Feasibility Studies of the Growth of Ill-V Compounds of Boron by MOCVD
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Chemical Vapor Deposition of Heteroepitaxial Boron Phosphide Thin Films
University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Doctoral Dissertations Graduate School 12-2013 Chemical Vapor Deposition of Heteroepitaxial Boron Phosphide Thin Films John Daniel Brasfield University of Tennessee - Knoxville, [email protected] Follow this and additional works at: https://trace.tennessee.edu/utk_graddiss Part of the Semiconductor and Optical Materials Commons Recommended Citation Brasfield, John Daniel, "Chemical aporV Deposition of Heteroepitaxial Boron Phosphide Thin Films. " PhD diss., University of Tennessee, 2013. https://trace.tennessee.edu/utk_graddiss/2558 This Dissertation is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a dissertation written by John Daniel Brasfield entitled "Chemical Vapor Deposition of Heteroepitaxial Boron Phosphide Thin Films." I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the equirr ements for the degree of Doctor of Philosophy, with a major in Chemistry. Charles S. Feigerle, Major Professor We have read this dissertation and recommend its acceptance: Laurence Miller, Frank Vogt, Ziling Xue Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) Chemical Vapor Deposition of Heteroepitaxial Boron Phosphide Thin Films A Dissertation Presented for the Doctor of Philosophy Degree The University of Tennessee, Knoxville John Daniel Brasfield December 2013 Copyright © 2013 by John Daniel Brasfield All rights reserved. -
Pyrophoric Materials
Appendix A PYROPHORIC MATERIALS Pyrophoric materials react with air, or with moisture in air. Typical reactions which occur are oxidation and hydrolysis, and the heat generated by the reactions may ignite the chemical. In some cases, these reactions liberate flammable gases which makes ignition a certainty and explosion a real possibility. Examples of pyrophoric materials are shown below. (List may not be complete) (a) Pyrophoric alkyl metals and derivatives Groups Dodecacarbonyltetracobalt Silver sulphide Dialkytzincs Dodecacarbonyltriiron Sodium disulphide Diplumbanes Hexacarbonylchromium Sodium polysulphide Trialkylaluminiums Hexacarbonylmolybdenum Sodium sulphide Trialkylbismuths Hexacarbonyltungsten Tin (II) sulphide Nonacarbonyldiiron Tin (IV) sulphide Compounds Octacarbonyldicobalt Titanium (IV) sulphide Bis-dimethylstibinyl oxide Pentacarbonyliron Uranium (IV) sulphide Bis(dimethylthallium) acetylide Tetracarbonylnickel Butyllithium (e) Pyrophoric alkyl non-metals Diethylberyllium (c) Pyrophoric metals (finely divided state) Bis-(dibutylborino) acetylene Bis-dimethylarsinyl oxide Diethylcadmium Caesium Rubidium Bis-dimethylarsinyl sulphide Diethylmagnesium Calcium Sodium Bis-trimethylsilyl oxide Diethylzinc Cerium Tantalum Dibutyl-3-methyl-3-buten-1-Yniborane Diisopropylberyllium Chromium Thorium Diethoxydimethylsilane Dimethylberyllium Cobalt Titanium Diethylmethylphosphine Dimethylbismuth chloride Hafnium Uranium Ethyldimthylphosphine Dimethylcadmium Iridium Zirconium Tetraethyldiarsine Dimethylmagnesium Iron Tetramethyldiarsine -
Download The
COORDINATION COMPOUNDS OF ALKYL GALLIUM HYDRIDES by VICTOR GRAHAM WIEBE B.Sc. (Hons.) University of British Columbia 1966 A THESIS SUBMITTED IN PARTIAL FULFILMENT OF THE REQUIREMENTS FOR THE DEGREE OF MASTER OF SCIENCE In The Department of Chemistry We accept this thesis as conforming to the required standard The University of British Columbia June 1968 In presenting this thesis in partial fulfilment of the requirements for an advanced degree at the University of British Columbia, I agree that the Library shall make it freely available for reference and Study. I further agree that permission for extensive copying of this thesis for scholarly purposes may be granted by the Head of my Department or by hits representatives. It is understood that copying or publication of this thesis for financial gain shall not be allowed without my written permission. Department of The University of British Columbia Vancouver 8, Canada - ii - Abstract Although the organo hydride derivatives of boron and aluminum are well characterized^little work has been reported on