Chemical Vapour Deposition

Total Page:16

File Type:pdf, Size:1020Kb

Chemical Vapour Deposition PRIMER Chemical vapour deposition Luzhao Sun 1,2, Guowen Yuan3, Libo Gao3 ✉ , Jieun Yang4, Manish Chhowalla4 ✉ , Meysam Heydari Gharahcheshmeh 5, Karen K. Gleason5 ✉ , Yong Seok Choi6,7,8, Byung Hee Hong6,7,8 ✉ and Zhongfan Liu 1,2 ✉ Abstract | Chemical vapour deposition (CVD) is a powerful technology for producing high-quality solid thin films and coatings. Although widely used in modern industries, it is continuously being developed as it is adapted to new materials. Today, CVD synthesis is being pushed to new heights with the precise manufacturing of both inorganic thin films of 2D materials and high-purity polymeric thin films that can be conformally deposited on various substrates. In this Primer, an overview of the CVD technique, including instrument construction, process control, material characterization and reproducibility issues, is provided. By taking graphene, 2D transition metal dichalcogenides (TMDs) and polymeric thin films as typical examples, the best practices for experimentation involving substrate pretreatment, high-temperature growth and post-growth processes are presented. Recent advances and scaling-up challenges are also highlighted. By analysing current limitations and optimizations, we also provide insight into possible future directions for the method, including reactor design for high-throughput and low-temperature growth of thin films. Chemical vapour deposition (CVD) is a widely used reactions or diffuse directly through the boundary layer materials processing technology in which thin films to the substrate. In both cases, the reactant gases and the are formed on a heated substrate via a chemical reac- intermediate reactants adsorb onto the heated substrate tion of gas-phase precursors. In contrast to physical surface and diffuse on the surface. The subsequent heter- vapour deposition methods, such as evaporation and ogeneous reactions at the gas–solid interface lead to con- sputtering, CVD offers a clear advantage by relying on tinuous thin film formation via nucleation, growth and chemical reactions that enable tunable deposition rates coalescence as well as formation of reaction by-products. as well as high-quality products with excellent confor- Finally, any gaseous products and unreacted species desorb mality. The greater demand for semiconductor thin films from the surface and are carried away from the reaction starting after World War II was the initial driving force zone. The gas-phase reactions occur when the tempera- for rapid development of CVD technology1–5. Recently, ture is sufficiently high or additional energy is introduced, low-dimensional materials such as carbon nanotubes, for example, in the form of plasma. In addition, the het- graphene and 2D transition metal dichalcogenides erogeneous reaction is essential if the deposition reaction (TMDs) have injected new vitality into the electronics relies on the surface catalysis of the underlying substrate, industry6–8 and introduced more stringent requirements such as in the case of the catalytic growth of graphene on for successful CVD of these materials with high purity a metal surface. and fine structure. CVD allows the tuning of the struc- In this Primer, we first provide an overview of the tures and properties of the resulting products9,10, and var- CVD instrumentation set-up before describing best ious advanced CVD systems and their variants have been practices for material preparation and characterization. developed, such as plasma-enhanced CVD2 and metal– The growth of graphene on metal and dielectric sub- organic CVD (MOCVD)4 (BOx 1). Usually, CVD does not strates are taken as representative examples of catalytic require high-vacuum working environments, making it CVD and non-catalytic CVD processes, respectively. a popular technology for electronics, optoelectronics, We then demonstrate the flexibility of this method by surface modification and biomedical applications. discussing important applications of CVD, including ✉e-mail: [email protected]; Irrespective of the variations in CVD types, the fun- growth of binary and ternary 2D materials and poly- [email protected]; damental process is similar and consists of the follow- meric thin films. We also highlight recent progress and [email protected]; 11,12 (Fig. 1) [email protected]; ing common elementary steps . First, the reactant challenges when scaling-up this technology, an impor- [email protected] gases are transported into the