Unlocking the narrow bandgap investigations of perovskite JHgF3 (J = Li, Na, and Rb) materials: Computational predictions for optoelectronic devices

In the current day, light control has become a significant issue that perovskite materials can help with. The physical properties of halide perovskite JHgF3 (where J = Li, Na, and Rb) materials are examined for this purpose utilizing the GGA-PBE exchange correlation-functional and first principle co...

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Published in:The Journal of physics and chemistry of solids Vol. 203; p. 112729
Main Authors: Shahzad, Muhammad Khuram, Hussain, Shoukat, Kumar, Abhinav, Rekha, M.M., Pattanayak, Binayak, Jayabalan, Karthikeyan, Pandey, Vivek Kumar, Oza, Ankit D., Tirth, Vineet, Hussien, Mohamed, Sfina, N.
Format: Journal Article
Language:English
Published: Elsevier Ltd 01.08.2025
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ISSN:0022-3697
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Abstract In the current day, light control has become a significant issue that perovskite materials can help with. The physical properties of halide perovskite JHgF3 (where J = Li, Na, and Rb) materials are examined for this purpose utilizing the GGA-PBE exchange correlation-functional and first principle computations (CASTEP). The compounds are cubic in shape, with five atoms per unit cell, and their space group is Pm3 m (221). Calculations reveal that the band structure of JHgF3 (where J = Li, Na, and Rb) exhibits a semiconductor nature with band gaps of 0.44, 0.45, and 0.62 eV. Perovskite materials' band structure graphs, partial DOS, and density of states (DOS) all clearly demonstrate their semi conductive characteristics. The JHgF3 (J = Li, Na, and Rb) compound is evaluated on the based of its mechanical aspects, including modulus (B, E, G), Poisson's ratiosvp (0.37, 0.36, and 0.34), Pugh's ratio (3.54, 3.43, and 3.82), mechanical index (14.020, 6.001, and 1.788), Cauchy pressure (22.585, 23.806, and 18.322), and hardness H (1.044, 1.265, and 1.688). In order to identify the light-matter interactions, the optical characteristics of JHgF3 have also been investigated and assessed. The study looks at thermodynamic parameters such as Debye temperature, melting temperature, sound velocity, and compressibility. The physical characteristics of the materials under study indicate that JHgF3 is appropriate for use in optoelectronic gadgets and applications. •JHgF3 (J = Li, Na, and Rb) perovskites have been investigated using DFT.•Compounds are found to be energetically, mechanically and dynamically stable.•Achieved narrow bandgap, higher effective light absorption, for optoelectronics applications.
AbstractList In the current day, light control has become a significant issue that perovskite materials can help with. The physical properties of halide perovskite JHgF3 (where J = Li, Na, and Rb) materials are examined for this purpose utilizing the GGA-PBE exchange correlation-functional and first principle computations (CASTEP). The compounds are cubic in shape, with five atoms per unit cell, and their space group is Pm3 m (221). Calculations reveal that the band structure of JHgF3 (where J = Li, Na, and Rb) exhibits a semiconductor nature with band gaps of 0.44, 0.45, and 0.62 eV. Perovskite materials' band structure graphs, partial DOS, and density of states (DOS) all clearly demonstrate their semi conductive characteristics. The JHgF3 (J = Li, Na, and Rb) compound is evaluated on the based of its mechanical aspects, including modulus (B, E, G), Poisson's ratiosvp (0.37, 0.36, and 0.34), Pugh's ratio (3.54, 3.43, and 3.82), mechanical index (14.020, 6.001, and 1.788), Cauchy pressure (22.585, 23.806, and 18.322), and hardness H (1.044, 1.265, and 1.688). In order to identify the light-matter interactions, the optical characteristics of JHgF3 have also been investigated and assessed. The study looks at thermodynamic parameters such as Debye temperature, melting temperature, sound velocity, and compressibility. The physical characteristics of the materials under study indicate that JHgF3 is appropriate for use in optoelectronic gadgets and applications. •JHgF3 (J = Li, Na, and Rb) perovskites have been investigated using DFT.•Compounds are found to be energetically, mechanically and dynamically stable.•Achieved narrow bandgap, higher effective light absorption, for optoelectronics applications.