the corresponding gallium systems. The present study was initiated to determine the relative stabilities and reactivity of organo gallium hydride derivatives as compared with the stabilities and reactions of the corresponding compounds of boron and aluminum. Various preparative routes to this new class of gallium compounds have been investigated. These include the use of organo-mercury, organo-lithium and lithium hydride derivatives in reactions with gallium hydride and gallium alkyl compounds and their halogen substituted derivatives: Me3NGaH3 + HgR2 >- Me3NGaH2R + l/2Hg + 1/2H2 Me3NGaH2Cl + LiR y Me3NGaH2R + LiCl Me3NGaR2Cl + LiH • Me3NGaHR2 + LiCl A fourth preparative method involves disproportionation reactions between gallium hydride compounds and organo gallium compounds to yield the mixed organo hydride derivatives. -
Guidelines for Pyrophoric Materials
Guidelines for Pyrophoric Materials Definition and Hazards Pyrophoric materials are substances that ignite instantly upon exposure to air, moisture in the air, oxygen or water. Other common hazards include corrosivity, teratogenicity, and organic peroxide formation, along with damage to the liver, kidneys, and central nervous system. Examples include metal hydrides, finely divided metal powders, nonmetal hydride and alkyl compounds, white phosphorus, alloys of reactive materials and organometallic compounds, including alkylithiums. Additional pyrophoric materials are listed in Appendix A. Failure to follow proper handling techniques could result in serious injury or death. Controlling the Hazards . If possible, use safer chemical alternatives. A “dry run” of the experiment should be performed using low-hazard materials, such as water or solvent, as appropriate. Limit the amount purchased and the amount stored. Do not accumulate unneeded pyrophoric materials. BEFORE working with pyrophoric materials, read the MSDS sheets. The MSDS must be reviewed before using an unfamiliar chemical and periodically as a reminder. A Standard Operating Procedure (SOP) should be prepared and reviewed for each process involving pyrophoric materials. In lab training should be completed and documented. If possible, use the “buddy system”. Working alone with pyrophorics is strongly discouraged. All glassware used for pyrophorics should be oven-dried and free of moisture. Review the location of the safety shower, eyewash, telephone, and fire extinguisher. Keep an appropriate fire extinguisher or extinguishing material close at hand. Additional controls when handling liquid pyrophoric materials . Secure pyrophoric reagent bottle to stand. Secure the syringe so if the plunger blows out of the body of the syringe the contents will not splash anyone. -
Chemical Names and CAS Numbers Final
Chemical Abstract Chemical Formula Chemical Name Service (CAS) Number C3H8O 1‐propanol C4H7BrO2 2‐bromobutyric acid 80‐58‐0 GeH3COOH 2‐germaacetic acid C4H10 2‐methylpropane 75‐28‐5 C3H8O 2‐propanol 67‐63‐0 C6H10O3 4‐acetylbutyric acid 448671 C4H7BrO2 4‐bromobutyric acid 2623‐87‐2 CH3CHO acetaldehyde CH3CONH2 acetamide C8H9NO2 acetaminophen 103‐90‐2 − C2H3O2 acetate ion − CH3COO acetate ion C2H4O2 acetic acid 64‐19‐7 CH3COOH acetic acid (CH3)2CO acetone CH3COCl acetyl chloride C2H2 acetylene 74‐86‐2 HCCH acetylene C9H8O4 acetylsalicylic acid 50‐78‐2 H2C(CH)CN acrylonitrile C3H7NO2 Ala C3H7NO2 alanine 56‐41‐7 NaAlSi3O3 albite AlSb aluminium antimonide 25152‐52‐7 AlAs aluminium arsenide 22831‐42‐1 AlBO2 aluminium borate 61279‐70‐7 AlBO aluminium boron oxide 12041‐48‐4 AlBr3 aluminium bromide 7727‐15‐3 AlBr3•6H2O aluminium bromide hexahydrate 2149397 AlCl4Cs aluminium caesium tetrachloride 17992‐03‐9 AlCl3 aluminium chloride (anhydrous) 7446‐70‐0 AlCl3•6H2O aluminium chloride hexahydrate 7784‐13‐6 AlClO aluminium chloride oxide 13596‐11‐7 AlB2 aluminium diboride 12041‐50‐8 AlF2 aluminium difluoride 13569‐23‐8 AlF2O aluminium difluoride oxide 38344‐66‐0 AlB12 aluminium dodecaboride 12041‐54‐2 Al2F6 aluminium fluoride 17949‐86‐9 AlF3 aluminium fluoride 7784‐18‐1 Al(CHO2)3 aluminium formate 7360‐53‐4 1 of 75 Chemical Abstract Chemical Formula Chemical Name Service (CAS) Number Al(OH)3 aluminium hydroxide 21645‐51‐2 Al2I6 aluminium iodide 18898‐35‐6 AlI3 aluminium iodide 7784‐23‐8 AlBr aluminium monobromide 22359‐97‐3 AlCl aluminium monochloride -