reactor. These reactant gases tant aspect of CVD when applied to industry. Finally, https://doi.org/10.1038/ then either undergo gas-phase reactions to form interme- we discuss what affects experimental reproducibility, s43586-020-00005-y diate reactants and gaseous by-products via homogeneous the current limitations of the technique and future NATURE REVIEWS | METHODS PRIMERS | Article citation I­D: (2021) 1:5 1 0123456789(); PRIMER Author addresses Mass flow controllers are essential for the gas supply, where the gas flow rate is automatically set via feedback 1 Center for Nanochemistry, Beijing Science and Engineering Center for Nanocarbons, control according to the mass of flowing gas. Liquid Beijing National Laboratory for Molecular Sciences, College of Chemistry and Molecular source reactants are delivered by ‘bubbling’ a carrier gas Engineering, Peking University, Beijing, China. controlled by the mass flow controller13,14 (Fig. 2b). Solid 2Beijing Graphene Institute, Beijing, China. 3National Laboratory of Solid State Microstructures, School of Physics, Collaborative source precursors that are less volatile are introduced Innovation Center of Advanced Microstructures, Nanjing University, Nanjing, China. to the reaction chamber by dissolution in a suitable 15 16–22 4Department of Materials Science and Metallurgy, University of Cambridge, solvent or by sublimation into the gas phase . Cambridge, UK. 5Department of Chemical Engineering, Massachusetts Institute of Technology, Reaction chamber. The horizontal23,24 (Fig. 2a) and verti- Cambridge, MA, USA. cal25,26 (Fig. 2c–e) configurations are the two main config- 6Graphene Research Center, Advanced Institute of Convergence Technology, urations of the reaction chamber (BOX 1). The reaction Suwon, Korea. chamber itself is usually a quartz tube, widely employed 7 Department of Chemistry, Seoul National University, Seoul, Korea. in semiconductor manufacturing because of its tolerance 8Graphene Square Inc., Suwon, Korea. to high temperatures and to rapid heating and cooling. A gas inlet injector is connected to the chamber using a developments of CVD together with exploration of metal flange, which is fitted with cooling components. new materials. To guarantee that the gas flow is laminar, a gas distribu- tor with through-holes is usually employed23,25 (FIG. 2c–e). Experimentation The substrate is usually located on a substrate holder To obtain high-quality thin films by CVD, suitable (also known as a ‘boat’ or ‘susceptor’) composed of quartz equipment is needed, and custom-built systems pro- or graphite because of their good chemical stability and vide the flexibility of operation often desired by CVD high-temperature resistance23,27,28. In order to meet the researchers. In this section, we discuss a series of designs target deposition characteristics (thickness, composition that satisfy the requirements of materials synthesis, and so on),the configuration of the substrate holder and including the heating methods, gas-flow control, the the deposition conditions (total gas flow, gas composi- loading of substrate and so on. In addition, the growth tion, temperature, pressure and so on) must be optimized parameters, including substrate, temperature, atmos- via experimental and numerical process engineering phere, pressure and so on, are essential for controlling studies23,25,26,29,30. In manufacturing applications, a cool- the quality of as-grown materials as well as the reaction ing chamber with a loading/unloading subsystem is rate (growth rate). Here, we will introduce CVD growth necessary to improve the productivity. of graphene following the procedure of substrate pre- treatment, heating, annealing, high-temperature growth Vacuum system. Purging the deposition chamber to and cooling. start the deposition process and obtaining the neces- sary pressure for transport of the reactants relies on the CVD equipment vacuum system, where measurement and control of A CVD system must meet the following basic require- the vacuum are essential and complement one another. ments: delivery of the gas-phase reactants in a control- To measure the pressure of the vacuum system, various lable manner; provision of a sealed reaction chamber; gauges are alternated: the Bourdon gauge, piezo sensor, evacuation of the gases and control of the reaction capacitance manometer and diaphragm manometer are pressure; supply of the energy source for the chemical the main mechanical gauges, which can measure the reactions; treatment of the exhaust gases to obtain safe vacuum by detecting physical changes in the strain or and harmless levels; and automatic process control to electrical capacitance, for example. The Bourdon gauge improve the stability of the deposition process. Figure 2 is inexpensive and has a long life, but it does not have shows a typical CVD system consisting of a gas deliv- an electronic output, and so is not suitable for feed- ery system, a reaction chamber, a vacuum system, an back control (Fig. 2f). Using a capacitance manometer, a energy system, an exhaust gas treatment system and measurement range of