ArticleNumber 112729
Author Rekha, M.M.
Pandey, Vivek Kumar
Oza, Ankit D.
Tirth, Vineet
Hussien, Mohamed
Jayabalan, Karthikeyan
Kumar, Abhinav
Hussain, Shoukat
Sfina, N.
Pattanayak, Binayak
Shahzad, Muhammad Khuram
Author_xml – sequence: 1
  givenname: Muhammad Khuram
  surname: Shahzad
  fullname: Shahzad, Muhammad Khuram
  email: khuram_chukhia@yahoo.com
  organization: Institute of Physics, Khwaja Fareed University of Engineering and Information Technology, Rahim Yar Khan, 64200, Pakistan
– sequence: 2
  givenname: Shoukat
  orcidid: 0000-0002-7472-0006
  surname: Hussain
  fullname: Hussain, Shoukat
  organization: Institute of Physics, Khwaja Fareed University of Engineering and Information Technology, Rahim Yar Khan, 64200, Pakistan
– sequence: 3
  givenname: Abhinav
  surname: Kumar
  fullname: Kumar, Abhinav
  email: drabhinav@ieee.org
  organization: Department of Nuclear and Renewable Energy, Ural Federal University Named After the First President of Russia Boris Yeltsin, Ekaterinburg, 620002, Russia
– sequence: 4
  givenname: M.M.
  surname: Rekha
  fullname: Rekha, M.M.
  organization: Department of Chemistry and Biochemistry, School of Sciences, JAIN (Deemed to be University), Bangalore, Karnataka, India
– sequence: 5
  givenname: Binayak
  surname: Pattanayak
  fullname: Pattanayak, Binayak
  organization: Department of Mechanical Engineering, Siksha 'O' Anusandhan (Deemed to be University), Bhubaneswar, Odisha, 751030, India
– sequence: 6
  givenname: Karthikeyan
  surname: Jayabalan
  fullname: Jayabalan, Karthikeyan
  organization: Department of Chemistry, Sathyabama Institute of Science and Technology, Chennai, Tamil Nadu, India
– sequence: 7
  givenname: Vivek Kumar
  surname: Pandey
  fullname: Pandey, Vivek Kumar
  organization: Centre for Research Impact & Outcome, Chitkara University Institute of Engineering and Technology, Chitkara University, Rajpura, 140401, Punjab, India
– sequence: 8
  givenname: Ankit D.
  surname: Oza
  fullname: Oza, Ankit D.
  organization: University Centre for Research and Development, Chandigarh University, Mohali, Punjab, 140413, India
– sequence: 9
  givenname: Vineet
  orcidid: 0000-0002-8208-7183
  surname: Tirth
  fullname: Tirth, Vineet
  organization: Central Labs, King Khalid University, AlQura'a, P.O. Box 960, Abha, Saudi Arabia
– sequence: 10
  givenname: Mohamed
  orcidid: 0000-0002-3551-9078
  surname: Hussien
  fullname: Hussien, Mohamed
  organization: Central Labs, King Khalid University, AlQura'a, P.O. Box 960, Abha, Saudi Arabia
– sequence: 11
  givenname: N.
  surname: Sfina
  fullname: Sfina, N.
  organization: College of Sciences and Arts in MahayelAsir, Department of Physics, King Khalid University, Abha, 61413, Saudi Arabia
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Snippet In the current day, light control has become a significant issue that perovskite materials can help with. The physical properties of halide perovskite JHgF3...
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SubjectTerms DFT
Electronic properties
Optoelectronic properties
Perovskites
Title Unlocking the narrow bandgap investigations of perovskite JHgF3 (J = Li, Na, and Rb) materials: Computational predictions for optoelectronic devices
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