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Jacobson MZ, Sambor DJ, Fan YF, Mühlbauer A. Effects of firebricks for industrial process heat on the cost of matching all-sector energy demand with 100% wind-water-solar supply in 149 countries. PNAS NEXUS 2024; 3:pgae274. [PMID: 39045017 PMCID: PMC11263865 DOI: 10.1093/pnasnexus/pgae274] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 03/09/2024] [Accepted: 05/19/2024] [Indexed: 07/25/2024]
Abstract
Refractory bricks are bricks that can withstand high temperatures without damage to their structures. They have been used to insulate kilns, furnaces, and other hot enclosures for thousands of years. Firebricks are refractory bricks that can, with one composition, store heat, and with another, insulate the firebricks that store the heat. Because firebricks are made from common materials, the cost per kilowatt-hour-thermal of a firebrick storage system is less than one-tenth the cost per kilowatt-hour-electricity of a battery system. It has thus been hypothesized that using excess renewable electricity to produce and store industrial process heat in firebricks can provide a low-cost source of continuous heat for industry. Here, it is hypothesized further that, upon a transition to 100% clean, renewable energy worldwide, using firebricks to store industrial process heat can reduce electricity generator, electricity storage, and low-temperature heat storage needs, thereby reducing overall energy cost. Both hypotheses are tested across 149 countries combined into 29 world regions. Results suggest, relative to a base case with no firebricks, using firebricks may reduce, among all 149 countries, 2050 battery capacity by ∼14.5%, annual hydrogen production for grid electricity by ∼31%, underground low-temperature heat storage capacity by ∼27.3%; onshore wind nameplate capacity by ∼1.2%, land needs by ∼0.4%, and overall annual energy cost by ∼1.8%. In sum, the use of firebricks for storing industrial process heat appears to be a remarkable tool in reducing the cost of transitioning to clean, renewable energy across all energy sectors.
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Affiliation(s)
- Mark Z Jacobson
- Department of Civil and Environmental Engineering, Stanford University, 473 Via Ortega, Room 397, Stanford, CA 94305-4020, USA
| | - Daniel J Sambor
- Department of Civil and Environmental Engineering, Stanford University, 473 Via Ortega, Room 397, Stanford, CA 94305-4020, USA
| | - Yuanbei F Fan
- Department of Civil and Environmental Engineering, Stanford University, 473 Via Ortega, Room 397, Stanford, CA 94305-4020, USA
| | - Andreas Mühlbauer
- Department of Civil and Environmental Engineering, Stanford University, 473 Via Ortega, Room 397, Stanford, CA 94305-4020, USA
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2
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Imran M, Musa MY, Rauf S, Lu D, Li R, Tian Y. Polarization-insensitive perfect absorption in van der waals hyper-structure. Sci Rep 2024; 14:10068. [PMID: 38698124 PMCID: PMC11066130 DOI: 10.1038/s41598-024-60891-0] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/12/2024] [Accepted: 04/29/2024] [Indexed: 05/05/2024] Open
Abstract
Infrared perfect absorption has been widely investigated due to its potential applications in photodetectors, photovoltaics and medical diagnostics. In this report, we demonstrate that at particular infrared frequencies, a simple planar structure made up of graphene-hexagonal Boron Nitride (hBN) hyper-structure is able to nearly perfectly absorb incident light irrespective of its polarization (Transverse-Magnetic TM, or Transverse-Electric TE). By using this interferenceless technique, the hyper-structure achieves nearly zero reflectance at a wide range of angles in a narrow frequency band. We analytically predict the condition of achieving such an important feature of perfect absorption for both TM and TE polarizations. Interestingly, the infrared perfect absorption can be redshifted by increasing the thickness of the hBN layers and blueshifted by increasing the graphene's chemical potential. Such flexible control of infrared perfect absorption offers a new tool for controlling electromagnetic waves and has potential applications in photodetection and other light control applications.
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Affiliation(s)
- Muhammad Imran
- College of Mechatronics and Control Engineering, Shenzhen University, Shenzhen, 518000, China
| | - Muhyiddeen Yahya Musa
- Department of Agriculture and Bio-Environmental Engineering Technology, Audu Bako College of Agriculture Dambatta, Kano, Nigeria
| | - Sajid Rauf
- College of Mechatronics and Control Engineering, Shenzhen University, Shenzhen, 518000, China
| | - Dajiang Lu
- College of Mechatronics and Control Engineering, Shenzhen University, Shenzhen, 518000, China
| | - Rujiang Li
- National Key Laboratory of Radar Detection and Sensing, School of Electronic Engineering, Xidian University, Xi'an, 710071, China.
| | - Yibin Tian
- College of Mechatronics and Control Engineering, Shenzhen University, Shenzhen, 518000, China.
