecific differences in the contents of macro- and microelements in the muscle of six fish species from of the Olsztyn Lake district (North-east of Poland). Pol. J. Food Nutr. Sci. 15(1): 29-35 [3] Joanna Łuczy ńska, El żbieta To ńska, Marek J. Łuczy ński, 2009. Essential mineral components in the muscles of six freshwater fish from the Mazurian Great Lakes (northeastern Poland). Arch. Pol. Fish. 17: 171-178 [4] Kamal J. Elnabris, Shareef K. Muzyed, Nizam M. El-Ashgar, 2013. Heavy metal concentrations in some commercially important fishes and their contribution to heavy metals exposure in Palestinian people of Gaza Strip (Palestine). Journal of the Association of Arab Universities for Basic and Applied Sciences . (13) 44–51 [5] Mazlin Bin Mokhtar, Ahmad Zaharin Aris, Vikneswaran Munusamy, Sarva Mangala Praveena, 2009. Assessment level of heavy metals in Penaues Monodon and Oreochromis Spp in selected aquanculture ponds of high densities development area. European Journal of Scientific Research . 30(3): 348-360 [6] O. Mogobe, K. Mosepele and W. R. L. Masamba, 2015. Essential mineral content of common fish species in Chanoga, Okavango Delta, Botswana. African J. of Food Science . 9(9): 480-486 [7] S. Squadrone, M. Prearo, P Brizio, S. Gavinelli., M. Pellegrino, T Scanzio, S. Guarise, A. Benedetto, M. C. Abete, 2012. Heavy metals distribution in muscle, liver, kidney and gill of European catfish (Silurus glanis) from Italian Rivers. J. Chemosphere . (90) 358–365
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Social activity of NGO members as exemplified by scouts
Maria KOTKIEWICZ , Faculty of Political Science, Institute of Political Science, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland Email: [email protected]
Recent years have seen a rapid development of non-governmental organisations (NGOs) in Poland, as they have played a crucial role in raising citizen awareness in both rural and urban areas. An example of an NGO is the Polish Scouting and Guiding Association (ZHP), which is the largest youth care organisation in Poland. This work presents the results of a survey concerning social activity of scouts, conducted online among a number of child, junior, and adult members of the Polish Scouting and Guiding Association. The aim of the study is to determine whether the membership in the scout movement, with all the knowledge and skills gained by the members, raises their citizen awareness and encourages their social activity outside the structure of the Association, and, if so, in what ways and to what extent.
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Session 3
O-13 Magdalena KRUPSKA-KLIMCZAK + + + Intermixing in Fe 3O4 films induced by 1MeV Ar , Kr and Au ion irradiation
O-14 PHAM Hoai Linh Study on fabrication of magnetic fluids based on spinel ferrite Fe 3O4 nanoparticles for applying in magnetic fluid hyperthermia cancer treatment
O-15 Tomasz MRÓZ Reactor neutron activation analysis in studies of C3-CAM transition of Mesembryantheum crystallinum L
O-16 Artur JACH-CHRZASZCZ The Treaty of Trianon: the politics of memory in contemporary Hungary
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52
Intermixing in Fe 3O4 films induced by 1MeV Ar +, Kr + and Au + ion irradiation
Magdalena KRUPSKA-KLIMCZAK 1,* , N.-T.H. KIM-NGAN 1, Sylwia SOWA 1, Adam G. BALOGH 2, Petr MALINSKY 3, Anna MACKOVA 3,4 1Nanostructure Laboratory, Institute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland 2Department of Mathematics and Natural Sciences, Darmstadt University of Applied Science, 64295 Darmstadt, Germany 3Nuclear Physics Institute, Academy of Sciences of the Czech Republic, v.v.i., 25 068 Rez, Czech Republic 4Department of Physics, Faculty of Science, J.E. Purkinje University, Ceske Mladeze 8, 400 96 Usti nad Labem, Czech Republic *Email: [email protected]
We used 1-2 MeV rare-gas (He, Ar, Kr) and metal (Au) ion beams to study and modify the surface and interfaces of thin films of materials with a high potential for applications. In this work we present our results obtained for magnetite (Fe 3O4) films. Fe 3O4 is one of the most known magnetic materials. It is considered recently as a promising candidate for applications as spintronic devices at room temperature. Fe 3O4 films were grown on MgO(001) substrate by molecular Beam Epitaxy (MBE) with single- and bi-layer structure (Fe 3O4/MgO(001) and Fe 3O4/Fe/MgO(001), respectively). To study the ion beam mixing effect and its influence on the film properties, crystallinity and stability, we performed ion irradiation experiments using 1MeV Ar +, Kr + [1] and Au + ions on these films. The chemical composition, layer thickness and film crystallinity of the films were investigated by using Rutherford Backscattering spectrometry (RBS), RBS-channeling experiments (RBS-C) and X-ray reflectometry. We show that Ar +, Kr + and Au + irradiation induced large interfacial zones due to a strong ion mixing. The most important finding is that the stoichiometric Fe 3O4 layer on the film surface of the bi-layered films (Fe 3O4/Fe/MgO(001)) could be well preserved upon Ar + and Kr + ion irradiation, despite of a large decrease of the layer thickness. The Au + ion irradiation revealed that Au + ions penetrates deeply into the MgO substrate. Acknowledgment The magnetite thin films were prepared within the scope of cooperation with prof. J. Korecki (AGH Kraków). We highly acknowledges the great help of RBS group in the Institute of Nuclear Physics of the University Frankfurt/Main during performing RBS and RBS-C experiments and Ar + and Kr + ion irradiation experiments. Additional RBS measurements and Au + ion irradiation experiments were carried out at the CANAM infrastructure of the NPICAS Rez supported through MEYS project No. LM2015056 and by the GACR project P108/12/G108. References [1] N-T. H. Kim-Ngan, M. Krupska, A. G. Balogh, P. Malinsky, A. Mackova, Adv. Nat. Sci.: Nanosci. Nanotechnol. 8 (2017) 045005
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Study on fabrication of magnetic fluids based on spinel ferrite Fe 3O4 nanoparticles for applying in magnetic fluid hyperthermia cancer treatment