Recommended publications
  • Synthesis, Structure and Properties of Metal Oxychalcogenides
    Durham E-Theses Synthesis, Structure and Properties of Metal Oxychalcogenides TUXWORTH, ANDREW,JAMES How to cite: TUXWORTH, ANDREW,JAMES (2014) Synthesis, Structure and Properties of Metal Oxychalcogenides, Durham theses, Durham University. Available at Durham E-Theses Online: http://etheses.dur.ac.uk/9497/ Use policy The full-text may be used and/or reproduced, and given to third parties in any format or medium, without prior permission or charge, for personal research or study, educational, or not-for-prot purposes provided that: • a full bibliographic reference is made to the original source • a link is made to the metadata record in Durham E-Theses • the full-text is not changed in any way The full-text must not be sold in any format or medium without the formal permission of the copyright holders. Please consult the full Durham E-Theses policy for further details. Academic Support Oce, Durham University, University Oce, Old Elvet, Durham DH1 3HP e-mail: [email protected] Tel: +44 0191 334 6107 http://etheses.dur.ac.uk Abstract “Synthesis, Structure and Properties of Metal Oxychalcogenides” PhD Thesis Andrew J. Tuxworth December 2013 Chapter 1 gives a brief review of oxychalcogenide materials and their properties, with particular focus on structures similar to the systems discussed in the later chapters. These oxychalcogenides, are of interest due to their potentially interesting magnetic and electronic properties. Chapter 2 discusses the synthetic methods and characterisation techniques used throughout this thesis. The theory behind both single crystal and powder diffraction techniques used in this work is described. Chapter 3 describes the synthesis of a new ZrCuSiAs-related transition metal containing oxychalcogenide La2O2ZnSe2.
    [Show full text]
  • Curriculum Vitae Mercouri G
    CURRICULUM VITAE MERCOURI G. KANATZIDIS Department of Chemistry, Northwestern University, Evanston, IL 60208 Phone 847-467-1541; Fax 847-491-5937; Website: http://chemgroups.northwestern.edu/kanatzidis/ Birth Date: 1957; Citizenship: US EXPERIENCE 8/06-Present: Professor of Chemistry, Northwestern University and Senior Scientist , Argonne National Laboratory, Materials Science Division, Argonne, IL 7/93-8/06: Professor of Chemistry, Michigan State University 7/91-6/93: Associate Professor, Michigan State University 7/87-6/91: Assistant Professor, Michigan State University EDUCATION Postdoctoral Fellow, 1987, Northwestern University Postdoctoral Associate, 1985, University of Michigan Ph.D. Inorganic Chemistry, 1984, University of Iowa B.S. Chemistry, November 1979, Aristotle University of Thessaloniki AWARDS • Presidential Young Investigator Award, National Science Foundation, 1989-1994 • ACS Inorganic Chemistry Division Award, EXXON Faculty Fellowship in Solid State Chemistry, 1990 • Beckman Young Investigator , 1992-1994 • Alfred P. Sloan Fellow, 1991-1993 • Camille and Henry Dreyfus Teacher Scholar, 1993-1998 • Michigan State University Distinguished Faculty Award, 1998 • Sigma Xi 2000 Senior Meritorious Faculty Award • University Distinguished Professor MSU, 2001 • John Simon Guggenheim Foundation Fellow, 2002 • Alexander von Humboldt Prize, 2003 • Morley Medal, American Chemical Society, Cleveland Section, 2003 • Charles E. and Emma H. Morrison Professor, Northwestern University, 2006 • MRS Fellow, Materials Research Society, 2010 • AAAS Fellow, American Association for the Advancment of Science, 2012 • Chetham Lecturer Award, University of California Santa Barbara, 2013 • Einstein Professor, Chinese Academy of Sciences, 2014 • International Thermoelectric Society Outstanding Achievement Award 2014 • MRS Medal 2014 • Royal Chemical Society DeGennes Prize 2015 • Elected Fellow of the Royal Chemical Society 2015 • ENI Award for the "Renewable Energy Prize" category • ACS Award in Inorganic Chemistry 2016 • American Physical Society 2016 James C.