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3
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Abushattal AA, Loureiro AG, Boukortt NEI. Ultra-High Concentration Vertical Homo-Multijunction Solar Cells for CubeSats and Terrestrial Applications. MICROMACHINES 2024; 15:204. [PMID: 38398933 PMCID: PMC10893176 DOI: 10.3390/mi15020204] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/14/2023] [Revised: 01/18/2024] [Accepted: 01/25/2024] [Indexed: 02/25/2024]
Abstract
This paper examines advances in ultra-high concentration photovoltaics (UHCPV), focusing specifically on vertical multijunction (VMJ) solar cells. The use of gallium arsenide (GaAs) in these cells increases their efficiency in a range of applications, including terrestrial and space settings. Several multijunction structures are designed to maximize conversion efficiency, including a vertical tunnel junction, which minimizes resistive losses at high concentration levels compared with standard designs. Therefore, careful optimization of interconnect layers in terms of thickness and doping concentration is needed. Homo-multijunction GaAs solar cells have been simulated and analyzed by using ATLAS Silvaco 5.36 R, a sophisticated technology computer-aided design (TCAD) tool aimed to ensure the reliability of simulation by targeting a high conversion efficiency and a good fill factor for our proposed structure model. Several design parameters, such as the dimensional cell structure, doping density, and sun concentrations, have been analyzed to improve device performance under direct air mass conditions AM1.5D. The optimized conversion efficiency of 30.2% has been achieved with investigated GaAs solar cell configuration at maximum concentration levels.
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Affiliation(s)
- Ahmad A Abushattal
- Centro Singular de Investigación en Tecnoloxías de Información (CiTIUS), Universidad de Santiago de Compostela, 15705 Santiago de Compostela, Spain
- Department of Physics, Al-Hussein Bin Talal University, P.O. Box 20, Ma'an 71111, Jordan
| | - Antonio García Loureiro
- Centro Singular de Investigación en Tecnoloxías de Información (CiTIUS), Universidad de Santiago de Compostela, 15705 Santiago de Compostela, Spain
| | - Nour El I Boukortt
- Centro Singular de Investigación en Tecnoloxías de Información (CiTIUS), Universidad de Santiago de Compostela, 15705 Santiago de Compostela, Spain
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Wang J, Wu Z, Liu Y, Hou S, Qiao Y, Tang Z, Mao J, Zhang Q, Cao F. High-Selectivity Planar Thermal Emitter with a Stable Temperature over 1400 K for a Thermophotovoltaic System. ACS APPLIED MATERIALS & INTERFACES 2023; 15:49123-49131. [PMID: 37842846 DOI: 10.1021/acsami.3c10191] [Citation(s) in RCA: 1] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 10/17/2023]
Abstract
A selective thermal emitter with superior thermal stability and perfect selective thermal emission in specific bands can facilitate the lifting of the thermophotovoltaic (TPV) energy conversion efficiency in TPV systems. Scalable planar selective thermal emitters with superior spectral selectivity and robust high-temperature stability are desired to meet the requirements of large-scale deployments of TPV systems. However, stably reradiating the available thermal photons at above 1273 K remains a significant challenge for selective thermal emitters. In this work, we demonstrated a high-selectivity planar thermal emitter based on the composite ceramic of ZrC and Al2O3. The prepared selective thermal emitter provides an emissivity of around 90% above the photon energy (0.6 eV) at 1423 K, a strong emission suppression effect below 0.6 eV, and superior thermal stability up to at least 1423 K. Therefore, the overall spectral efficiency can reach around 53%. Coupled with an InGaAs PV cell, the TPV system based on the selective thermal emitter demonstrates a predicted heat-to-electricity power conversion efficiency of 29.78% at 1423 K due to the matched spectral response of the emitter with the PV cell. Our work opens a new way forward for TPV systems based on planar selective thermal emitters.