The Preparation of Organomagnesium Fluorides
THE PREPARATION OF ORGANOMAGNESIUM FLUORIDES BY ORGANOMETALLIC EXCHANGE REACTIONS AND THE COMPOSITION IN SOLUTION OF ALKOXY(METHYL)MAGNESIUM AND DIALKYLAMINO(METHYL)MAGNESIUM COMPOUNDS A THESIS Presented To The Faculty of the Graduate Division by John A. Nackashi In Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy In the School of Chemistry Georgia Institute of Technology May, 1974 THE PREPARATION OF ORGANOMAGNESIUM FLUORIDES BY ORGANOMETALLIC EXCHANGE REACTIONS AND THE COMPOSITION IN SOLUTION OF ALKOXY(METHYL)MAGNESIUM AND DIALKYLAMINO(METHYL)MAGNESIUM COMPOUNDS Approved: E. C. Ashby, Chairman A. Bertrand C. L. Liotta Date approved by Chairman: ii ACKNOWLEDGMENTS The author is grateful to Dr. E. C. Ashby for his guidance, direction and patience during this research. The reading of this thesis by Dr. A. Bertrand and Dr. C. Liotta is greatly appreciated. The author is also indebted to John P. Oliver for his assistance and friendship, and to the mem bers of the research group who made the successes of this research a joy and the failures acceptable. The warm friend ship expressed by the research group will always be cherished. Financial assistance by the Georgia Institute of Tech nology and the National Science Foundation is gratefully ack nowledged. The author acknowledges a special appreciation to his parents and particularly his wife, Bryan. Their gentle en couragement and patient understanding throughout the entire period of study has made this thesis possible. iii TABLE OF CONTENTS Page ACKNOWLEDGMENTS ii LIST OF TABLES vi LIST OF ASSOCIATION PLOTS iii LIST OF SPECTRA ix SUMMARY x PART I THE PREPARATION OF ORGANOMAGNESIUM FLUORIDES BY ORGANOMETALLIC EXCHANGE REACTIONS CHAPTER I. -
Synthesis and Characterization of Diamond and Boron Phosphide
University of Rhode Island DigitalCommons@URI Open Access Dissertations 1972 Synthesis and Characterization of Diamond and Boron Phosphide K. P. Ananthanarayanan University of Rhode Island Follow this and additional works at: https://digitalcommons.uri.edu/oa_diss Recommended Citation Ananthanarayanan, K. P., "Synthesis and Characterization of Diamond and Boron Phosphide" (1972). Open Access Dissertations. Paper 690. https://digitalcommons.uri.edu/oa_diss/690 This Dissertation is brought to you for free and open access by DigitalCommons@URI. It has been accepted for inclusion in Open Access Dissertations by an authorized administrator of DigitalCommons@URI. For more information, please contact [email protected]. T-P 7'i7 3. S ])5 Aisc°' .:. 1 SYNTHESIS AND CHARACTERIZATION OF DIAMOND AND BORON PHOSPHIDE / BY K. P. ANANTHANARAYANAN A THESIS SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY IN CHEMICAL ENGINEERING UNIVERSITY OF RHODE ISLAND 1972 DOCTOR OF PHILOSOPHY THESIS OF K. P. ANANTHANARAYANAN Approved: Thesis Committee: Dean of the Graduate School UNIVERSITY OF RHODE ISLAND 1972 ABSTRACT Semiconducting diamond has been synthesized from carbon-metal melts in a 600 ton tetrahedral anvil press at about 60 kbar and 1400°c. The experimental set up, pressure and temperature calibra- tions, and the growth region in the pressure-temperature regime are indicated. Micrographs of synthesized crystals are shown. The semiconducting properties of diamond, doped with boron, aluminum and titanium have been interpreted using the log R versus l/T curves. In boron-doped diamond ''high concentration" type im- purity conduction occurs and the activation energies vary from 0.15 eV to 0.30 eV. -
Flexible Thermal Interface Based on Self-Assembled Boron Arsenide for High-Performance Thermal Management
