Preparation and Characterization of (Gesbte)) Semiconductors for Phase-Change Optical Storage Hessa Ali Humeid Al-Shamisi

Total Page:16

File Type:pdf, Size:1020Kb

Preparation and Characterization of (Gesbte)) Semiconductors for Phase-Change Optical Storage Hessa Ali Humeid Al-Shamisi United Arab Emirates University Scholarworks@UAEU Theses Electronic Theses and Dissertations 2008 Preparation and Characterization of (GeSbTe)) Semiconductors for Phase-Change Optical Storage Hessa Ali Humeid Al-Shamisi Follow this and additional works at: https://scholarworks.uaeu.ac.ae/all_theses Part of the Materials Science and Engineering Commons Recommended Citation Humeid Al-Shamisi, Hessa Ali, "Preparation and Characterization of (GeSbTe)) Semiconductors for Phase-Change Optical Storage" (2008). Theses. 293. https://scholarworks.uaeu.ac.ae/all_theses/293 This Thesis is brought to you for free and open access by the Electronic Theses and Dissertations at Scholarworks@UAEU. It has been accepted for inclusion in Theses by an authorized administrator of Scholarworks@UAEU. For more information, please contact [email protected]. United Arab Emirates University Deanship of Graduate Studies PREPARATION AND CHARACTERIZATION OF (GeSbTe) SEMICONDUCTORS FOR PHASE-CHANGE OPTICAL STORAGE By Hessa Ali Humeid AI-Shamisi Supervised by Dr. Hassan Ghamlouche Physics Department Faculty of Science, UAEU Dr. Naser Qamhieh Dr. Saleh Thaker Physics Department Physics Department Faculty of Science, UAEU Faculty of Science, UAEU A Thesis Submitted to the Deanship of Graduate Studies in Partial Fulfillment of the Requirements fo r Degree of Master of Science in Materials Science and Engineering 2008 Acknowledgments First, always and fo remost, I thank almighty Allah fo r rus blessing and fo r providing me the capability to successfullycomplete trus work. I would like to express my heartiest thanks and sincere gratitude to my supervisors, Dr. Hassan Ghamlouche, Dr. Naser Qamrueh and Dr. Saleh Thaker fo r their guidance, support, encouragement, patience, unlimited assistance, critical reviewing and providing me the required fa cilities during the work. 1 fe el both honored and privileged to work with such a group. Many thanks to Mr. Mohammed Elshaer (lab technician in the physics department) and Mr. Esam Attia (technician in the Central Lab Unit), fo r their help in preparing some experiments and analyzing the samples. Special thanks to Ms. Sadeeqa Ahmed, from the physics department, fo r her assistance and support. Special appreciation is expressed to my colleagues and friends in UAE University, especially in the physics department. No words can ever express my great gratitude and special thanks to my great fa mily, especially my parents fo r their great support and my husband fo r his patience and great help throughout my study. II Abstract In the last decade, the phase change optical recording based upon chalcogenide glasses has advanced remarkably at full-scale commercial applications in the fo rm of rewritable compact disks (CD-RWs) and digital video disks (DVD-RWs). The principle of phase-change optical recording is based on a thermally induced reversi ble transformation between amorphous and crystalline phases. The search fo r recording materials possessing fa st crystallization rate and long data retention has been pursued. Research results have revealed that Ge-Sb-Te compounds exhibit fa st crystallization, which has been explained in terms of their single-phase structure. In the present work, electrical properties of Ge-Sb-Te thin films using Impedance Spectroscopy, Current-Voltage, and Capacitance-Voltage techniques is presented. First, we studied the effect of the electrical contacts, deposited on top of Ge-Sb-Te films, on the measured electrical signal (Impedance Spectroscopy). To do this, three different configurations of the electrical contacts were prepared. The results show that the electrical contacts have no effect when the silver paste is placed on the gold electrodes away from the thin film under test. This guarantees no interaction between the silver paste and the film under test during the heating process. Also the results show that the order of depositing layers (material and the gold) is not important and what matters is the location of the silver paste on the gold electrodes. Second, the Impedance Spectroscopy and Current-Voltage data shows similar resistance and relaxation frequency temperature dependence with activation energies 0.36 and 0.39 eV, respectively. Therefore the corresponding energy gap is estimated to be 0.72 eV and 0.78 eY. This result agrees with the optical gap (0.7 eV) reported in literature. This agreement co nfirms that Ge2Sb2 Te5 belongs to the chalcogenide fa mily. In addition, " III the I-V curves show that the amorphous-crystalline transition temperature (Tc is around 135 °C Third, the Capacitance-Voltage measurements were performed on