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Affiliation(s)
- Jian Wang
- School of Science, and Ministry of Industry and Information Technology Key Lab of Micro-Nano Optoelectronic Information System, Harbin Institute of Technology, Shenzhen 518055, China
| | - Zuoxu Wu
- School of Science, and Ministry of Industry and Information Technology Key Lab of Micro-Nano Optoelectronic Information System, Harbin Institute of Technology, Shenzhen 518055, China
| | - Yijie Liu
- School of Science, and Ministry of Industry and Information Technology Key Lab of Micro-Nano Optoelectronic Information System, Harbin Institute of Technology, Shenzhen 518055, China
| | - Shuaihang Hou
- School of Materials Science and Engineering, and Institute of Materials Genome & Big Data, Harbin Institute of Technology, Shenzhen 518055, Guangdong, China
| | - Youwei Qiao
- School of Science, and Ministry of Industry and Information Technology Key Lab of Micro-Nano Optoelectronic Information System, Harbin Institute of Technology, Shenzhen 518055, China
| | - Zunqian Tang
- School of Science, and Ministry of Industry and Information Technology Key Lab of Micro-Nano Optoelectronic Information System, Harbin Institute of Technology, Shenzhen 518055, China
| | - Jun Mao
- School of Materials Science and Engineering, and Institute of Materials Genome & Big Data, Harbin Institute of Technology, Shenzhen 518055, Guangdong, China
| | - Qian Zhang
- School of Materials Science and Engineering, and Institute of Materials Genome & Big Data, Harbin Institute of Technology, Shenzhen 518055, Guangdong, China
| | - Feng Cao
- School of Science, and Ministry of Industry and Information Technology Key Lab of Micro-Nano Optoelectronic Information System, Harbin Institute of Technology, Shenzhen 518055, China
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5
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Lee HJ, Ker PJ, Gamel MMA, Jamaludin MZ, Wong YH. Predictive analysis of the power spectral irradiance from blackbody radiation source using single pixel detector. Heliyon 2023; 9:e20585. [PMID: 37842600 PMCID: PMC10569944 DOI: 10.1016/j.heliyon.2023.e20585] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/19/2023] [Revised: 08/11/2023] [Accepted: 09/29/2023] [Indexed: 10/17/2023] Open
Abstract
Accurate spectral irradiance measurement in the near-infrared range is significant for the design and characterization of photodetector and photovoltaic cells. Approximation method is commonly used to solve for the input power using estimated spectral irradiance, where the dependency on wavelength and temperature remains uncertain. This study aims to determine the power spectrum at different radiation temperatures using a single pixel photodetector, taking into consideration factors such as transmission spectra of alumina radiator, CaF2 collimating lens, responsivity, and measured photocurrent information of photodetectors. Utilizing predictive mathematical model, five commercial photodetectors, including Silicon, Germanium, In0.53Ga0.47As, In0.73Ga0.27As, and In0.83Ga0.17As were used to solve for the power densities as a function of wavelengths at radiation temperatures of 1000 °C and 1500 °C. The spectral irradiance of photodetectors was determined with a percentage difference of <4.9 %, presenting an accurate power density estimation for the spectrum at a wide range of radiation temperatures. Power irradiance data obtained were validated in the narrow wavelength range with 1000 nm, 1400 nm, 1500 nm, and 2000 nm bandpass filters. The reported work demonstrates a simple and efficient way which could contribute to develop a cost-effective method of measuring and determining the spectrum irradiances of objects at different radiation temperatures. This predictive analysis method hopefully intensifies the progress of efforts to reduce the reliance on complex optoelectronic instruments in accurately solving power irradiance information.