Pham Hoai Linh 1,* , Pham Hong Nam 1, Ta Ngoc Bach 1,Vu Dinh Lam 1, Le Van Hong 1, Nguyen Xuan Phuc 1, Pham Thanh Phong 2 1Institute of Materials Science, Vietnam Acadermy of Science and Technology, 18 Hoang Quoc Viet road, Cau Giay ward, Hanoi, Vietnam 2Theoretical Physics Research Group, Advanced Institute of Materials Science, Ton Duc Thang University, Ho Chi Minh City, Viet Nam *Email: [email protected]
In recent years, magnetic fluid hyperthermia (MFH) therapy has been considered as a promising therapy for cancer treatment because it offers fewer unwanted effects than conventional therapies such as chemotherapy, surgery, and radiotherapy [1]. In the MFH therapy, magnetic nanoparticles (MNPs) in stable colloidal suspensions are injected locally into cancer tissues. Under the help of an external alternating magnetic field (AMF), the MNPs are able to generate heat (corresponding to the temperature in range of 42 oC-46 oC) only in the tissues containing MNPs to reduces cancer cell viability and destroy them without harm to surrounding healthy tissue [2]. Althought the MFH therapy has many advantages, but clinical applications of MFH therapy are still great challenge such as quantifying the maximum allowable magnetic field condition, engineering MNPs to achive subtantial accumulation in cancer tumor after systermic delivery... [3]. In real in- vivo application, MNPs are likely to aggregate and form clusters after they have been injected into blood vessels or cancer tumors. A better understanding of magnetic heating behavior of magnetic nanoclusters allows us obtain the reliable heating responses as the case of nanoparticles located in biological subjects. Interestingly, recent studies have also indicated that MNP clusters have a much higher saturation magnetization than individual MNPs [4]. This feature may open an alternative way to enhance heating efficiency [5]. In addition, the core MNPs coated with dextran or OCMCS were well-dispersed in the solution in the form of colloidal cluster [6]. Thus, a well-understanding the influence of the colloidal cluster interactions on the heating capacity is important factor to design the advanced cluster structures [7]. In this work, we studied and successfully fabricated magnetic fluids based on Fe 3O4 nanoparticles coated with dextran or O-carboxymethy chitosan [8-9]. The coated particles are well dispersed in aqueous solution in form of clusters with an average size of about 148 nm for magnetic fluids based on Fe 3O4 NPs coated dextran and from 52 nm to 179 nm for the coated with OCMCS. Magnetic fluids exhibit high SAR and ILP ( intrinsic loss power, used to compare the induction heating of magnetic fluid at various magnetic fields) values, at low field strength and low Fe 3O4 concentration. The highest SLP and ILP were obtained for dextran coated Fe 3O4 concentration of 1mg/mL were 167 W/g and 14.8 nHm 2/kg. The magnetic fluid based on Fe 3O4 NPs coated OCMCS yield a high SAR of 204 W/g and ILP of 17.15 54
nHm 2/kg for sample with the smaless hydrodynamic size. In particular, the role of magnetic interaction between magnetic clusters on heat dissipation of magnetic fluid under alternating field was addressed. Our results imply that magnetic interactions between magnetic clusters directly and strongly influence the magnetic response of the nanoparticles to external field of mT range and, therefore, lead to large SLP and ILP in magnetic fluids.
Fig 1. TEM images of Fe 3O4 NPs (a), their corresponding size distribution histograms (b), OCMCS-coated Fe 3O4 NPs with different amounts of OCMCS during synthesis: S0.1 (c, f), S0.3 (d, g), S0.6 (e, h).
Fig. 2. Heating curves of OCMCS-coated Fe 3O4 NP samples at different magnetic concentrations and SAR as a function of magnetic concentration.
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References [1] Challa.S.S.R.Kumar, F.Mohammad ((2011)) Magnetic nano materials for hyperthermia-based therapy and controlled drug delivery . AdvDrug Deliv Rev 63:789–808 [2] Dutz S, Hergt R (2013) Magnetic nanoparticle heating and heat transfer on a microscale: basic principles, realities and physical limitations of hyperthermia for tumour therapy . Int J Hyperthermia 29:790–800 [3] Sophie Laurent, Silvio Dutz, Urs O. Häfeli, Morteza Mahmoudi (2011) Magneticfluid hyperthermia: Focus on superparamagnetic iron oxide nanoparticles . Advances in Colloid and Interface Science 166:8–23 [4] Lartigue L, Hugounenq P, Alloyeau D, Clarke SP, Levy M, Bacri JC, Ménager C (2012) Cooperative organization in iron oxide multi-core nanoparticles potentiates their efficiency as heating mediators and MRI contrast agents . ACS Nano 6:10935e10949 [5] Serantes D, Simeonidis K, Angelakeris M, Chubykalo-Fesenko O, Marciello M, Morales MdP, Baldomir D, Martinez-Boubeta C (2014) Multiplying Magnetic Hyperthermia Response by Nanoparticle Assembling . J Phys Chem C 118:5927−5934 [6] Anastasia K. Hauser, Ronita Mathias, Kimberly W. Anderson, Hilt JZ (2015) The effects of synthesis method on the physical and chemical properties of dextran coated iron oxide nanoparticles . Materials Chemistry and Physics 160:177–186 [7] Ihab M. Obaidat, Bashar Issa, Yousef Haik (2015) Magnetic Properties of Magnetic Nanoparticles for Efficient Hyperthermia . Nanomaterials 5(1):63-89. [8] P.H. Linh, N. V. Chien, D. D. Dung, P. H. Nam, D. T. Hoa, N. T. N. Anh, L. V. Hong, N. X. Phuc, and P. T. Phong, Biocompatible nanoclusters of O- carboxymethyl chitosan-coated Fe 3O4 nanoparticles: synthesis, characterization and magnetic heating efficiency , Journal of Materials Science, (2018)53.8887- 8900. https://doi.org/10.1007/s10853-018-2180-0 (fisrt online 05/03/2018). [9] P. H. Linh, N. X. Phuc, L. V. Hong, L. L. Uyen, N. V. Chien, P. H. Nam, N. T. Quy, H. T. M. Nhung, P. T. Phong, In-Ja Lee, Dextran coated magnetite high susceptibility nanoparticles for hyperthermia applications , Accepted for publication in Journal of Magnetism and Magnetic Materials 460 (2018) 128– 136.