amorphous samples of Ino.3Ge2Sb2 Te5 and Ge2Sb2Tes thin films in order to study the effect of doping on the electrical properties of Ge2Sb2 Te5. The results show that inducing Indium to Ge2Sb2 Tes decrease the capacitance of the sample as the bias voltage increases fo r the whole range of temperatures. However, the same behavior is observed fo r undoped sample (Ge2Sb2 Te5) only at temperatures close to the amorphous-crystalline transition temperature and at high applied bias voltages (� 15 volts). The behavior is attributed to the increase in electron concentration as the bias voltage and temperature increase. For lno.3Ge2Sb2 Te5 sample, the indium can be considered as an additional source of free electrons. This would contribute to a furtherand significant decrease in the capacitance ofIno.3Ge2Sb2 Te5 sample, and eventually the capacitance becomes negative. The nonlinearity in the capacitance and conductivity could be related to the nucleation mechanism as the temperature becomes clo e to the amorphous-crystalline transition temperature. Finally in the conclusion 1 proposed some study to be conducted on Ge2Sb2 Te5 films. o IV TABLE OF CONTENTS LIST OF FIGUR ES ...................................................................................................... VII LIST OF TABLES ........................................................................................................ IX CHAPTER I ........................................................................................................... 1 INTRODUCTION ........................................................................................................... 1 CHAPTER II ........................................................................................................... 5 THEORETICAL BACKGROUND ................................................................................. 5 2. 1 Introduction ....................................... ........................ ................. ...... ............ .. 5 2.2. Glass fo rmation and the amorphous phase ..................... ............... ................ ....... 6 2.3 Phase-change materials ......... .................. ............. .......... ........ '" .........................9 2.3.1 Chalcogenides . .................... ...... .......... ................ ...... ............. ............ ... 10 2.4 Density of states in amorphous semiconductors ..... ....................... ...................... 13 2 5 Conduction in amorphous semiconductors ...... ............ ............. .......................... 16 2.5.1 Extended state conduction........ ........... ....... ............ ............ ..... .............. .... 17 2.5.2 Hopping conductivity ..................... .................. ........... .............................. 19 2.6 AC conductivity ... .............. .... ......... ......... ... .................... ........ .... ................... 20 CHAPTERll ......................................................................................................... 24 SAMPLE PREPARATION AND EXPERIMENTAL TECHNIQUES . ...................... 24 3. 1 Sample preparation ...... .......... .. ...., ................................................................. 26 3.1.1 Preparation of bulk materials .. ... .. .......... ................. ............ · ........ · ··· · ........ 26 3 1.2 Thermal Evaporation Technique (TE) .......... ........ ............ .......................... 27 3. 1 . 3 Sputtering Technique ........................... ............. ...... · ..... .......· .................. · 28 3 .1.4 Deposition of electrodes ................... ...............········ ··································· 28 o v 3 2 Mea uring Technique ...... ... ... ........... ....... ........ .... ................. ....... ...... ... ... 29 3 2.1 The impedance pectroscopy ........... ......... ... ............. ..... .... ... ... .... ........... .. 29 3 .2.2 Current-Voltage technique ... .................... ........ ......... .... ... ... ... ................. 31 3.2.3 Capacitance-Voltage technique . ..... ... ... ........... ....... ..... ... .................. ..... 31 CHAPTER IV ......................................................................................................... 32 RESULTS AND DISCUSSIONS .............. .. ...................... .............. ............................. 32 4. 1 DC Measurements .... ... .......... ....... ...... ........... ...... ...... ...... ... .... .......... ............. 32 4.2 Impedance spectroscopy measurements ......... ............ ...... ........................... .. 35 43 Capacitance-Voltage measurements of Ge2Sb2Tes and Ino.3Ge2Sb2Tes ....... ... ...... 42 ................................. ......... ..................... ....... ................. .. ... CONCLUSION ....... 51 REFERENCES ................................................. .......... ...........................................