    [Show full text]
  • Layered Oxychalcogenides: Structural Chemistry and Thermoelectric Properties
    CORE Metadata, citation and similar papers at core.ac.uk Provided by Elsevier - Publisher Connector Available online at www.sciencedirect.com ScienceDirect J Materiomics 2 (2016) 131e140 www.ceramsoc.com/en/ www.journals.elsevier.com/journal-of-materiomics/ Layered oxychalcogenides: Structural chemistry and thermoelectric properties Son D.N. Luu a,b, Paz Vaqueiro b,* a Institute of Chemical Sciences, Heriot-Watt University, Edinburgh, EH14 4AS, UK b Department of Chemistry, University of Reading, Whiteknights, Reading, RG6 6AD, UK Received 16 February 2016; revised 18 March 2016; accepted 3 April 2016 Available online 8 April 2016 Abstract Layered oxychalcogenides have recently emerged as promising thermoelectric materials. The alternation of ionic oxide and covalent chalcogenide layers found in these materials often results in interesting electronic properties, and also facilitates the tuning of their properties via chemical substitution at both types of layers. This review highlights some common structure types found for layered oxychalcogenides and their interrelationships. This review pays special attention to the potential of these materials for thermoelectric applications, and provides an overview of the thermoelectric properties of materials of current interest, including BiCuSeO. © 2016 The Chinese Ceramic Society. Production and hosting by Elsevier B.V. This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/). Keywords: Oxychalcogenides; Layered structures; Thermoelectric;
    [Show full text]
  • Layered Oxychalcogenides: Structural Chemistry and Thermoelectric Properties
    Layered oxychalcogenides: structural chemistry and thermoelectric properties Article Accepted Version Creative Commons: Attribution-Noncommercial-No Derivative Works 4.0 Luu, S. D. N. and Vaqueiro, P. (2016) Layered oxychalcogenides: structural chemistry and thermoelectric properties. Journal of Materiomics, 2 (2). pp. 131-140. ISSN 2352-8478 doi: https://doi.org/10.1016/j.jmat.2016.04.002 Available at http://centaur.reading.ac.uk/62768/ It is advisable to refer to the publisher’s version if you intend to cite from the work. See Guidance on citing . To link to this article DOI: http://dx.doi.org/10.1016/j.jmat.2016.04.002 Publisher: Elsevier All outputs in CentAUR are protected by Intellectual Property Rights law, including copyright law. Copyright and IPR is retained by the creators or other copyright holders. Terms and conditions for use of this material are defined in the End User Agreement . www.reading.ac.uk/centaur CentAUR Central Archive at the University of Reading Reading’s research outputs online Layered oxychalcogenides: structural chemistry and thermoelectric properties Son D N Luu1,2, Paz Vaqueiro2* 1Institute of Chemical Sciences, Heriot-Watt University, Edinburgh, EH14, 4AS, UK 2Department of Chemistry, University of Reading, Whiteknights, Reading, RG6 6AD, UK Abstract Layered oxychalcogenides have recently emerged as promising thermoelectric materials. The alternation of ionic oxide and covalent chalcogenide layers found in these materials often results in interesting electronic properties, and also facilitates the tuning of their properties via chemical substitution at both types of layers. This review highlights some common structure types found for layered oxychalcogenides and their interrelationships. This review pays special attention to the potential of these materials for thermoelectric applications, and provides an overview of the thermoelectric properties of materials of current interest, including BiCuSeO.