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Reactor neutron activation analysis in studies of C 3-CAM transition of Mesembryantheum crystallinum L.
Tomasz MRÓZ 1,2,* , Andrzej KORNA Ś1 1Pedagogical University of Cracow, Institute of Biology, Kraków 30084, Poland 2Jagiellonian University in Cracow, Institute of Physics, Kraków, Poland *Email: [email protected]
Instrumental neutron activation (INAA) analysis is non-destructive technique of determination elemental composition in investigated samples. INAA is based on inducing artificial radioactivity by irradiating sample with high flux of neutrons and measurements of gamma-rays being emitted by decaying nuclei. In our study we have used INAA for determination of elemental composition changes in Mesembryantheum crystallinum L. samples collected during experimentally induced C 3-to-CAM (Crassulacean Acid Metabolism) transition. Our studies showed, that INAA is powerful tool to use in biological studies, which provides information about concentration of almost 50 elements in one analyzed sample, with detection limits comparable with mass spectroscopy (such as ICP-MS).
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The Treaty of Trianon: the politics of memory in contemporary Hungary
Artur JACH-CHRZASZCZ Faculty of Political Science, Institute of Political Science Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland Email: [email protected]
Historically, Vietnam and Hungary are not strongly connected with each other. Looking from the prism of modern times – they are, because the relationships in the field of international relations like trade and scientific exchange and others are established between these countries. However, such relations in the XIX and XX century did not occur, but the history of the formation of independent states was similar both in Vietnam and Hungary. In the aforementioned period, both countries changed their borders. Moreover, they were influenced by other powers. This state prevented the development and functioning of both countries for a long time. The years from 1843 to 1940 are the period of protectorate for Vietnam, and in fact – a French colony. In a similar period, the fate of Hungary hanged in the air. Although in the case of this country, the period of domination of foreign powers in Hungary really began with the defeat in the Battle of Mohács in 1526, the consequence of this event was the division of Hungarian lands into three parts in 1541. Therefore, Hungary became a Turkish province. At the end of the XVII century, the country passed from the hands of the Ottoman Empire to the rule of the Habsburgs. This did not contribute to the independence of Hungary in any way. The year 1848 is the time of the Hungarian uprising, which indirectly allows Hungary to unite with Austria and create the dualistic monarchy of Austria and Hungary. This time until the outbreak of the First World War is the period (still despite the lack of full independence) of prosperity in Hungary. However, the price for this monarchy will cause a national trauma among Hungarians that continues to this day. On June 4, 1920, the Treaty of Trianon was signed at the Grand Trianon Palace. It resulted in the loss of 2/3 of the existing lands and population living in pre-treaty Hungary. The numerous numbers of ethnic Hungarians inhabiting the territories incorporated into the newly created countries directed the Hungarian policy to efforts aimed at the recovery of the lost lands. Thus, the interwar policy of Miklós Horthy was based on the recovery of the lost lands. These territories were promised to Hungary by Adolf Hitler in exchange for a military alliance. Despite the recovered parts of the lands (under the provisions of the Vienna arbitrage) after losing the Second World War on February 10, 1947, Hungary (by signing the peace treaty with the Allies) returned to the borders determined by the Treaty of Trianon. The objective of the presentation is to present to the listeners the political events and the history of Hungary, as well as the geopolitical situation occurring in these years in Europe. The author, due to the conducted researches and the subject matter related to his doctoral thesis, will pay special attention to the decisions and
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consequences connected with the Treaty of Trianon. Moreover, he will present Hungary’s current aspirations to commemorate events affecting the present shape of the Hungarian state.