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Affiliation(s)
- Hui Jing Lee
- Electrical & Electronics Department, College of Engineering, Institute of Power Engineering, Universiti Tenaga Nasional, 43000, Kajang, Selangor, Malaysia
| | - Pin Jern Ker
- Electrical & Electronics Department, College of Engineering, Institute of Sustainable Energy, Universiti Tenaga Nasional, 43000, Kajang, Selangor, Malaysia
| | | | - Md Zaini Jamaludin
- Electrical & Electronics Department, College of Engineering, Institute of Power Engineering, Universiti Tenaga Nasional, 43000, Kajang, Selangor, Malaysia
| | - Yew Hoong Wong
- Department of Mechanical Engineering, Faculty of Engineering, Universiti Malaya, 50603, Kuala Lumpur, Malaysia
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Sutherland WJ, Bennett C, Brotherton PNM, Butterworth HM, Clout MN, Côté IM, Dinsdale J, Esmail N, Fleishman E, Gaston KJ, Herbert-Read JE, Hughes A, Kaartokallio H, Le Roux X, Lickorish FA, Matcham W, Noor N, Palardy JE, Pearce-Higgins JW, Peck LS, Pettorelli N, Pretty J, Scobey R, Spalding MD, Tonneijck FH, Tubbs N, Watson JEM, Wentworth JE, Wilson JD, Thornton A. A global biological conservation horizon scan of issues for 2023. Trends Ecol Evol 2023; 38:96-107. [PMID: 36460563 DOI: 10.1016/j.tree.2022.10.005] [Citation(s) in RCA: 3] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/07/2022] [Revised: 10/24/2022] [Accepted: 10/25/2022] [Indexed: 12/03/2022]
Abstract
We present the results of our 14th horizon scan of issues we expect to influence biological conservation in the future. From an initial set of 102 topics, our global panel of 30 scientists and practitioners identified 15 issues we consider most urgent for societies worldwide to address. Issues are novel within biological conservation or represent a substantial positive or negative step change at global or regional scales. Issues such as submerged artificial light fisheries and accelerating upper ocean currents could have profound negative impacts on marine or coastal ecosystems. We also identified potentially positive technological advances, including energy production and storage, improved fertilisation methods, and expansion of biodegradable materials. If effectively managed, these technologies could realise future benefits for biological diversity.
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Affiliation(s)
- William J Sutherland
- Conservation Science Group, Department of Zoology, Cambridge University, The David Attenborough Building, Pembroke Street, Cambridge CB2 3QZ, UK; Biosecurity Research Initiative at St Catharine's (BioRISC), St Catharine's College, University of Cambridge, Cambridge, UK.
| | - Craig Bennett
- Royal Society of Wildlife Trusts, The Kiln, Waterside, Mather Road, Newark, Nottinghamshire NG24 1WT, UK
| | - Peter N M Brotherton
- Natural England, 4th Floor Foss House, Kings Pool, 1-2 Peasholme Green, York YO1 7PX, UK
| | - Holly M Butterworth
- Natural Resources Wales, Cambria House, 29 Newport Road, Cardiff CF24 0TP, UK
| | - Mick N Clout
- Centre for Biodiversity and Biosecurity, School of Biological Sciences, University of Auckland, PB 92019, Auckland, New Zealand
| | - Isabelle M Côté
- Department of Biological Sciences, Simon Fraser University, Burnaby, BC V5A 1S6, Canada
| | - Jason Dinsdale
- Environment Agency, Horizon House, Deanery Road, Bristol BS1 5AH, UK
| | - Nafeesa Esmail
- Wilder Institute/Calgary Zoo, 1300 Zoo Road NE, Calgary, AB T2E 7V6, Canada
| | - Erica Fleishman
- College of Earth, Ocean, and Atmospheric Sciences, Oregon State University, Corvallis, OR 97331, USA
| | - Kevin J Gaston
- Environment and Sustainability Institute, University of Exeter, Penryn, Cornwall TR10 9FE, UK
| | | | - Alice Hughes
- School of Biological Sciences, University of Hong Kong, Pok Fu Lam, Hong Kong
| | | | - Xavier Le Roux
- University of Lyon, Microbial Ecology Centre, INRAE (UMR1418), CNRS (UMR5557), University Lyon 1, 69622 Villeurbanne, France
| | - Fiona A Lickorish
- UK Research and Consultancy Services (RCS) Ltd, Valletts Cottage, Westhope, Hereford HR4 8BU, UK
| | - Wendy Matcham
- Natural Environment Research Council, UK Research and Innovation, Polaris House, North Star Avenue, Swindon SN2 1FL, UK
| | - Noor Noor
- UN Environment Programme World Conservation Monitoring Centre (UNEP-WCMC), 219 Huntingdon Road, Cambridge CB3 0DL, UK
| | - James E Palardy
- The Pew Charitable Trusts, 901 E St. NW, Washington, DC 20004, USA
| | - James W Pearce-Higgins
- Conservation Science Group, Department of Zoology, Cambridge University, The David Attenborough Building, Pembroke Street, Cambridge CB2 3QZ, UK; British Trust for Ornithology, The Nunnery, Thetford, Norfolk IP24 2PU, UK
| | - Lloyd S Peck
- British Antarctic Survey, Natural Environment Research Council, High Cross, Madingley Road, Cambridge CB3 0ET, UK