Recommended publications
  • Reduction of Rocksalt Phase in Ag-Doped Ge2sb2te5: a Potential Material for Reversible Near-Infrared Window
    PHYSICAL REVIEW APPLIED 10, 054070 (2018) Reduction of Rocksalt Phase in Ag-Doped Ge2Sb2Te5: A Potential Material for Reversible Near-Infrared Window Palwinder Singh,1,2 A.P. Singh,3 Jeewan Sharma,4 Akshay Kumar,4 Monu Mishra,5 Govind Gupta,5 and Anup Thakur2,* 1 Department of Physics, Punjabi University, Patiala, Punjab 147002, India 2 Advanced Materials Research Lab, Department of Basic and Applied Sciences, Punjabi University, Patiala, Punjab 147002, India 3 Department of Physics, Dr. B. R. Ambedkar National Institute of Technology, Jalandhar 144011, India 4 Department of Nanotechnology, Sri Guru Granth Sahib World University, Fatehgarh Sahib, Punjab 140407, India 5 Advanced Materials and Devices Division, CSIR-National Physical Laboratory, New Delhi 110012, India (Received 15 July 2018; revised manuscript received 1 November 2018; published 30 November 2018) Phase-change materials are attracting much attention in the scientific and engineering communities owing to their applications and underlying basic phenomena. Ge2Sb2Te5 is reversible-phase-change mate- rial (amorphous to crystalline and vice versa) that is used for optical data storage and phase-change random-access memory and has recently been explored for use as a reversible near-infrared (NIR) win- dow [Singh et al., Appl. Phys. Lett. 111, 261102 (2017)]. For a reversible NIR window, large transmission contrast between two phases and low phase-transition temperature are required to reduce the power con- ( ) = sumption. In the present work, phase transition in thermally deposited Ge2Sb2Te5 100−xAgx (x 0, 1, 3, 5, and 10) thin films is achieved by vacuum thermal annealing. Transmission sharply decreases with phase transition in the NIR region.
    [Show full text]
  • Phase-Change Properties of Gesbte Thin Films Deposited by Plasma
    Song et al. Nanoscale Research Letters (2015) 10:89 DOI 10.1186/s11671-015-0815-5 NANO EXPRESS Open Access Phase-change properties of GeSbTe thin films deposited by plasma-enchanced atomic layer depositon Sannian Song1*, Dongning Yao1, Zhitang Song1, Lina Gao2, Zhonghua Zhang1,LeLi1, Lanlan Shen1, Liangcai Wu1, Bo Liu1, Yan Cheng1 and Songlin Feng1 Abstract Phase-change access memory (PCM) appears to be the strongest candidate for next-generation high-density nonvolatile memory. The fabrication of ultrahigh-density PCM depends heavily on the thin-film growth technique for the phase-changing chalcogenide material. In this study, Ge2Sb2Te5 (GST) and GeSb8Te thin films were deposited by plasma-enhanced atomic layer deposition (ALD) method using Ge [(CH3)2 N]4,Sb[(CH3)2 N]3,Te (C4H9)2 as precursors and plasma-activated H2 gas as reducing agent of the metallorganic precursors. Compared with GST-based device, GeSb8Te-based device exhibits a faster switching speed and reduced reset voltage, which is attributed to the growth-dominated crystallization mechanism of the Sb-rich GeSb8Te films. These results show that ALD is an attractive method for preparation of phase-change materials. Keywords: Phase-change memory; Atomic layer deposition; Microstructure; Electric properties Background of the limited on-current drive capability of the cell tran- Phase-change memory (PCM) has been regarded as one sistor [6]. It has been reported that a confined cell struc- of the most promising nonvolatile memories for the next ture where the phase-change material is formed inside a generation because of the advantages of high speed, low contact via is expected to be essential for the next- power, good endurance, high scalability, and fabrication generation PCM device because it requires lower switch- compatibility with complementary metal-oxide semicon- ing power [7,8].