References [1] E. Paul, Slovak Views of the Hungarian Minority , 31 , 485-493 (2003) [2] E. Raffay, Magyar tragédia: Trianon 75 éve , Püski Kiadó, 193-199 (2006) [3] G. Jeszenszky, The Afterlife of the Treaty of Trianon , 184 , 101-111 (2006) [4] M. Zeidler, Trianon , Osiris Kiadó, 674-676 (2003) [5] O. Jászi, Kossuth and the Treaty of Trianon , Foreign Affairs, 12 , 86-97 (1933) [6] S. Vardy, The Impact of Trianon upon Hungary , 10 , 21-42 (1983)
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Session 4
O-17 NGUYEN Ngoc Anh Experimental study on nuclear level scheme, nuclear level density, and radiative strength function using the gamma–gamma coincidence spectrometer in Vietnam
O-18 Maria PODGÓRNA Raman scattering investigations of phase transitions in the nanocrystals of PbZrO 3-BiFeO 3 system
O-19 NGUYEN Minh Nguyet Impact of external factors on electromagnetic properties of metamaterial absorbers in THz region
O-20 NGUYEN Thi Thu Ha Synthesis the series of compounds Sr 2MO 3FeAs (M = V, Cr)
O-21 VU Hoang Anh Assessment of impacts to biodiversity forest in Dong Chau forest - Nuoc Trong stream, Kim Thuy commune, Le Thuy district, Quang Binh province
O-22 Anna MICHNIEWSKA Khan Academy - a platform supporting the teaching and learning process in Poland
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Experimental study on nuclear level scheme, nuclear level density, and radiative strength function using the gamma – gamma coincidence spectrometer in Vietnam
Ngoc Anh NGUYEN 1,* , Xuan Hai NGUYEN 1, Dinh Khang PHAM 2, Huu Thang HO 1, Van Minh TRUONG 3 1Dalat Nuclear Research Institute, 01 Nguyen Tu Luc, Dalat, Vietnam 2Hanoi University of Science and Technology, 1 Dai Co Viet, Hanoi, Vietnam 3Dong Nai University, Bien Hoa, Vietnam *Email: [email protected]
Experimental nuclear level scheme (NLS), nuclear level density (NLD), and radiative strength function (RSF) are all together important quantities, which are necessary for nuclear reaction, nuclear structure, and astronomical studies. It has been well-known that the gamma–gamma coincidence method [1] can be used to study the NLS, NLD, and RSF in the energy range from 0.5 MeV to B n-0.5 MeV (B n is the neutron binding energy). Within this method, the cascade decays, which are obtained fr om the decay of the initial compound state to the different final states, are measured. Based on the experimental cascade decays, the NLS and the gamma cascade intensity distribution are constructed. Since the gamma cascade intensity distribution is relate d to both the NLD and RSF, these quantities can be extracted from the gamma cascade intensity distribution [2-5]. This talk presents our recent studies on NLS, NLD, and RSF via (n, γ) reaction using the gamma – gamma coincidence spectrometer at Dalat Nucle ar Research Institute, Vietnam. The experimental setup is given in Fig. 1. Our achievement with NLS of 172 Yb [6], as well as some unpublished and recent results obtained for 153 Sm and 183,187 W, will be discussed.
Figure 1. The experimental setup of the gamma –gamma coincidence spectrometer at Dalat Nuclear Research Institute 63
Acknowledgment We would like to thank the Ministry of Science and Technology of Vietnam for the financial support through the projects coded KC05. We would like also to thank the operation team of Dalat Nuclear Research Reactor for their kind support during our experiments. The corresponding author wants to thank Dr. A.M. Sukhovoj at the Joint Institute of Nuclear Physics, Dubna, Russia for his generous and thoughtful guidance on the gamma–gamma coincidence method.
References [1] S.T. Boneva, E. V Vasil’eva, Y.P. Popov, A.M. Sukhovoi, V.A. Khitrov, Two- quantum cascades of radiative neutron capture 1. Spectroscopy of excited states of complex nuclei in the neutron binding energy region , Fiz. Elme. Chastits At. Yadra. 22 (1991) 479. [2] S.T. Boneva, V.A. Khitrov, A.M. Sukhovoj, A.V. Vojnov, Excitation study of high-lying states of differently shaped heavy nuclei by the method of two-step cascades , Nucl. Phys. A. 589 (1995) 293–306. [3] E. V. Vasilieva, A.M. Sukhovoj, V.A. Khitrov, Direct experimental estimate of parameters that determine the cascade gamma decay of compound states of heavy nuclei , Phys. At. Nucl. 64 (2001) 153–168. [4] A.M. Sukhovoj, New model of the cascade gamma decay of neutron resonances for practitioners: Basic concepts and attainable precision , Phys. At. Nucl. 78 (2015) 230–245. [5] F. Be čvá ř, P. Cejnar, J. Honzátko, K. Kone čný, I. Tomandl, R.E. Chrien, E 1 and M 1 strengths studied from two-step γ cascades following capture of thermal neutrons in Dy 162 , Phys. Rev. C. 52 (1995) 1278–1294. [6] N.A. Nguyen, X.H. Nguyen, D.K. Pham, Q.H. Nguyen, H.T. Ho, Updated level scheme of 172 Yb from 171 Yb(nth, γ) reaction studied via gamma–gamma coincidence spectrometer , Nucl. Phys. A. 964 (2017) 55–68.