| | - Nathalie Pettorelli
- Institute of Zoology, Zoological Society of London, Regent's Park, London NW1 4RY, UK
| | - Jules Pretty
- Centre for Public and Policy Engagement and School of Life Sciences, University of Essex, Colchester CO4 3SQ, UK
| | - Richard Scobey
- TRAFFIC, The David Attenborough Building, Pembroke Street, Cambridge CB2 3QZ, UK
| | - Mark D Spalding
- Conservation Science Group, Department of Zoology, Cambridge University, The David Attenborough Building, Pembroke Street, Cambridge CB2 3QZ, UK; The Nature Conservancy, Strade delle Tolfe, 14, Siena 53100, Italy
| | | | - Nicolas Tubbs
- WWF-Belgium, BD Emile Jacqumainlaan 90, 1000 Brussels, Belgium
| | - James E M Watson
- School of Earth and Environmental Sciences, University of Queensland, St Lucia, QLD 4072, Australia
| | - Jonathan E Wentworth
- Parliamentary Office of Science and Technology, 14 Tothill Street, Westminster, London SW1H 9NB, UK
| | - Jeremy D Wilson
- RSPB Centre for Conservation Science, 2 Lochside View, Edinburgh EH12 9DH, UK
| | - Ann Thornton
- Conservation Science Group, Department of Zoology, Cambridge University, The David Attenborough Building, Pembroke Street, Cambridge CB2 3QZ, UK
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Islam NA, Choi S. Bowtie Nanoantenna Coupled Metal-Oxide-Silicon (p-Doped) Diode for 28.3 THz IR Rectification. NANOMATERIALS (BASEL, SWITZERLAND) 2022; 12:3940. [PMID: 36432226 PMCID: PMC9693361 DOI: 10.3390/nano12223940] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 10/17/2022] [Revised: 10/31/2022] [Accepted: 11/06/2022] [Indexed: 06/16/2023]
Abstract
Low-temperature waste heat in the infrared (IR) wavelength region offers an opportunity to harvest power from waste energy and requires further investigation in order to find efficient conversion techniques. Although grating-coupled metal-oxide-semiconductor (MOS) diode devices offer efficient conversion from low and moderate-temperature thermal sources, the integration of such diodes with a nanoantenna structure has yet to be explored. We propose a bowtie nanoantenna coupled with a p-doped MOS diode for IR to direct current (DC) conversion without any bias voltage at 28.3 THz. The nanoantenna was designed and optimized to provide maximum field enhancement in a 4 nm-thick oxide layer at the resonant frequency. The device was fabricated following the complementary MOS (CMOS) fabrication process and measured in a custom DC and optical characterization setup using a 10.6 μm wavelength CO2 laser. The results reveal two different types of devices with linear and nonlinear I-V curves having kΩ and MΩ zero-bias resistance, respectively. The linear device generates a micron-level open-circuit voltage (Voc) with clear polarization dependence from the laser input, but the nonlinear case suffers from a weak noise-like signal. Finally, we analyze two types of devices using thermoelectric and tunneling effects and discuss the future direction of nanoantenna-integrated MOS devices for efficient IR harvesters.
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Affiliation(s)
- Nasim Al Islam
- Department of Electrical, Electronic, and Computer Engineering, University of Ulsan, Ulsan 44610, Korea
| | - Sangjo Choi
- School of Electronics Engineering, Kyungpook National University, Daegu 41566, Korea
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Refractory All-Ceramic Thermal Emitter for High-Temperature Near-Field Thermophotovoltaics. ENERGIES 2022. [DOI: 10.3390/en15051830] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 02/01/2023]
Abstract
Thermophotovoltaics is a promising technology for heat recovery and has garnered tremendous attention in the last decades. This work theoretically evaluates the performance of a thermophotovoltaic system equipped with refractory all-ceramic selective thermal emitters made of boron carbide, silicon carbide and beryllium oxide for a high working temperature of 2000 ∘C, which corresponds to the external quantum efficiency of a SiC/Si tandem cell. The influence of thickness and filling ratio on the emissivity of thermal emitters over the wavelength ranging from 0.2 μm to 2.5 μm is studied. The corresponding spectral heat flux and output power are analyzed as well. For a specific configuration, the parameters for the thermophotovoltaic system are obtained, including short circuit current, open circuit voltage, fill factor, total heat flux, output power and conversion efficiency. The proposed all-ceramic thermal emitter ensures the robustness in the high-temperature working condition due to its thermal stability. The tuning of emissivity is achieved and analyzed based on distinct emitter nanostructures, and the further influence on the thermophotovoltaic system performance is deeply explored. This work sheds light on research of high-temperature thermal management and power generation.