    [Show full text]
  • The Role of Local Structure in Dynamical Arrest
    Physics Reports 560 (2015) 1–75 Contents lists available at ScienceDirect Physics Reports journal homepage: www.elsevier.com/locate/physrep The role of local structure in dynamical arrest C. Patrick Royall a,b,c,∗, Stephen R. Williams d a HH Wills Physics Laboratory, Tyndall Avenue, Bristol, BS8 1TL, UK b School of Chemistry, University of Bristol, Cantock Close, Bristol, BS8 1TS, UK c Centre for Nanoscience and Quantum Information, Tyndall Avenue, Bristol, BS8 1FD, UK d Research School of Chemistry, The Australian National University, Canberra, ACT 0200, Australia article info a b s t r a c t Article history: Amorphous solids, or glasses, are distinguished from crystalline solids by their lack of long- Accepted 17 November 2014 range structural order. At the level of two-body structural correlations, glassformers show Available online 4 December 2014 no qualitative change upon vitrifying from a supercooled liquid. Nonetheless the dynamical editor: Randall Kamien properties of a glass are so much slower that it appears to take on the properties of a solid. While many theories of the glass transition focus on dynamical quantities, a solid's Keywords: resistance to flow is often viewed as a consequence of its structure. Here we address the Geometric frustration viewpoint that this remains the case for a glass. Recent developments using higher-order Locally favoured structures Model glassforming systems measures show a clear emergence of structure upon dynamical arrest in a variety of glass formers and offer the tantalising hope of a structural mechanism for arrest. However a rigorous fundamental identification of such a causal link between structure and arrest remains elusive.
    [Show full text]
  • Optical Properties and Phase-Change Transition in Ge2sb2te5 Flash Evaporated Thin Films Studied by Temperature Dependent Spectroscopic Ellipsometry
    Optical properties and phase-change transition in Ge2Sb2Te5 flash evaporated thin films studied by temperature dependent spectroscopic ellipsometry J. Orava1*, T. Wágner1, J. Šik2, J. Přikryl1, L. Beneš3, M. Frumar1 1Department of General and Inorganic Chemistry, Faculty of Chemical Technology, University of Pardubice, Cs. Legion’s Sq. 565, Pardubice, 532 10 Czech Republic 2ON Semiconductor Czech Republic, R&D Europe, 1. máje 2230, Rožnov pod Radhoštěm, 756 61 Czech Republic 3Joint Laboratory of Solid State Chemistry of the Institute of Macromolecular Chemistry AS CR, v.v.i. and University of Pardubice, Studentská 84, Pardubice, 53210 Czech Republic *Corresponding author: tel.: +420 466 037 220, fax: +420 466 037 311 *E-mail address: [email protected] Keywords: Ge2Sb2Te5, optical properties, ellipsometry, amorphous, fcc PACs: 07.60.Fs, 77.84.Bw, 78.20.-e, 78.20.Bh Abstract We studied the optical properties of as-prepared (amorphous) and thermally crystallized (fcc) flash evaporated Ge2Sb2Te5 thin films using variable angle spectroscopic ellipsometry in the photon energy range 0.54 - 4.13 eV. We employed Tauc-Lorentz model (TL) and Cody- Lorentz model (CL) for amorphous phase and Tauc-Lorentz model with one additional Gaussian oscillator for fcc phase data analysis. The amorphous phase has optical bandgap opt energy Eg = 0.65 eV (TL) or 0.63 eV (CL) slightly dependent on used model. The Urbach edge of amorphous thin film was found to be ~ 70 meV. Both models behave very similarly and accurately fit to the experimental data at energies above 1 eV. The Cody-Lorentz model is more accurate in describing dielectric function in the absorption onset region.
