(12) Patent Application Publication (10) Pub. No.: US 2006/0172083 A1 Lee Et Al

Total Page:16

File Type:pdf, Size:1020Kb

(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. 3, 2006 METHOD OF FABRICATING ATHIN FILM region 11b and the lower electrode 16. The heat generated by the Supplied current may adjust a phase state of the phase PRIORITY STATEMENT change film 17 (e.g., to convert or maintain the phase change film 17 at one of a crystalline state and an amorphous 0001. This application claims priority of Korean Patent state), where a resistance corresponding to the phase state of Application No. 10-2005-0008753, filed on Jan. 31, 2005, in the phase-change film 17 may be indicative of a first logic the Korean Intellectual Property Office, the disclosure of level (e.g., a higher logic level or logic “1”) or a second logic which is incorporated herein in its entirety by reference. level (e.g., a lower logic level or logic “0”). The supplied current may be controlled so as to set a phase state of the BACKGROUND OF THE INVENTION phase-change film 17. 0002) 1. Field of the Invention 0010. A conventional phase-change material which may 0003. Example embodiments of the present invention be used in the PRAM 100 may be a compound including relate to a method of fabricating a thin film, and more germanium (Ge), antimony (Sb), and tellurium (Te) (e.g., particularly to a method of fabricating a thin film having GST or GeSbTe). In another example, the phase-change film reduced impurities. may be embodied as a chalcogenide material layer. 0004 2. Description of the Related Art 0011 A power consumption of the conventional PRAM 100 may be reduced by reducing its current consumption. In 0005. A phase-change material may be selectively con an example where the PRAM 100 includes GST, a reset verted between crystalline and amorphous states based on an current (e.g., a current for transitioning from a crystalline operating temperature. A phase-change material may have a state to an amorphous state) may be higher, thereby con lower resistance when in a crystalline state as compared to Suming higher amounts of power during an operation of the the phase-change material in an amorphous state. In the crystalline state, the phase-change material may be charac PRAM 1 OO. terized as having a systematic or ordered arrangement of 0012. A conventional GST thin film may be fabricated atoms. The phase-change material may be reversibly with a physical vapor deposition (PVD) process. If a thin changed between the crystalline and amorphous states Such film is deposited using the PVD process, it may be difficult that a conversion from one state to the other may not be to control the thin film growth, the speed of deposition of the permanent. A phase-change random access memory thin film may be lower, and the thin film may not have a (PRAM) device may be a memory device having charac sufficient density. Additionally, the thin film may be difficult teristics of the phase-change material. A resistance of a to form in Smaller regions. Accordingly, a contact area PRAM may vary based on a state (e.g., crystalline, amor between a heating unit (e.g., Supplying the Supply current) phous, etc.) of a phase-change material included therein. and the thing film (e.g., including GST) may increase. Heat loss may thereby be increased due to the increased contact 0006. A conventional PRAM may include a phase area. The increased heat loss characteristic may cause higher change film electrically connected to source and drain levels of reset current to be applied in the PRAM 100 so as regions through a contact plug. The PRAM may be config to precipitate a phase state change. Therefore, it may be ured to operate in accordance with the variation in resistance caused by a state change (e.g., to a crystalline structure, to difficult to employ conventional PRAMs at higher integra an amorphous structure, etc.) in the phase-change film. tions. 0007 FIG. 1 illustrates a cross-sectional view of a con SUMMARY OF THE INVENTION ventional PRAM 100. Referring to FIG. 1, the conventional PRAM 100 may include a first impurity region 11a and a 0013 An example embodiment of the present invention second impurity region 11b on a semiconductor Substrate 10. is directed to a method of fabricating a thin film, including The conventional PRAM 100 may further include a gate forming a GeSbTe thin film on a surface of a substrate by insulating layer 12 contacting the first and second impurity chemically reacting a first precursor including germanium regions 11a and 11b and a gate electrode layer 13. The gate (Ge), a second precursor including antimony (Sb), and a insulating layer 12 and the gate electrode layer 13 may each third precursor including tellurium (Te) in a reaction cham be stacked on the substrate 10. The first impurity region 11a ber and processing the surface of the GeSbTe thin film with may function as a source, and the second impurity region hydrogen plasma. 11b may function as a drain. 