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9
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Liu H, Dan Y, Zhang A, Liu S, Yue J, Li J, Ma X, Huang Y, Liu Y, Cui T. First-Principles Study of High-Pressure Phase Stability and Electron Properties of Be-P Compounds. MATERIALS 2022; 15:ma15031255. [PMID: 35161197 PMCID: PMC8839631 DOI: 10.3390/ma15031255] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 12/23/2021] [Revised: 01/27/2022] [Accepted: 02/01/2022] [Indexed: 11/23/2022]
Abstract
New, stable stoichiometries in Be-P systems are investigated up to 100 GPa by the CALYPSO structure prediction method. Along with the BeP2-I41/amd structure, we identify two novel compounds of Be3P2-P-421m and Be3P2-C2/m. It should be noted that the Be-P compounds are predicted to be energetically unfavorable above 40 GPa. As can be seen, interesting structures may be experimentally synthesizable at modest pressure. Our results indicate that at 33.2 GPa, the most stable ambient-pressure tetragonal Be3P2-P-421m transitions to the monoclinic Be3P2-C2/m structure. Moreover, the predicted Be3P2-P-421m and Be3P2-C2/m phases are energetically favored compared with the Be3P2-Ia-3 structure synthesized experimentally. Electronic structure calculations reveal that BeP2-I41/amd, Be3P2-P-421m, and Be3P2-C2/m are all semiconductors with a narrow band gap. The present findings offer insight and guidance for exploration toward further fundamental understanding and potential applications in the semiconductor field.
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Affiliation(s)
- Han Liu
- Institute of High Pressure Physics, School of Physical Science and Technology, Ningbo University, Ningbo 315211, China; (H.L.); (Y.D.); (A.Z.); (J.Y.); (J.L.); (Y.H.)
- Department of Physics, College of Science, Yanbian University, Yanji 133000, China
| | - Yaqian Dan
- Institute of High Pressure Physics, School of Physical Science and Technology, Ningbo University, Ningbo 315211, China; (H.L.); (Y.D.); (A.Z.); (J.Y.); (J.L.); (Y.H.)
| | - Ao Zhang
- Institute of High Pressure Physics, School of Physical Science and Technology, Ningbo University, Ningbo 315211, China; (H.L.); (Y.D.); (A.Z.); (J.Y.); (J.L.); (Y.H.)
- Department of Physics, College of Science, Yanbian University, Yanji 133000, China
| | - Siyuan Liu
- School of Physics, Southeast University, Nanjing 211189, China;
| | - Jincheng Yue
- Institute of High Pressure Physics, School of Physical Science and Technology, Ningbo University, Ningbo 315211, China; (H.L.); (Y.D.); (A.Z.); (J.Y.); (J.L.); (Y.H.)
| | - Junda Li
- Institute of High Pressure Physics, School of Physical Science and Technology, Ningbo University, Ningbo 315211, China; (H.L.); (Y.D.); (A.Z.); (J.Y.); (J.L.); (Y.H.)
| | - Xuejiao Ma
- Science and Technology on Transient Impact Laboratory, No. 208 Research Institute of Ordnance Industries, Beijing 102202, China;
| | - Yanping Huang
- Institute of High Pressure Physics, School of Physical Science and Technology, Ningbo University, Ningbo 315211, China; (H.L.); (Y.D.); (A.Z.); (J.Y.); (J.L.); (Y.H.)
| | - Yanhui Liu
- Institute of High Pressure Physics, School of Physical Science and Technology, Ningbo University, Ningbo 315211, China; (H.L.); (Y.D.); (A.Z.); (J.Y.); (J.L.); (Y.H.)
- Correspondence: (Y.L.); (T.C.)
| | - Tian Cui
- Institute of High Pressure Physics, School of Physical Science and Technology, Ningbo University, Ningbo 315211, China; (H.L.); (Y.D.); (A.Z.); (J.Y.); (J.L.); (Y.H.)
- Correspondence: (Y.L.); (T.C.)
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