    [Show full text]
  • Glass Stability from Thermal, Structural and Optical Properties for IR Lens Application
    Journal of the Korean Ceramic Society https://doi.org/10.4191/kcers.2017.54.6.08 Vol. 54, No. 6, pp. 484~491, 2017. Communication Evaluations of Sb20Se80-xGex (x = 10, 15, 20, and 25) Glass Stability from Thermal, Structural and Optical Properties for IR Lens Application Gun-Hong Jung*, Heon Kong*, Jong-Bin Yeo**, and Hyun-Yong Lee***,† *Department of Advanced Chemicals and Engineering, Chonnam National University, Gwangju 61186, Korea **The Research Institute for Catalysis, Chonnam National University, Gwangju 61186, Korea ***School of Chemical Engineering, Chonnam National University, Gwangju 61186, Korea (Received June 30, 2017; Revised September 24, 2017; Accepted October 22, 2017) ABSTRACT Chalcogenide glasses have been investigated in their thermodynamic, structural, and optical properties for application in vari- ous opto-electronic devices. In this study, the Sb20Se80-xGex with x = 10, 15, 20, and 25 were selected to investigate the glass sta- bility according to germanium ratios. The thermal, structural, and optical properties of these glasses were measured by differential scanning calorimetry (DSC), X-ray diffraction (XRD), and UV-Vis-IR Spectrophotometry, respectively. The DSC results revealed that Ge20Sb20Se60 composition showing the best glass stability theoretically results due to a lower glass transi- tion activation energy of 230 kJ/mol and higher crystallization activation energy of 260 kJ/mol. The structural and optical anal- yses of annealed thin films were carried out. The XRD analysis reveals obvious results associated with glass stabilities. The values of slope U, derived from optical analysis, offered information on the atomic and electronic configuration in Urbach tails, associated with the glass stability.
    [Show full text]
  • Chemical Phase Segregation During the Crystallization of Ge-Rich Gesbte Alloys Marta Agati, Maxime Vallet, Sébastien Joulié, Daniel Benoit, Alain Claverie
    Chemical phase segregation during the crystallization of Ge-rich GeSbTe alloys Marta Agati, Maxime Vallet, Sébastien Joulié, Daniel Benoit, Alain Claverie To cite this version: Marta Agati, Maxime Vallet, Sébastien Joulié, Daniel Benoit, Alain Claverie. Chemical phase segre- gation during the crystallization of Ge-rich GeSbTe alloys. Journal of Materials Chemistry C, Royal Society of Chemistry, 2019, 7 (28), pp.8720-8729. 10.1039/c9tc02302j. hal-03015385 HAL Id: hal-03015385 https://hal.archives-ouvertes.fr/hal-03015385 Submitted on 4 Dec 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Chemical phase segregation during the crystallization of Ge-rich GeSbTe alloys Marta Agati,a Maxime Vallet,a Sébastien Joulie,a Daniel Benoit,b Alain Claverie.a,* a) CEMES-CNRS, 29 Rue Jeanne Marvig, 31055 Toulouse, France. b) STMicroelectronics, 850 Rue Jean Monnet, 38920 Crolles, France. [email protected] [email protected] [email protected] [email protected] [email protected] * Address all correspondence to Alain Claverie at [email protected] Key words: Phase Change Materials; GST alloys; transmission electron microscopy; phase separation; crystallization. Abstract Ge-rich Ge-Sb-Te alloys are foreseen materials for new non-volatile memories named Phase Change Memories offering an extended range of possible applications.