0014) Another example embodiment of the present 0008 Referring to FIG. 1, an insulating layer 15 may be invention is directed to a method of fabricating a thin film, formed on the first impurity region 11a, the gate electrode including injecting at least one precursor into a reactor layer 13 and the second impurity region 11b. A contact plug chamber and depositing the at least one precursor onto a 14 may penetrate the insulating layer 15 to contact the Substrate within the reactor chamber using a chemical vapor second impurity region 11b. A lower electrode 16 may be deposition process so as to form the thin film. mounted on the contact plug 14. A phase-change film 17 and an upper electrode 18 may be formed on the lower electrode BRIEF DESCRIPTION OF THE DRAWINGS 16. 0015 The accompanying drawings are included to pro 0009. A conventional process for storing data in the vide a further understanding of the invention, and are PRAM 100 of FIG. 100 will now be described. Heat, which incorporated in and constitute a part of this specification. may be measured in Joules, may be generated in an area The drawings illustrate example embodiments of the present where the phase-change film 17 contacts the lower electrode invention and, together with the description, serve to explain 16 due to a current Supplied through the second impurity principles of the present invention. US 2006/0172083 A1 Aug. 3, 2006 0016 FIG. 1 illustrates a cross-sectional view of a con ing as commonly understood by one of ordinary skill in the ventional phase-change random access memory (PRAM). art to which this invention belongs. It will be further understood that terms, such as those defined in commonly 0017 FIGS. 2A through 2D are schematic diagrams used dictionaries, should be interpreted as having a meaning illustrating a process of fabricating a thin film according to that is consistent with their meaning in the context of the an example embodiment of the present invention. relevant art and will not be interpreted in an idealized or DETAILED DESCRIPTION OF EXAMPLE overly formal sense unless expressly so defined herein. EMBODIMENTS OF THE PRESENT 0024 FIGS. 2A through 2D are schematic diagrams INVENTION illustrating a process of fabricating a thin film according to 0018 Detailed illustrative example embodiments of the present invention are disclosed herein. However, specific an example embodiment of the present invention. structural and functional details disclosed herein are merely 0025. In the example embodiment of FIG. 2A, a first representative for purposes of describing example embodi precursor including germanium (Ge), a second precursor ments of the present invention. Example embodiments of the including antimony (Sb), and a third precursor including present invention may, however, be embodied in many tellurium (Te) may be prepared. In an example, the first, alternate forms and should not be construed as limited to the second, and third precursors may include GeN(CH), embodiments set forth herein. SbN(CH), and Te(CH) CH, respectively. The first, 0.019 Accordingly, while example embodiments of the second, and third precursors may be injected into a reaction invention are susceptible to various modifications and alter chamber (e.g., sequentially injected one after the other, native forms, specific embodiments thereof are shown by simultaneously or concurrently injected, etc.) and may be way of example in the drawings and will herein be described chemically deposited on a surface of the substrate 20 of the in detail.
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]
  • 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]
  • 1/17 This Manuscript Was Published In: Nature Materials, Volume
    This manuscript was published in: Nature Materials, volume 17, pages 681–685 (2018) Link to published article: https://www.nature.com/articles/s41563-018-0110-9 DOI: 10.1038/s41563-018-0110-9 SharedIt link to access a view-only version of the article for free: https://rdcu.be/bhNaG This file also includes the supplementary information that accompanied the manuscript. Title: Monatomic phase change memory Authors: Martin Salinga*1,2, Benedikt Kersting1,2, Ider Ronneberger1,2, Vara Prasad Jonnalagadda1, Xuan Thang Vu2, Manuel Le Gallo1, Iason Giannopoulos1, Oana Cojocaru-Mirédin2, Riccardo Mazzarello2, Abu Sebastian1 1 IBM Research-Zurich, CH-8803 Rüschlikon, Switzerland 2 RWTH Aachen University, D-52074 Aachen, Germany Phase Change Memory (PCM) has been developed into a mature technology capable of storing information in a fast and non-volatile way1-3, with potential for neuromorphic computing applications4-6. However, its future impact in electronics depends crucially on how the materials at the core of this technology adapt to the requirements arising from continued scaling towards higher device densities. A common strategy to fine-tune the properties of PCM materials, reaching reasonable thermal stability in optical data storage, relies on mixing precise amounts of different dopants, resulting often in quaternary or even more complicated compounds6-8. Here we show how the simplest material imaginable, a single element (in this case antimony), can become a valid alternative when confined in extremely small volumes. This compositional simplification eliminates problems related to unwanted deviations from the optimized stoichiometry in the switching volume, which become increasingly pressing when devices are aggressively miniaturized9,10.
    [Show full text]