    [Show full text]
  • Download Article (PDF)
    Z. Kristallogr. 226 (2011) 435–446 / DOI 10.1524/zkri.2011.1363 435 # by Oldenbourg Wissenschaftsverlag, Mu¨nchen Structural chemistry of superconducting pnictides and pnictide oxides with layered structures Dirk JohrendtI, Hideo HosonoII, Rolf-Dieter HoffmannIII and Rainer Po¨ttgen*, III I Department Chemie und Biochemie, Ludwig-Maximilians-Universita¨t Mu¨nchen, Butenandtstraße 5–13 (Haus D), 81377 Mu¨nchen, Germany II Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan III Institut fu¨r Anorganische und Analytische Chemie, Universita¨t Mu¨nster, Corrensstraße 30, 48149 Mu¨nster, Germany Received October 29, 2010; accepted February 6, 2011 Pnictide / Pnictide oxide / Superconductivity / for hydride formation of CeRuSi ! CeRuSiH [6] and Intermetallics / Group-subgroup relation CeRuGe ! CeRuGeH [7]. The crystal chemical data of the huge number of ZrCuSiAs materials have recently Abstract. The basic structural chemistry of supercon- been reviewed [8]. ducting pnictides and pnictide oxides is reviewed. Crystal Although the basic crystallographic data of the many chemical details of selected compounds and group sub- ThCr2Si2 and ZrCuSiAs type compounds are known for group schemes are discussed with respect to phase transi- several years, especially for the ZrCuSiAs family, systema- tions upon charge-density formation, the ordering of va- tic property studies have been performed only recently. cancies, or the ordered displacements of oxygen atoms. These investigations mainly focused on p-type transparent Furthermore, the influences of doping and solid solutions semiconductors like LaCuSO (for a review see [9]) or the on the valence electron concentration are discussed in or- colored phosphide and arsenide oxides REZnPO [10] and der to highlight the structural and electronic flexibility of REZnAsO [11].
    [Show full text]
  • IONIZATION ENERGIES of GAS-PHASE MOLECULES Sharon G
    IONIZATION ENERGIES OF GAS-PHASE MOLECULES Sharon G. Lias This table presents values for the first ionization energies (IP) of approximately 1000 molecules and atoms. Substances are listed by molecular formula in the modified Hill order (see introduction). Values enclosed in parentheses are considered not to be well established. Data appearing in the 1988 reference, were updated in 1996 for inclusion in the database of ionization energies available at the Internet site of the Standard Reference Data program of the National Institute of Standards and Technology (http://webbook.nist.gov). The list appearing here includes these updates. ∆ The list also includes values for enthalpies of formation of the ions at 298 K, fHion, given according to the ion convention used by mass ∆ spectrometrists; to convert these values to the electron convention used by thermodynamicists, add 6 kJ/mol. Details on the calculation of fHion as well as data for a much larger number of molecules, may be found in the reference and on the Internet site. REFERENCE Lias, S.G., Bartmess, J.E., Liebman, J.F., Holmes, J.L., Levin, R.D., and Mallard, W.G., Gas-Phase Ion and Neutral Thermochemistry, J. Phys. Chem. Ref. Data, Vol. 17, Suppl. No. 1, 1988. ∆ Mol. f Hion Form. Name IP/eV kJ/mol Substances not containing carbon Ac Actinium 5.17 905 Ag Silver 7.57624 1016 AgCl Silver(I) chloride (≤ 10.08) ≤ 1065 AgF Silver(I) fluoride (11.0 ± 0.3) 1071 Al Aluminum 5.98577 905 AlBr Aluminum monobromide (9.3) 913 AlBr3 Aluminum tribromide (10.4) 593 AlCl Aluminum monochloride 9.4
    [Show full text]
  • Aleksi Matikainen MIXED-ANION COMPOUNDS