    [Show full text]
  • (12) Patent Application Publication (10) Pub. No.: US 2006/0172083 A1 Lee Et Al
    US 2006O172083A1 (19) United States (12) Patent Application Publication (10) Pub. No.: US 2006/0172083 A1 Lee et al. (43) Pub. Date: Aug. 3, 2006 (54) METHOD OF FABRICATING ATHIN FILM Publication Classification (75) Inventors: Jung-Hyun Lee, Yongin-si (KR); (51) Int. Cl. Charig-Soo Lee, Yongin-si (KR): C23C I6/00 (2006.01) Yoon-Ho Khang, Yongin-si (KR) (52) U.S. Cl. ......................................... 427/535; 427/248.1 Correspondence Address: HARNESS, DICKEY & PIERCE, P.L.C. (57) ABSTRACT E.SE O195 US Methods of fabricating a thin film. An example method 9 (US) includes forming a GeSbTe thin film on a surface of a (73) Assignee: Samsung Electronics Co., LTD Substrate by chemically reacting a first precursor including gnee. g es germanium (Ge), a second precursor including antimony 21) Appl. No.: 11A341.718 (Sb), and a third precursor including tellurium (Te) in a (21) Appl. No 9 reaction chamber and processing the surface of the GeSbTe (22) Filed: Jan. 30, 2006 thin film with hydrogen plasma. Another example method includes injecting at least one precursor into a reactor (30) Foreign Application Priority Data chamber and depositing the at least one precursor onto a Substrate within the reactor chamber using a chemical vapor Jan. 31, 2005 (KR)............................ 10-2005-OOO8753 deposition process so as to form the thin film. Patent Application Publication Aug. 3, 2006 Sheet 1 of 2 US 2006/0172083 A1 FIG. 1 (CONVENTIONAL ART) Patent Application Publication Aug. 3, 2006 Sheet 2 of 2 US 2006/0172083 A1 31 FIG. 2A PHYSICAL SORPTION PRECURSOR(SOURCE) . (e) CEucal-sortional US 2006/0172083 A1 Aug.
    [Show full text]
  • Young's Modulus and Residual Stress of Gesbte Phase-Change Thin Films
    Young's modulus and residual stress of GeSbTe phase-change thin films Hammad Nazeera, Harish Bhaskaranb, L´eonA Wolderinga, Leon Abelmanna,c,∗ aMESA+ Research Institute, University of Twente bDepartment of Materials, University of Oxford, Oxford, United Kingdom cKIST Europe, Saarbr¨ucken, Germany Abstract The mechanical properties of phase change materials alter when the phase is transformed. In this paper, we report on experiments that determine the change in crucial parameters such as Young's modulus and residual stress for two of the most widely employed compositions of phase change films, Ge1Sb2Te4 and Ge2Sb2Te5, using an accurate microcantilever methodology. The results support understanding of the exact mechanisms that account for the phase transition, especially with regards to stress, which leads to drift in non-volatile data stor- age. Moreover, detailed information on the change in mechanical properties will enable the design of novel low-power nonvolatile MEMS. Keywords: Youngs modulus, strain, phase change, GeSbTe, cantilever resonance 1. Introduction The present quest in Nanoelectromechanical Systems (NEMS) and Micro- electromechanical Systems (MEMS) is for ever-lighter and lower power tech- nologies, thus there is a constant effort to reduce device dimensions. The use 5 of phase change materials in such devices is a rather nascent concept, and is stymied by the lack of understanding of the exact nature of the mechanical ∗Corresponding author Email address: +49 6819382229, [email protected] (Leon Abelmann) Preprint submitted to Thin Solid Films September 7, 2015 property change in such materials. However, an understanding of the phase change transition will be transformational. For example, tunable resonators all require high speed tuning of the resonance frequency of mechanical resonators.