UCLA UCLA Previously Published Works Title Flexible thermal interface based on self-assembled boron arsenide for high-performance thermal management. Permalink https://escholarship.org/uc/item/4b77z423 Journal Nature communications, 12(1) ISSN 2041-1723 Authors Cui, Ying Qin, Zihao Wu, Huan et al. Publication Date 2021-02-24 DOI 10.1038/s41467-021-21531-7 Peer reviewed eScholarship.org Powered by the California Digital Library University of California ARTICLE https://doi.org/10.1038/s41467-021-21531-7 OPEN Flexible thermal interface based on self-assembled boron arsenide for high-performance thermal management ✉ Ying Cui1, Zihao Qin1, Huan Wu1, Man Li1 & Yongjie Hu 1 Thermal management is the most critical technology challenge for modern electronics. Recent key materials innovation focuses on developing advanced thermal interface of elec- 1234567890():,; tronic packaging for achieving efficient heat dissipation. Here, for the first time we report a record-high performance thermal interface beyond the current state of the art, based on self- assembled manufacturing of cubic boron arsenide (s-BAs). The s-BAs exhibits highly desirable characteristics of high thermal conductivity up to 21 W/m·K and excellent elastic compliance similar to that of soft biological tissues down to 100 kPa through the rational design of BAs microcrystals in polymer composite. In addition, the s-BAs demonstrates high flexibility and preserves the high conductivity over at least 500 bending cycles, opening up new application opportunities for flexible thermal cooling. Moreover, we demonstrated device integration with power LEDs and measured a superior cooling performance of s-BAs beyond the current state of the art, by up to 45 °C reduction in the hot spot temperature. -
Ultrahigh Thermal Conductivity in Isotope-Enriched Cubic Boron Nitride
Ultrahigh thermal conductivity in isotope-enriched cubic boron nitride The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Chen, Ke et al. "Ultrahigh thermal conductivity in isotope-enriched cubic boron nitride." Science 367, 6477 (January 2020): 555-559 © 2020 The Authors As Published http://dx.doi.org/10.1126/science.aaz6149 Publisher American Association for the Advancement of Science (AAAS) Version Author's final manuscript Citable link https://hdl.handle.net/1721.1/127819 Terms of Use Creative Commons Attribution-Noncommercial-Share Alike Detailed Terms http://creativecommons.org/licenses/by-nc-sa/4.0/ Ultrahigh thermal conductivity in isotope-enriched cubic boron nitride Ke Chen1*, Bai Song1*†‡,, Navaneetha K. Ravichandran2*, Qiye Zheng3§, Xi Chen4#, Hwijong Lee4, Haoran Sun5, Sheng Li6, Geethal Amila Gamage5, Fei Tian5, Zhiwei Ding1, Qichen Song1, Akash Rai3, Hanlin Wu6, Pawan Koirala6, Aaron J. Schmidt1, Kenji Watanabe7, Bing Lv6, Zhifeng Ren5, Li Shi4,8, David G. Cahill3, Takashi Taniguchi7, David Broido2†, and Gang Chen1† 1Department of Mechanical Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139, USA. 2Department of Physics, Boston College, Chestnut Hill, MA 02467, USA. 3Department of Materials Science and Engineering and Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, IL 61801, USA. 4Materials Science and Engineering Program, Texas Materials Institute, The University of Texas at Austin, Austin, TX 78712, USA 5Department of Physics and Texas Center for Superconductivity, University of Houston, Houston, TX 77204, USA. 6Department of Physics, The University of Texas at Dallas, Richardson, TX 75080, USA. 7National Institute for Materials Science, Namiki 1-1, Tsukuba, Ibaraki 305-0044, Japan. -
Thermoelectric Transports in Pristine and Functionalized Boron Phosphide Monolayers Min‑Shan Li1,3, Dong‑Chuan Mo2,3 & Shu‑Shen Lyu2,3*
www.nature.com/scientificreports OPEN Thermoelectric transports in pristine and functionalized boron phosphide monolayers Min‑Shan Li1,3, Dong‑Chuan Mo2,3 & Shu‑Shen Lyu2,3* Recently, a new monolayer Group III–V material, two‑dimensional boron phosphide (BP), has shown great potential for energy storage and energy conversion applications. We study the thermoelectric properties of BP monolayer as well as the efect of functionalization by frst‑principles calculation and Boltzmann transport theory. Combined with a moderate bandgap of 0.90 eV and ultra‑high carrier mobility, a large ZT value of 0.255 at 300 K is predicted for two‑dimensional BP. While the drastically reduced thermal conductivity in hydrogenated and fuorinated BP is favored for thermoelectric conversion, the decreased carrier mobility has limited the improvement of thermoelectric fgure of merit. Termoelectric material, which can directly convert waste heat into electricity, provides a promising solution for global issues like energy crisis1–4. Te thermoelectric performance of a material can be characterized by a dimensionless fgure of merit: S2σT ZT = , (1) kel + kla where S is the Seebeck coefcient, σ is the electronic conductivity, kel and kla are the thermal conductivities con- tributed by electrons and phonons, respectively. To obtain high thermoelectric performance, a material generally needs to have high electrical conductivity σ, high Seebeck coefcient S and low thermal conductivity k at the same time5. While the inter-coupling of the electronic parameters has made the optimization of thermoelectric performance a great challenge, early studies suggest that lowering the dimension of materials appears to be an efective approach6–9. -