    Aleksi Matikainen MIXED-ANION COMPOUNDS: AN UNEXPLORED ALD PLAYGROUND FOR APPLICATIONS Master´s Programme in Chemical, Biochemical and Materials Engineering Major in Chemistry Master’s thesis for the degree of Master of Science in Technology submitted for inspection, Espoo, 9 July, 2018. Supervisor Professor Maarit Karppinen Instructor Ph. D. Tripurari Sharan Tripathi Aalto University, P.O. BOX 11000, 00076 AALTO www.aalto.fi Abstract of master's thesis Author Aleksi Matikainen Title of thesis Mixed-anion compounds: An unexplored ALD playground for applications Degree Programme Master’s programme in Chemical, Biochemical and Materials Engineering Major Chemistry Thesis supervisor Professor Maarit Karppinen Thesis advisor(s) / Thesis examiner(s) PhD Tripurari Sharan Tripathi Date 09.07.2018 Number of pages 89 Language English Abstract Mixed-anion compounds, such as oxypnictides and oxychalcogenides, are an emerging research subject as functional solid-state materials. Their structures are more complex compared with traditional oxides, which provides novel building blocks for new functional materials. Potential applications include transparent electronics, photovoltaics and thermoelectrics. Atomic layer deposition (ALD) is a possible solution for fabricating mixed-anion thin films with superior properties to bulk mixed-anion compounds. Oxysulfides are an interesting group of mixed-anion compounds with desirable electrical properties and an inexpensive and non-toxic composition of earth-abundant elements. Their layered structure induces several intriguing properties such as superconductivity, transparent p-type semiconductivity and wide band gap. Only a few oxysulfides have been fabricated with ALD before. In this work, a novel atomic layer deposition process for fabricating oxysulfide LaOCuS (lanthanum oxide copper sulfide) thin films was implemented.
    [Show full text]
  • Design and Synthesis of Perovskites and Corundum Derivatives with Unusual Magnetic, Electronic, and Structural Coupling
    © 2021 Corey Frank ALL RIGHTS RESERVED DESIGN AND SYNTHESIS OF PEROVSKITES AND CORUNDUM DERIVATIVES WITH UNUSUAL MAGNETIC, ELECTRONIC, AND STRUCTURAL COUPLING By Corey Elizabeth Frank A dissertation submitted to the School of Graduate Studies Rutgers, The State University of New Jersey in partial fulfillment of the requirements for the degree of Doctor of Philosophy Graduate Program in Chemistry Written under the direction of Professor Martha Greenblatt and approved by ______________________________ ______________________________ ______________________________ ______________________________ New Brunswick, NJ January 2021 ABSTRACT OF THE DISSERTATION Design and Synthesis of Perovskites and Corundum Derivatives with Unusual Magnetic, Electronic, and Structural Coupling By Corey Elizabeth Frank Dissertation Director: Martha Greenblatt ABO3 perovskites and derivative structures are versatile materials, critical to the function of modern life, and the discovery of new perovskites is essential to developing the fields of photovoltaics, microelectronics, and telecommunication (푟 +푟 ) among others. The Goldschmidt tolerance factor (푡 = 퐴 푥 ) has been used for √2(푟퐵+푟푥) years to qualitatively predict stable perovskites; this formula predicts that with small A-cations (effective ionic radius < 0.9 Å) and B transition metal B-cations the perovskite structure will not form. With careful synthesis techniques, and the application of high pressure, this limitation can be overcome, unlocking distorted materials with interesting electronic-magnetic-structural coupling behaviors. These materials include highly distorted transition metal only double perovskites, such as Mn2CoReO6; quadruple perovskites with a square-planar coordinated A’ cation, such as La3Mn4RhO12; and even double corundum derivatives which feature face-sharing dimers of octahedrally coordinated A and B cations, such as Fe3-xInSnxO6 (x = 0, 0.25, 0.5) and In2Mn1.1Sn0.9O6.