    [Show full text]
  • P020190719558587609057.Pdf
    microtechnology and mems Springer-Verlag Berlin Heidelberg GmbH microtechnology and mems Series Editor: H. Baltes D. Liepmann The series Microtechnology and MEMS comprises text books, monographs, and state-of-the-art reports in the very active field of microsystems and microtechno- logy. Written by leading physicists and engineers, the books describe the basic science, device design, and applications. They will appeal to researchers, engineers, and advanced students. Mechanical Microsensors By M. Elwenspoek and R. Wiegerink CMOS Cantilever Sensor Systems Atomic Force Microscopy and Gas Sensing Applications By D. Lange, O. Brand, and H. Baltes Micromachines as Tools for Nanotechnology Editor: H. Fujita H. Fujita (Ed.) Micromachines as Tools for Nanotechnology With 183 Figures 13 Professor I [iroyuki Pujita Th(' Univ('rsity ofTokyo [nstitut(' of [ndustrial Sci('nc(' 4-6-1 Komaba, Meguro-ku Tokyo 153-8505, lapan E-mail: [email protected] Scrics Edilors: Professor Dr, I r. l3altcs ETH Ziirich, Phy~ical Electronics Laboralory ETI 1 [lo('Jlgg('rb('rg, 1[1'T -l [6, 1:\093 llirich, Switz('rland Profcssor Dr. Dorian Licpmann Univ('rsity of California, D('partment of Bioengineering 466 Evan~ Hali, #1762, Berkeley, CA 94720-1762, USA ISSN 1615-8}26 ISBN 978-3-642-62465-0 l.ibrary o f Co ngn'S~ Calaloging_in_Publica tionllata Fujila, Hiroyuki. 1952- Mircromachin<?s as lools for nanolechno[og)' III. !'ujita. p. Cm. __ (Mi rcol~..:bnology and MEMS) Inc!udcs bibliographical referen"'. arul index. ISBN 978-3-642-62465-0 ISBN 978-3-642-55503-9 (eBook) DOI 10.1007/978-3-642-55503-9 1.
    [Show full text]
  • A Refractive Index Database of Chalcogenide Phase Change Materials for Tunable Nanophotonic Device Modelling
    PCM-net: A refractive index database of chalcogenide phase change materials for tunable nanophotonic device modelling Hyun Jung Kim1,2*, Jung-woo Sohn3, Nina Hong4, Calum Williams5, William Humphreys2 1. National Institute of Aerospace, Hampton, Virginia 23666, USA 2. NASA Langley Research Center, Hampton, Virginia 23666, USA 3. Institute for Life Science Entrepreneurship, New Jersey 07083, USA 4. J.A. Woollam Co., Inc, Lincoln, Nebraska 68508, USA 5. Department of Physics, Cavendish Laboratory, University of Cambridge, Cambridge, CB3 0HE, UK * corresponding author: [email protected] Keywords: online database; refractive index; phase change material; tunable; GeSbTe; nanophotonics; index modulation; optical metasurface; optical filter, PCM-net (http://nekocloud.com/pnet/); online repository; device modelling, Abstract The growing demand for multifunctional nanophotonic devices has led to the exploration, and utilization, of a plethora of exotic electro-optical materials. Recently, chalcogenide glass based phase change materials (PCMs) have shown utility as a tuning material for a range of nanophotonic devices. Owing to their low loss, ultrafast switching speeds and wide waveband operation, PCMs are integrated in an increasing number of next-generation tunable components, including integrated photonic switches, metasurface optics and tunable spectral filters. Nonetheless, modelling of PCM-based devices is challenging—both in terms of accurate representation of experimentally-derived material properties in different phase states, and standardization of results across the research community. Further, as each device requires optimization of specific performance metrics dependent on their respective application, any inaccuracies will lead to erroneous outcomes. In this work, we introduce PCM-net (http://nekocloud.com/pnet/): an online database of the complex refractive indices of a variety of chalcogenide glass PCMs (such as GeSbTe), as an accessible and indexed repository for data sharing across the PCM community.