Advanced Crystal Growth Techniques with Iii-V Boron Compound
ADVANCED CRYSTAL GROWTH TECHNIQUES WITH III-V BORON COMPOUND SEMICONDUCTORS by CLINTON E. WHITELEY B.S., Benedictine Collage, 2005 M.S., Kansas State University, 2008 AN ABSTRACT OF A DISSERTATION submitted in partial fulfillment of the requirements for the degree DOCTOR OF PHILOSOPHY Department of Chemical Engineering College of Engineering KANSAS STATE UNIVERSITY Manhattan, Kansas 2011 ABSTRACT Semiconducting icosahedral boron arsenide, B12As2, is an excellent candidate for neutron detectors and radioisotope batteries, for which high quality single crystals are required. Thus, the present study was undertaken to grow B12As2 crystals by precipitation from metal solutions (nickel) saturated with elemental boron and arsenic in a sealed quartz ampoule. B12As2 crystals of 8-10 mm were produced when a homogeneous mixture of the three elements was held at 1150 °C for 48-72 hours and slowly cooled (3°C/hr). The crystals varied in color and transparency from black and opaque to clear and transparent. X-ray topography (XRT), Raman spectroscopy, and defect selective etching confirmed that the crystals had the expected rhombohedral structure and a low density of defects (5x107 cm-2). The concentrations of residual impurities (nickel, carbon, etc) were found to be relatively high (1019 cm-3 for carbon) as measured by secondary ion mass spectrometry (SIMS) and elemental analysis by energy dispersive x-ray spectroscopy (EDS). The boron arsenide crystals were found to have favorable electrical properties (µ = 24.5 cm2 / Vs), but no interaction between a prototype detector and an alpha particle bombardment was observed. Thus, the flux growth method is viable for growing large B12As2 crystals, but the impurity concentrations remain a problem. -
Boron Isotope Effect on the Thermal Conductivity of Boron Arsenide Single Crystals
Boron isotope effect on the thermal conductivity of boron arsenide single crystals Haoran Sun1, Ke Chen2, Geethal Amila Gamage1, Hamidreza Ziyaee3, Fei Wang1, Yu Wang1,4, Viktor G. Hadjiev3, Fei Tian1†, Gang Chen2, and Zhifeng Ren1† 1 Department of Physics and Texas Center for Superconductivity (TcSUH), University of Houston, Houston, Texas 77204, USA 2 Department of Mechanical Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139, USA 3 Department of Mechanical Engineering and Texas Center for Superconductivity (TcSUH), University of Houston, Houston, Texas 77204, USA 4 Institute of Advanced Materials, Hubei Normal University, Huangshi, Hubei 435002, China †To whom correspondence should be addressed, email: [email protected], [email protected] Abstract Boron arsenide (BAs) with a zinc blende structure has recently been discovered to exhibit unusual and ultrahigh thermal conductivity (k), providing a new outlook for research on BAs and other high thermal conductivity materials. Technology for BAs crystal growth has been continuously improving, however, the influence of boron isotopes, pure or mixed, on the thermal conductivity in BAs is still not completely clear. Here we report detailed studies on the growth of single crystals of BAs with different isotopic ratios and demonstrate that the k of isotopically pure BAs is at least 10% higher than that of BAs grown from natural B. Raman spectroscopy characterization shows differences in scattering among various BAs samples. The presented results will be helpful in guiding further studies on the 1 influence of isotopes on optimizing k in BAs. 2 Introduction The heat produced in high power density electronic devices imposes a major limitation on the performance of these devices.