    [Show full text]
  • Arxiv:1704.01441V1 [Cond-Mat.Str-El] 5 Apr 2017 Tronic, Magnetic, and Structural Properties They Possess
    The magnetic and electronic properties of Oxyselenides - influence of transition metal ions and lanthanides C. Stock1 and E. E. McCabe2 1School of Physics and Astronomy, University of Edinburgh, Edinburgh EH9 3FD, UK 2School of Physical Sciences, University of Kent, Canterbury, CT2 7NH, UK (Dated: October 15, 2018) Magnetic oxyselenides have been a topic of research for several decades, firstly in the context of photoconductivity and thermoelectricity owing to their intrinsic semiconduct- ing properties and ability to tune the energy gap through metal ion substitution. More recently, interest in the oxyselenides has experienced a resurgence owing to the possible relation to strongly correlated phenomena given the fact that many oxyselenides share a similar structure to unconventional superconducting pnictides and chalcogenides. The two dimensional nature of many oxyselenide systems also draws an analogy to cuprate physics where a strong interplay between unconventional electronic phases and localised magnetism has been studied for several decades. It is therefore timely to review the physics of the oxyselenides in the context of the broader field of strongly correlated magnetism and electronic phenomena. Here we review the current status and progress in this area of research with the focus on the influence of lanthanides and transition metal ions on the intertwined magnetic and electronic properties of oxyselenides. The emphasis of the review is on the magnetic properties and comparisons are made with iron based pnictide and chalcogenide systems. CONTENTS 8. Summary of the magnetic structure variation with transition metal ion 21 I. Introduction 1 E. Magnetic interactions 22 1. La2O2Fe2OSe2 and Ce2O2FeSe2 22 2+ 2+ II. Experimental techniques 2 2.
    [Show full text]
  • Two-Dimensional Oxides: Recent Progress in Nanosheets
    Z. Phys. Chem. 2019; 233(1): 117–165 Review Richard Hinterding* and Armin Feldhoff Two-Dimensional Oxides: Recent Progress in Nanosheets A Retrospection on Synthesis, Microstructure and Applications https://doi.org/10.1515/zpch-2018-1125 Received January 26, 2018; accepted February 27, 2018 Abstract: Two-dimensional (2D) materials have been widely investigated for the last few years, introducing nanosheets and ultrathin films. The often superior electrical, optical and mechanical properties in contrast to their three-dimen- sional (3D) bulk counterparts offer a promising field of opportunities. Especially new research fields for already existing and novel applications are opened by downsizing and improving the materials at the same time. Some of the most promising application fields are namely supercapacitors, electrochromic devices, (bio-) chemical sensors, photovoltaic devices, thermoelectrics, (photo-) catalysts and membranes. The role of oxides in this field of materials deserves a closer look due to their availability, durability and further advantages. Here, recent progress in oxidic nanosheets is highlighted and the benefit of 2D oxides for applications discussed in-depth. Therefore, different synthesis techniques and micro structures are compared more closely. Keywords: nanosheet; oxide; thermoelectric; two-dimensional; ultrathin film. 1 Introduction With the enablement of measuring functional properties of two-dimensional (2D) graphene sheets and the discovery of electrons being able to behave like Dirac-type fermions without restmass [1], new interest in 2D materials was awaken. Actual research considers all elements of the periodic table and their *Corresponding author: Richard Hinterding, Leibniz University Hannover, Institute of Physical Chemistry and Electrochemistry, Callinstraße 3A, D-30176 Hannover, Germany, e-mail: [email protected] Armin Feldhoff: Leibniz University Hannover, Institute of Physical Chemistry and Electrochemistry, Callinstraße 3A, D-30176 Hannover, Germany 118 R.