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Raman scattering investigations of phase transitions in the nanocrystals of PbZrO 3-BiFeO 3 system
Maria PODGÓRNA 1,* , Maciej PTAK 2, Maciej CHRUNIK 3, Irena JANKOWSKA-SUMARA 1, Julita PIECHA 4, Dariusz ZASADA 5 1Institute of Physics, Pedagogical University of Cracow, Podchor ąż ych 2, 30-084 Kraków, Poland 2Institute of Low Temperature and Structure Research, Polish Academy of Sciences, Okólna 2, 50-950 Wrocław 2, Poland 3Institute of Applied Physics, Military University of Technology, Urbanowicza 2, 00-908 Warsaw, Poland 4Institute of Physics, University of Silesia, Uniwersytecka 4, 40-007 Katowice, Poland 5Department of Advanced Materials and Technologies, Military University of Technology, Urbanowicza 2, 00-908 Warsaw, Poland *Email: [email protected]
Recently, the origin of antiferroelectricity is widely discussed in literature. Basing on the lattice dynamics in PbZrO 3 a phenomenological model with competing interactions between AFE and FE modes was proposed by Tagantsev [1]. It is well know that competing interactions can be strengthened by doping or pressure. Consequently some chemical modifications by different cation replacement can strengthen either FE mode (i.e. Ti 4+ ) or AFE mode (i.e. Sn 4+ ) [2]. Form the available literature it is known that doping of PbZrO 3 with BiFeO 3 less than 20% does not alter the parent orthorhombic structure of PbZrO 3 [3]. PbZrO 3 is as classical antiferroelectric with Pbam orhorhombic space group [1] whereas BiFeO 3 is known as multiferroic possessing rohombohedral R3m structure [3]. Here we reinvestigate the phase transitions sequence of PbZrO 3 substituted with small amount ( up to mol 4% ) of BiFeO 3 by means of, micro-Raman scattering, dielectric and differential scanning calorimetry (DSC) measurements. Polycrystalline powders of PbZrO 3 (PZ), 0.98PbZrO 3-0.02BiFeO 3 (0.98PZ- 0.02BF) and 0.96PbZrO3-0.04BiFeO 3 (0.96PZ-0.04BF) were synthesized by means of Molten Salt Synthesis (MSS) route. The crystalline structure and morphology were studied by X-ray diffraction and scanning electron microscopy, respectively. The frequencies of the Raman lines were analyzed and discussed in terms of the sequence of structural phase transitions. The measurements revealed the existence of new intermediate phase below TC and an additional anomaly at T2 most likely connected with magnetic transition coming from BF contribution. The incorporation of multiferroic BiFeO 3 (BF) into the structure of aniferroelectric PbZrO 3 (PZ) suggests that (1-x)PZ-xBF solid solution forms a multiferroic system even for low BF content. The Raman measurements were supplemented by dielectric and differential scanning calorimetry (DSC) measurements. Excellent agreement for transition temperatures obtained by means of these three techniques suggests that BF is uniformly distributed in the material without introducing any mechanical stress.
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References [1] A.K. Tagantsev et al., The origin of antiferroelectricity in PbZrO 3, Nat. Commun. 4, 2229 (2013) [2] I. Jankowska-Sumara, M. Podgórna, A. Majchrowski, J. Żukrowski, Thermal analysis of phase transitions in PbZr 1-xSn xO3 antiferroelectric single crystals , Journal of Thermal Analysis 128 , 2, 713-719 (2016) [3] R. Gerson, P. Chou, and W. J. James, Ferroelectric Properties of PbZrO 3– BiFeO 3 Solid Solutions, Journal of Applied Physics 38 , 55 (1967)
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Impact of external factors on electromagnetic properties of metamaterial absorbers in THz region
Minh Nguyet NGUYEN 1, The Linh PHAM 1, Van Huynh TRAN 1, Hong Luu DANG 1, Dac Tuyen LE 2, Dinh Lam VU 1, *
1Institute of Materials Science, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet, Hanoi, Vietnam 2Department of Physics, Hanoi University of Mining and Geology, 18 Pho Vien, Hanoi,Vietnam *Email: [email protected]
This year, the first theoretical elaboration of negative refractive index materials by Veselago reaches its 50-year milestone [1]. Since then, metamaterials have become one of the most sought-after research topics, continue to attract more interests. With unique responses when interacting with electromagnetic waves, metamaterials are promising for innovative technologies unattainable by ordinary natural materials. Through clever designs of the metamolecules, metamaterials could exhibit an unprecedented wide range of properties, such as negative refraction, perfect absorption and many more. Metamaterial absorber (MA) is one type of metamaterials which can achieve perfect absorption of electromagnetic waves [2]. It can be implemented for detection, sensing and imaging, with applications ranging from military field to health care and communication. On the other aspect, in regard to the operating frequency region of metamaterials, the Terahertz territory is accumulating attraction with applications covering from security screening, medical imaging to wireless communications, and others [3,4]. [2]-3]. Unfortunately, the unique electromagnetic resonance of these materials often occurs at a narrow frequency band and also is dependent on the polarization of the incident wave. The conventional MA structure with fixed geometrical parameters can only operate at a determined frequency, which impedes on its applications. To solve this hindrance, reconfigurable materials have been integrated into metamaterial structures to gain tunability. Hence, electromagnetic responses of MA structures can be modified by means of external stimulation [5]. For the first tunable MA, the study exploits vanadium dioxide (VO 2) as shown in Figure 1(a). The conductivity of VO 2 can be tuned by the optical pumping power incident [6]. Figure 1(b) presents the dependence of the absorption spectra on the conductivity of VO 2. When the conductivity of VO 2 increases, the absorption peak experiences a blue-shift. For the second tunable MA, indium antimonide (InSb) was implemented into the split-ring structure as shown in Figure 2(a). InSb is a narrow gap semiconductor material, thus it is responsive to temperature [7]. By tuning the conductivity of InSb through temperature, we are able to manipulate absorption peak of MA as presented in Figure 2(b).
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Figure 1. (a) Ring structure with VO 2: r 1 = 12 , r 2 = 10 , , r 3 = 4 , t = t s = 2 , a = 50 . (b) Absorption spectra of the ring structure with different conductivity of VO 2.
Figure 2. (a) Ring structure with InSb: r 1 = 12 , r 2 = 10 , c = 1 . (b) Absorption spectra of the integrated ring structure with different temperatures ranging from 260K to 360K.
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Finally, Figure 3(a) illustrates a tunable MA based on graphene, which is a single carbon layer arranged in a honeycomb lattice with several intriguing features such as high carrier mobility at room temperature with low loss and thermal stability [8] . By controlling the Fermi energy of graphene, the absorption peak of the MA can be modified as shown in Figure 3(b).
Figure 3. (a) Disk structure with graphene: r 1 = 12 . (b) Absorption spectra of the integrated disk structure with different Fermi energies .