    [Show full text]
  • Reconfigurable Flat Optics with Programmable
    Reconfigurable Flat Optics with Programmable Reflection Am- plitude Using Lithography-Free Phase-Change Materials Ultra Thin Films Sébastien Cueff, Arnaud Taute, Antoine Bourgade, Julien Lumeau, Stephane Monfray, Qinghua Song, Patrice Genevet, Xavier Letartre, L Berguiga To cite this version: Sébastien Cueff, Arnaud Taute, Antoine Bourgade, Julien Lumeau, Stephane Monfray, et al.. Reconfigurable Flat Optics with Programmable Reflection Am- plitude Using Lithography- Free Phase-Change Materials Ultra Thin Films. Advanced Optical Materials, Wiley, 2020, 10.1002/adom.202001291. hal-02996004 HAL Id: hal-02996004 https://hal-amu.archives-ouvertes.fr/hal-02996004 Submitted on 9 Nov 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Distributed under a Creative Commons Attribution| 4.0 International License Reconfigurable Flat Optics with Programmable Reflection Am- plitude Using Lithography-Free Phase-Change Materials Ultra Thin Films S´ebastien Cueff Arnaud Taute Antoine Bourgade Julien Lumeau Stephane Monfray Qinghua Song Patrice Genevet Xavier Letartre Lotfi Berguiga* Dr. L. Berguiga Universit´ede Lyon, Institut des Nanotechnologies de Lyon - INL, UMR 5270, INSA Lyon - CNRS, 69621 Villeurbanne, France Email Adress: lotfi[email protected] Dr S. Cueff, A. Taute, Dr. X. Letartre Universit´ede Lyon, Institut des Nanotechnologies de Lyon - INL, UMR 5270, Ecole Centrale de Lyon - CNRS, 69134 Ecully, France A.
    [Show full text]
  • Laser Revolution Overview and Status of Direct-Drive Inertial Confinement Fusion
    MON-1-PL1 MON-1-PL2 The Fibre Laser Revolution Overview and status of Direct-Drive Inertial Confinement Fusion David N. Payne E. M Campbell Optoelectronics Research Centre, University of Southampton, Southampton, United Kingdom SO31 4QG Laboratory for Laser Energetics, University of Rochester, Rochester, NY 14623, USA [email protected] [email protected] Fibre lasers have been a revolution in laser technology for the manufacturing industry because of their high Laser Direct Drive (DD) is one of the three viable approaches for Inertial Confinement Fusion (ICF) that offer a efficiency, robust, all solid state monolithic construction and reliability. The single-fibre power limit appears to potential path for high yield and ignition at the MegaJoule energy scale of the National Ignition Facility (NIF). The be around 20kW, more than enough for most applications. critical physics for direct drive is being studied on the OMEGA/OMEGA-EP and the NIF laser facilities. In the DD approach nominally identical laser beams are used to drive an imploding cryogenic shell of deuterium and tritium Fibre lasers have also caught the imagination for applications requiring beam combination up to a 100kW in the to obtain pressures exceeding 100 Gbars and temperatures greater than 5 KeV in a hot spot surrounded and near term, or multi MW in the future. Their near-perfect beam quality, stability and versatility, coupled with confined by a cold dense nearly Fermi-Degenerate fuel. Hydrodynamically scaled implosions are studied on the the low cost of the gain medium, make them ideal candidates for coherently-combining perhaps up to a 1000 30 kJ 60-beam OMEGA laser.
    [Show full text]