    [Show full text]
  • GW100: Benchmarking G0W0 for Molecular Systems
    GW 100: Benchmarking G0W0 for molecular systems Michiel J. van Setten,∗,y,z Fabio Caruso,{,x Sahar Sharifzadeh,k Xinguo Ren,#,@ Matthias Scheffler,@ Fang Liu,4 Johannes Lischner,r, Lin Lin, Jack R. Deslippe, Steven G. Louie,,r Chao Yang, Florian Weigend,, Jeffey B. Neaton, Ferdinand Evers, and Patrick Rinke,@ Nanoscopic Physics, Institute of Condensed Matter and Nanosciences, Université Catholique de Louvain, Louvain-la-Neuve, 1348, Belgium, Institute of Nanotechnology, Karlsruhe Institute of Technology Campus North, Karlsruhe, 76344 Germany, Fritz-Haber-Institut der Max-Planck-Gesellschaft, Berlin, 4195, Germany, Department of Materials, University of Oxford, Oxford, OX1 3PH, United Kingdom, Molecular Foundry, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA, Department of Electrical and Computer Engineering, Boston University, Boston, MA 02215, USA, Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, 230026, China, Fritz-Haber-Institut der Max-Planck-Gesellschaft, Berlin, 14195, Germany, School of Applied Mathematics, Central University of Finance and Economics, Beijing, Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA, Department of Physics, University of California, Berkeley, CA 94720, USA, Computational Research Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA, National Energy Research Scientific Computing Center, Berkeley, CA 94720, USA, Department of Physics, University of California, Berkeley, CA 94720, USA , Institute of Nanotechnology, Karlsruhe Institute of Technology Campus North, Karlsruhe, 76344, Germany, Institute of Theoretical Physics, University of Regensburg, Regensburg, 93040, Germany, and COMP/Department of Applied Physics, Aalto University School of Science, Aalto, 00076, Finland E-mail: [email protected] 2 May 16, 2015 Abstract ab initio GW calculations for 100 molecules, a benchmark set we term as GW 100, are presented using three independent codes and using different methods.
    [Show full text]
  • Structure and Physical Properties of New Layered Iron Oxychalcogenide
    Structure and physical properties of new layered iron oxychalcogenide BaFe2OSe2 Hechang Lei,1, Hyejin Ryu,1,2 John Warren,3 A. I. Frenkel,4 V. Ivanovski,5 B. Cekic5 and C. Petrovic1,2 1Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA 2Department of Physics and Astronomy, Stony Brook University, Stony Brook, New York 11794-3800, USA 3Instrumentation Division, Brookhaven National Laboratory, Upton, New York 11973, USA 4Physics Department, Yeshiva University, 245 Lexington Avenue, New York, New York 10016, USA 5Institute of Nuclear Sciences Vinca, University of Belgrade, Belgrade 11001, Serbia (Dated: June 8, 2018) We have successfully synthesized a new layered iron oxychalcogenide BaFe2OSe2 single crystal. This compound is built up of Ba and Fe-Se(O) layers alternatively stacked along the c-axis. The Fe-Se(O) layers contain double chains of edge-shared Fe-Se(O) tetrahedra that propagate along the b-axis and are bridged by oxygen along the a-axis. Physical property measurements indicate that BaFe2OSe2 is a semiconductor without the Curie-Weiss behavior up to 350 K. There is a possible long range antiferromagnetic (AFM) transition at 240 K, corresponding to the peak in specific heat measurement and two glassy transitions at 115 K and 43 K. The magnetic entropy up to 300 K is much smaller than the expected value for Fe2+ in tetrahedral crystal fields and M¨osbauer spectrum indicates that long range magnetic order is unlikely at 294 K. Both results suggest that a short range magnetic correlations exist above the room temperature. PACS numbers: 75.50.Ee, 75.10.Pq, 75.30.Gw, 75.47.Np 2− I.
    [Show full text]