Acknowledgement This research is funded by Vietnam National Foundation for Science and Technology Development (NAFOSTED) under grant number 103.02-2017.67
References [1] V. G. Veselago, Sov. Phys. Uspekhi , 10 , 509 (1968) [2] N. I. Landy, S. Sajuyigbe, J. J. Mock, D. R. Smith, W. J. Padilla, Phys. Rev. Lett. 100 , 207402 (2008) [3] H. Tanoto, L. Ding, J. H. Teng, Int. J. Terahertz Sci. Technol. 6, 1–25 (2013) [4] C. M. Watts, X. Liu, and W. J. Padilla, Adv. Opt. Mater. 24 , 98 –120 (2012) [5] J. P. Turpin, J. A. Bossard, K. L. Morgan, D. H. Werner and P. L. Werner, Int. J. Antennas Propag. , 2014 , 429837 (2014) [6] S. Wang, L. Kang, and D. H. Werner, Sci. Rep. 8, 189 (2018) [7] A. Keshavarz and A. Zakery, Appl. Phys. A 123 , 797 (2017) [8] D. Chen, J. Yang, J. Zhang, J. Huang, and Z. Zhang, Sci. Rep. 7, 15836 (2017)
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Synthesis and magnetic property of Sr 2MFeAsO 3 (M=V, Cr)
Thi Thu Ha NGUYEN 1,* , Z. BUKOWSKI 2, V.H. TRAN 2 1 Faculty of Physics and Astronomy, University of Wroclaw, Pl. Uniwersytecki 1, 50-137 Wrocław Poland 2Institute of Low Temperature and Structure Research, Polish Academy of Science, Okólna 2, 50-422 Wrocław, Poland *Email: [email protected]
In this work, we report on the synthesis and properties of two isostructural oxyarsenides Sr 2VFeAsO 3 and Sr 2CrFeAsO 3. Sr 2VFeAsO 3 attract interest because of high superconducting critical temperature (T c=37.2 K) [1] coexisting with magnetic ordering of V sublattice [2]. Sr 2CrFeAsO 3 is not superconducting [3] and show a long- range magnetic ordering [4]. The polycrystalline samples with varied oxygen constent were synthesized by solid state reaction method. The phase purity and crystal structure were studied using powder X-ray diffraction. Magnetization measurements were used to characterize superconducting and magnetic properties. The samples synthesized from stoichiometric Sr 2VFeAsO 3 composition always contained Sr 2VO 4 as an impurity. The purity of samples is substantially improved when samples are prepared starting from nominal oxygen deficient composition Sr 2VFeAsO 3-δ(0< δ<0.6). The effects of oxygen deficient magnetic properties and superconductivity of
Sr 2VFeAsO 3−δ will be reported.
References [1] X. Zhu, F. Han, G. Mu, P. Cheng, B. Shen, B. Zeng, H. Wen, Phys. Rev. B 79 , 220512 (2009). [2] S. Tatematsu, E. Satomi, Y. Kobayashi, M. Sato, J. Phys. Soc. Jpn 79 , 123712 (2010). [3] H. Ogino, Y. Katsura, S. Horii, K. Kishio, J. Shimoyama, Supercond. Sci. Technol. 22, 085001(2009) [4] M. Tegel, F. Hummel, Y. Su, T. Chatterji, M. Brunelli, D. Johrendt, Europhys. Lett. 89 , 37006 (2010)
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Assessment of impacts to biodiversity forest in Dong Chau forest - Nuoc Trong stream, Kim Thuy commune, Le Thuy district, Quang Binh province
VU H. A *, PHUONG L. T. T. Faculty of Agriculture, Forestry and Fisheries, Quang Binh University, 312 Ly Thuong Kiet Str, Dong Hoi, Quang Binh, Vietnam *Email: [email protected]
Dong Chau forest - Nuoc Trong stream is located in Le Thuy district, Quang Binh province, in the Southwest, joining with Laos - Vietnam border and Nature Reservs North Huong Hoa (Quang Tri province) [1-3]. Investigations results of the flora in the area of Nuoc Trong stream has 987 species [2]. However, negative impacts on forests, such as illegal logging and trapping of wildlife, are still occurring that seriously affect the biodiversity and conservation value of one of the few areas of high Forest cover accounts for 99% of the total area.in scientific researchs and conservation of biodiversity resources in geographical researchs.
References [1] Quang Binh Provincial FPD, 2014). Final Report on Conservation. [2] Thanh L.D, 2013. Thesis: Studying characteristics of flora of Khe Nuoc Trong area to propose establishment of Khe Nuoc Trong Nature Reserve in Quang Binh province, Institute of Ecology and Biological Resources, forestry science and technology of Vietnam. [3] Trung T.V, 1997. Tropical Forest Ecosystems in Vietnam, Science and Technology Publishing House.
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Khan Academy - a platform supporting the teaching and learning process in Poland
Anna Michniewska Pedagogical University, Podchorazych 2,30-084 Krakow, Poland Email: [email protected]
The development of information and telecommunications technologies that took place at the beginning of the 21st century opened new opportunities in distance learning. Social changes that have taken place at the turn of recent years, in particular the need to acquire knowledge throughout life, justify the need to develop new methods that allow learning regardless of age, place, origin or stage of education. Thanks to the development of technology, people can use e-learning courses or virtual universities in any place on Earth [1] MOOC courses are an excellent solution for remote education - massive, open online courses ("Massive Open Online Courses") that bring together people wanting to acquire knowledge and become a part of the community of like-minded people. According to Gra żyna Penkowska, the foundations of MOOCs are that every person has the right to learn throughout life [2]. Remote teaching systems offer recipients a wide range of education using global information resources, enabling the acquisition of knowledge beyond the framework of teaching and textbook content [3]. The broadly understood openness of e-learning courses and MOOCs meant that the teaching and learning process is no longer only identified with the walls of a school or university [4]. New media are conducive to learning based on interaction and participation, rather than on passive learning [5]. One example of mass courses in which participation takes place via the network is Khan Academy. This platform has a broad base of materials in the form of films, articles and exercises. The author of the publication have analyzed the resources of the Polish platform to quantify the materials that can be used by students and teachers in the teaching and learning process.
References [1] J. Bednarek, E. Lubina, Kształcenie na odległo ść . Podstawy dydaktyki, Wydawnictwo Naukowe PWN SA, Warszawa (2008) [2] G. Penkowska, E-learning w dobie MOOC’s [in:] Człowiek-Media-Eduakcja, red. nauk. J. Morbitzer, D. Mora ńska, E. Musiał, Wydawnictwo Naukowe Wy ższej Szkoły Biznesu w Dąbrowie Górniczej, D ąbrowa Górnicza (2015) [3] A. Barczak, J. Florek, S. Jakubowski, T. Sydoruk, Zdalna edukacja. Potrzeby, problemy, szanse i zagro żenia, Warszawa (2006) [4] K. Gurba MOOC. Historia i przyszło ść , Uniwersytet Papieski Jana Pawła II w Krakowie Wydawnictwo naukowe Kraków (2015) [5] E. Musiał, Szkoła w cyfrowym świecie – w stron ę idei partnerstwa edukacja [in:] Człowiek-Media-Eduakcja, J. Morbitzer, D. Mora ńska, E. Musiał, Wydawnictwo Naukowe Wy ższej Szkoły Biznesu w Dąbrowie Górniczej, D ąbrowa Górnicza (2015)
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Session 5
O-23 PHAM Van Phuc Fabrication of the MA/FA/Cs triple cation perovskite solar cells using one-step and two-step approaches
O-24 MAI Thi Ly DFT study of electronic structure properties of SrAFe 4As 4 (A = Rb and Cs) superconductors
O-25 TRAN Van Hau Functional integral method in quantum field theory of Dirac fermions in graphene
O-26 NGUYEN Viet Dung Effects of filler surface on molecular mobility and resulting deformation and fracture behaviour of thermoplastic polymer composites
O-27 TRUONG Van Canh Provincial spatial distribution of Gini coefficient in Vietnam
O-28 Malwina KOSTRZEWSKA-OBERTANIEC Trust of Youth to the local government
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Fabrication of the MA/FA/Cs triple cation perovskite solar cells using one-step and two-step approaches
Phuc V. PHAM 1, Lien T.D. THACH 2, Chi H. LE 2* 1University of Engineering and Technology of Hanoi, E3 Building, 144 Xuan Thuy Street, Cau Giay, Hanoi, Vietnam 2Institute of Materials Science, Vietnamese Academy of Science and Technology, 18 Hoang Quoc Viet Street, Cau Giay District, Hanoi, Viet Nam *Email: [email protected]
In the last few years, organometallic halide perovskites have been received great attention as promising photovoltaic materials due to their unique structure and physical-chemical properties such as large optical absorption coe fficient, high charge carrier mobility, tunable band gap and easy processability at low temperature. Herein we studied a one-step and two-step solution approaches for the MA/FA/Cs triple cation layers. The crystalline structure, morphology, coverage, pore-filling and characterization of the deposited mixed-cation perovskite layers were investigated. We found that the enhanced photovoltaic performance of the two-step processed MA/FA/Cs triple cation perovskite solar cell was attributed to the reduced recombination traps due to the better crystalline quality and larger grain size.
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DFT study of electronic structure properties of SrAFe 4As 4 (A = Rb and Cs) superconductors
Thi Ly MAI * and Vinh Hung TRAN Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P. O. Box 1410, 50-422 Wroclaw, Poland *Email: [email protected]
Superconductivity in SrAFe 4As 4 (A = Rb and Cs) with Tc = 35 - 37 K has recently been reported [1]. The materials have a tetragonal structure with space group P4/mmm. The structure is built of atomic layers; those of the Sr and A atoms are inserted alternatively between the Fe 2As 2 layers along the c-axis. With the aim of better understanding the relationship between the electronic structure of SrAFe 4As 4 (A = Cs and Rb) and their superconducting properties, we have performed theoretical investigation based on DFT methods. The calculations have been made with the full- potential linearized augmented plane wave (FP-LAPW) approach as implemented in ELK code [2]. We have used the generalized gradient approximation (GGA) of Perdew - Burke - Ernzerhoft [3]. Based on calculated spin-up and spin-down DOS data we conclude that there is no spin polarization effect and the DOS may be characterized by four peak-structured regions centering around -4.50, -2.70, -0.37 and 1.10 eV. The farthest region below Fermi energy EF is due to valence band of As 4 p orbitals, the second region is contributed by a mixture of Fe 3 d and As 4 p orbitals, and the last two regions are due mainly to the Fe 3 d orbitals. It is worthwhile to point out that the peak located at -0.37 eV resembles Van Hove singularity, suggestive of electronic instabilities in the investigated superconductors. The total DOS for both 2 spin directions at EF is 9.6 states/(eV f.u.), corresponding to 22.6 mJ/(mol.K ). The high-Tc superconductivity of SrAFe 4As 4 can be ascribed to electronic bands crossing EF. We observe that these bands appear only along high symmetry lines lying in planes perpendicular to the Z-G direction. The Fermi surface formed by these bands evidence that that the FS of SrAFe 4As 4 have six hole-type cylindrical 2D-like sheets around the Z-G line and four electron-type located at the corners of the Brillouin zone. It is worthwhile to point out that the hole-type FS sheets of Rb-based superconductor are reminiscent of shape of nodal d-wave gap superconductors. The electron localization function iso-surfaces exhibit different electron distribution around atoms involved. Relatively high ELF values around Rb (Cs), Sr and As suggest strong covalent bonding whereas low ELF values around Fe atoms definitively point to intermetallic character. We will present DFT prediction 57 Fe Mossbauer Isomer Shifts and Quadrupole Splittings in SrAFe 4As 4 and compare their EBS with those of SrFe 2As 2.
Acknowledgments The work was supported by the National Science Centre (Poland) under the Grant No.2016/21/B/ST3/01366.
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References [1] A. Iyo et al. J. Am. Chem. Soc., 138, 3410 (2016). [2] Dewhurst, J. K. et al. Elk FP-LAPW code, version 4.3.6, http://elk.sourceforge.net , Date of access: 20/4/2017 (2017). [3] John P. Perdew, Kieron Burke and Matthias Ernzerhof, Phys. Rev. Lett. 78, 1396 (1997).
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Functional integral method in quantum field theory of Dirac fermions in graphene
TRAN Van Hau 1,2,* , Nguyen Van Hieu 1,2 1Institute of Materials Science, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet, Cau Giay, Hanoi, Vietnam 2VNU-University of Engineering and Technology, 144 Xuan Thuy, Cau Giay, Hanoi, Vietnam *Email: [email protected]
The purpose of present work is to elaborate the functional integral method in quantum field theory of Dirac fermions in the Dirac fermion gas of a graphene single layer at vanishing absolute temperature. The starting point to be assumed as the fundamental principle of the theory is the explicit expression of the action functional of this system. The efficient mathematical tool to be used in the study is the generating functional containing the Grassmann parameters anticommuting with the Dirac fermion field operators. The analytical expression of the generating functional of free Dirac fermion system is exactly derived and efficiently used in the study of 2n-point Green functions of free Dirac fermions. Then the celebrated Hubbard-Stratonovich transformation is applied to rewrite the functional integral of the interacting system of Dirac fermions in a new form expressing in terms of a scalar Hermitian quantum field describing the collective excitations in the interacting Dirac fermion gas and related to the graphene plasmons Keywords: functional integral, Dirac fermions, collective excitations, generating functional, Green functions
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Effects of filler surface on molecular mobility and resulting deformation and fracture behaviour of thermoplastic polymer composites
Viet Dung NGUYEN 1,2,3,* , Ke The NGO 1 and Jiri KOTEK 3 1Institute of Materials Science, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet, Cau Giay, Ha Noi, Vietnam 2Graduate University of Science and Technology, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet, Cau Giay, Ha Noi, Vietnam 3Institute of Macromolecular Chemistry, Academy of Sciences of the Czech Republic, Heyrovský Sq. 2, 162 06 Prague 6, Czech Republic *Email: [email protected]
Modification of thermoplastic polymers via addition of rigid particulate fillers has a long history, and it further continues to play a significant role. The reason is the possibility to tailor end-use properties in very wide intervals, thus expanding their applications. The fillers affect physical and mechanical behavior of matrix polymer in many ways. In this study, the isotactic polypropylene, a semicrystalline polymer, was used as a matrix for composites containing 20% and 40% (by weight) of glass beads filler. Selected surface treatment was applied to obtain different adhesion between particles and polymer matrix. In addition to non-treated filler, filler treated with i) a release agent (labelled as NO adhesion) and ii) an adhesion promoter (labelled as GOOD adhesion) were incorporated into the matrix. The morphology, tensile mechanical and fracture behaviour ( J-integral) were investigated. Morphology observation revealed a poor interfacial adhesion in the case of non-treated and “NO adhesion” samples represented with debonding of particles. In contrast, strong particle-matrix interactions were confirmed in “GOOD adhesion” samples. The presence of rigid filler particles increased the stiffness, while strain at break was decreased with the lowest value for the composites with strong interfacial adhesion. On the other hand, the higher rigidity and lower deformability decreased in fracture toughness, Figure 1. Solid state 1H and 13 C NMR experiments were also applied to recognize the changes in molecular mobility in these composites. The most mobile polymer segments were found in parent PP, while the most rigid polymer segments were found in the composite with “GOOD adhesion” as is reflected by the broadest 1H MAS NMR line in Figure 2.
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Figure. 1. Fracture toughness of PP/glass beads composites.
Figure. 2. 1H MAS NMR spectra of PP/glass beads composites Recorded at 350 K and MAS 6 kHz.
Acknowledgement This work was supported by the Czech Academy of Sciences, UNESCO and IUPAC named "UNESCO/IUPAC Postgraduate Course in Polymer Science".
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Provincial spatial distribution of Gini coefficient in Vietnam
Van Canh TRUONG Faculty of Geography and Regional Studies, University of Warsaw, Krakowskie Przedmie ście 30, 00-927 Warsaw, Poland Email: [email protected]
The Gini index or Gini coefficient is a statistical measure of distribution developed by the Italian statistician Corrado Gini in 1912. It is often used as a gauge of economic inequality, measuring income distribution or, less commonly, wealth distribution among a population [1]. The coefficient ranges from 0 to 1, with 0 representing perfect equality and 1 representing perfect inequality. Recently, in Vietnam, data for Gini coefficient is conducted by General Statistics Office of Viet Nam every year for whole country, regions, rural and urban area. Yet we are still lacking the data for Gini coefficient at provincial level which can help us have an overall view about provincial income inequality. The article presents a method for measuring Gini coefficient at provincial level by data for 5 income quintiles of population of provinces from the results of Vietnam household living standards survey and illustrates provincial Gini coefficient on map to comprehend spatial distribution of income inequality in Vietnam. The Gini coefficient is calculated by subtracting the sum of the two cumulative percentages of the average person spending one person per month for two successive men (average spending per person per month (January price of the year to be calculated and the same price level) in incremental order) and their cumulative percentages [1]. The Gini (G) coefficient is calculated by the following formula: