Pub Date : 2024-08-29DOI: 10.1016/j.ssc.2024.115671
Sagar Bhattarai , Mustafa K.A. Mohammed , Ismail Hossain , Pratap Kumar Dakua , Rahul Pandey , Jaya Madan
Photovoltaics (PV) having perovskite material have an enormous influence on the progress in solar cell technology. Excluding the high efficiency, stability, and flexibility, the extended impact has now been given on utilizing lead-free environmentally suitable, and much cheaper materials for the PSC fabrication. The material with a volatile free, that is, cesium tin iodide (CsSnI3), is capable for the fabrication of the Perovskite Solar Cell that creates eco-friendly as well as enhanced optical-electronic features for the low bandgap, that is 1.27eV. Sn could increase the steadiness of the lead-free perovskite. However, as widely known, Sn2+ always suffers from oxidation with I2 and O2 and induces instability issues. In the ongoing work, cesium tin iodide, is employed as the primary absorber, in so much the root-extracted naturally manufactured ZnO is used as ETM for less cost in production. Correspondingly, Spiro-OMeTAD is used as HTM for enhancement in hole collection in the device. The inclusive numerical simulation with the bio-synthesized ZnO-NP can be applied in designing the solar cell having an applicable thickness of CsSnI3, suitable temperature, total defect density, and the influence of the resistance, respectively. The current simulation of PSC offers the extraordinary power conversion efficiency (η) of 26.40 % considering CsSnI3 as the absorber. The results described in this investigation may confirm an effective approach to design and the expansion of the lead-free PSC.
{"title":"Bio-synthesized ZnO in cesium based perovskite solar cells: A pathway to sustainable high efficiency","authors":"Sagar Bhattarai , Mustafa K.A. Mohammed , Ismail Hossain , Pratap Kumar Dakua , Rahul Pandey , Jaya Madan","doi":"10.1016/j.ssc.2024.115671","DOIUrl":"10.1016/j.ssc.2024.115671","url":null,"abstract":"<div><p>Photovoltaics (PV) having perovskite material have an enormous influence on the progress in solar cell technology. Excluding the high efficiency, stability, and flexibility, the extended impact has now been given on utilizing lead-free environmentally suitable, and much cheaper materials for the PSC fabrication. The material with a volatile free, that is, cesium tin iodide (CsSnI<sub>3</sub>), is capable for the fabrication of the Perovskite Solar Cell that creates eco-friendly as well as enhanced optical-electronic features for the low bandgap, that is 1.27eV. Sn could increase the steadiness of the lead-free perovskite. However, as widely known, Sn<sup>2+</sup> always suffers from oxidation with I<sub>2</sub> and O<sub>2</sub> and induces instability issues. In the ongoing work, cesium tin iodide, is employed as the primary absorber, in so much the root-extracted naturally manufactured ZnO is used as ETM for less cost in production. Correspondingly, Spiro-OMeTAD is used as HTM for enhancement in hole collection in the device. The inclusive numerical simulation with the bio-synthesized ZnO-NP can be applied in designing the solar cell having an applicable thickness of CsSnI<sub>3</sub>, suitable temperature, total defect density, and the influence of the resistance, respectively. The current simulation of PSC offers the extraordinary power conversion efficiency (η) of 26.40 % considering CsSnI<sub>3</sub> as the absorber. The results described in this investigation may confirm an effective approach to design and the expansion of the lead-free PSC.</p></div>","PeriodicalId":430,"journal":{"name":"Solid State Communications","volume":"393 ","pages":"Article 115671"},"PeriodicalIF":2.1,"publicationDate":"2024-08-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142096820","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-28DOI: 10.1016/j.ssc.2024.115668
F. Chafai , W. Bouzidi , R. Fersi , L. Patout , M. Descoins , K. Hoummada , L. Bessais , A. Charaï , N. Thabet Mliki
Nanocrystalline rare-earth (R) and transition metal (T) alloys are known for their outstanding magnetic properties, which are driven by the combination of (R) and (T) magnetic moments. Adding carbon (C) has been proven to alter these magnetic properties. In the present work, we use X-ray diffraction, transmission electron microscopy, and atom probe tomography to investigate and characterize the impact of carbon addition on the crystalline structure, morphology, and chemical distribution of Pr5Co19 and its carbides Pr5Co19Cx. The nanocrystalline Pr5Co19 compound was synthesized by high-energy ball milling and the addition of carbon was performed by a solid-solid reaction between Pr5Co19 and C10H14. TEM study revealed that after carbonation the microstructure is refined, and the mean grain size decreases from 126 nm in Pr5Co19 to 65 nm with a carbon of content 1.5. Three-dimensional APT was performed to characterize the chemical composition of Pr-Co binary systems. The analyzed Pr5Co19C1.5 sample reveals an irregular nano-lamella structure decorated by carbon atoms, the distance between the lamellas varying from 8 to 20 nm. An under-stoichiometry of Co was found in the C-rich lamellas. Fundamental magnetic properties such as saturation magnetization Ms, exchange field Hex and magnetic susceptibility of the Pr5Co19 and its carbides were calculated using the random magnetic anisotropy (RMA) method.
{"title":"Structural, morphological, and magnetic properties of carbon-modified nanocrystalline Pr5Co19 alloys","authors":"F. Chafai , W. Bouzidi , R. Fersi , L. Patout , M. Descoins , K. Hoummada , L. Bessais , A. Charaï , N. Thabet Mliki","doi":"10.1016/j.ssc.2024.115668","DOIUrl":"10.1016/j.ssc.2024.115668","url":null,"abstract":"<div><p>Nanocrystalline rare-earth (R) and transition metal (T) alloys are known for their outstanding magnetic properties, which are driven by the combination of (R) and (T) magnetic moments. Adding carbon (C) has been proven to alter these magnetic properties. In the present work, we use X-ray diffraction, transmission electron microscopy, and atom probe tomography to investigate and characterize the impact of carbon addition on the crystalline structure, morphology, and chemical distribution of Pr<sub>5</sub>Co<sub>19</sub> and its carbides Pr<sub>5</sub>Co<sub>19</sub>C<sub>x</sub>. The nanocrystalline Pr<sub>5</sub>Co<sub>19</sub> compound was synthesized by high-energy ball milling and the addition of carbon was performed by a solid-solid reaction between Pr<sub>5</sub>Co<sub>19</sub> and C<sub>10</sub>H<sub>14</sub>. TEM study revealed that after carbonation the microstructure is refined, and the mean grain size decreases from 126 nm in Pr<sub>5</sub>Co<sub>19</sub> to 65 nm with a carbon of content 1.5. Three-dimensional APT was performed to characterize the chemical composition of Pr-Co binary systems. The analyzed Pr<sub>5</sub>Co<sub>19</sub>C<sub>1.5</sub> sample reveals an irregular nano-lamella structure decorated by carbon atoms, the distance between the lamellas varying from 8 to 20 nm. An under-stoichiometry of Co was found in the C-rich lamellas. Fundamental magnetic properties such as saturation magnetization M<sub>s</sub>, exchange field H<sub>ex</sub> and magnetic susceptibility <span><math><mrow><mi>χ</mi></mrow></math></span> of the Pr<sub>5</sub>Co<sub>19</sub> and its carbides were calculated using the random magnetic anisotropy (RMA) method.</p></div>","PeriodicalId":430,"journal":{"name":"Solid State Communications","volume":"393 ","pages":"Article 115668"},"PeriodicalIF":2.1,"publicationDate":"2024-08-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142122791","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-26DOI: 10.1016/j.ssc.2024.115669
Athar Javed , Muhammad Haseeb , Altaf Hussain , Muhammad Amir Rafiq
Structural, electronic, optical, mechanical, thermoelectric and dielectric properties of binary Bi2A3 (A = S, Se, Te) chalcogenide semiconductors are studied by first-principles approach. Bismuth sulfide (Bi2S3) is found to be structurally stable in orthorhombic structure while bismuth selenide (Bi2Se3) and bismuth telluride (Bi2Te3) are stable in trigonal structure. Calculated mechanical properties reveal that all three Bi2A3 (A = S, Se, Te) compounds fulfil the mechanical stability criteria. Band structure calculations reveal that the Bi2S3 exhibits direct optical band gap (Eg = 1. 58 eV) which lies in the near-infrared (NIR) region, while the calculated Eg of Bi2Se3 and Bi2Te3 are found to be 0.53 eV and 0.35 eV, respectively lying in the far-infrared region. For Bi2S3 and Bi2Se3 compounds, the calculated dielectric properties show strong anisotropic behavior, while negligible anisotropic dielectric behavior is observed for Bi2Te3. Calculated optical properties show that all three Bi2A3 compounds possess high absorption coefficient (> 104 cm−1). For all three Bi2A3 (A = S, Se, Te) compounds, the calculated optical conductivity show prominent peak corresponding to the occurrence of optical conduction at energies 3.36 eV, 2.65 eV and 2.02 eV respectively. Calculated optical results support the results deduced from band structures and density of states spectra. Optical properties and dielectric behavior suggest that the Bi2S3 compound has suitable band gap and has potential to use for photovoltaic applications while Bi2A3 (A = Se, Te) compounds could be used in infrared detectors and other optical devices. Calculated thermal properties reveal that the Bi2A3 (A = S, Se, Te) chalcogenides could be potential materials for thermoelectric applications.
{"title":"Properties of bismuth based Bi2A3 (A = S, Se, Te) chalcogenides for optoelectronic and thermoelectric applications","authors":"Athar Javed , Muhammad Haseeb , Altaf Hussain , Muhammad Amir Rafiq","doi":"10.1016/j.ssc.2024.115669","DOIUrl":"10.1016/j.ssc.2024.115669","url":null,"abstract":"<div><p>Structural, electronic, optical, mechanical, thermoelectric and dielectric properties of binary Bi<sub>2</sub>A<sub>3</sub> (A = S, Se, Te) chalcogenide semiconductors are studied by first-principles approach. Bismuth sulfide (Bi<sub>2</sub>S<sub>3</sub>) is found to be structurally stable in orthorhombic structure while bismuth selenide (Bi<sub>2</sub>Se<sub>3</sub>) and bismuth telluride (Bi<sub>2</sub>Te<sub>3</sub>) are stable in trigonal structure. Calculated mechanical properties reveal that all three Bi<sub>2</sub>A<sub>3</sub> (A = S, Se, Te) compounds fulfil the mechanical stability criteria. Band structure calculations reveal that the Bi<sub>2</sub>S<sub>3</sub> exhibits direct optical band gap (<em>E</em><sub><em>g</em></sub> = 1. 58 eV) which lies in the near-infrared (NIR) region, while the calculated <em>E</em><sub><em>g</em></sub> of Bi<sub>2</sub>Se<sub>3</sub> and Bi<sub>2</sub>Te<sub>3</sub> are found to be 0.53 eV and 0.35 eV, respectively lying in the far-infrared region. For Bi<sub>2</sub>S<sub>3</sub> and Bi<sub>2</sub>Se<sub>3</sub> compounds, the calculated dielectric properties show strong anisotropic behavior, while negligible anisotropic dielectric behavior is observed for Bi<sub>2</sub>Te<sub>3</sub>. Calculated optical properties show that all three Bi<sub>2</sub>A<sub>3</sub> compounds possess high absorption coefficient (> 10<sup>4</sup> cm<sup>−1</sup>). For all three Bi<sub>2</sub>A<sub>3</sub> (A = S, Se, Te) compounds, the calculated optical conductivity show prominent peak corresponding to the occurrence of optical conduction at energies 3.36 eV, 2.65 eV and 2.02 eV respectively. Calculated optical results support the results deduced from band structures and density of states spectra. Optical properties and dielectric behavior suggest that the Bi<sub>2</sub>S<sub>3</sub> compound has suitable band gap and has potential to use for photovoltaic applications while Bi<sub>2</sub>A<sub>3</sub> (A = Se, Te) compounds could be used in infrared detectors and other optical devices. Calculated thermal properties reveal that the Bi<sub>2</sub>A<sub>3</sub> (A = S, Se, Te) chalcogenides could be potential materials for thermoelectric applications.</p></div>","PeriodicalId":430,"journal":{"name":"Solid State Communications","volume":"393 ","pages":"Article 115669"},"PeriodicalIF":2.1,"publicationDate":"2024-08-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142136960","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-24DOI: 10.1016/j.ssc.2024.115667
Rui-Zhou Zhang, Xiao-Hong Li , Hong-Ling Cui
Preadsorbing suitable gas molecule on the substrate can effectively improve the adsorption strength of the system. The adsorption properties of preadsorping NH3 on SO2-adsorbed Hf2CO2 monolayer are explored by first-principles calculation. All possible adsorption sites are considered. SO2 molecule cannot be adsorbed by Hf2CO2 monolayer, while preadsorbing NH3 can increase the adsorption strength of SO2-adsorbed Hf2CO2 monolayer. The adsorption system has the direct semiconductor character and is the reusable SO2 gas sensor because of short recovery time and the appropriate adsorption strength. Preadsorbing NH3 can decrease the carrier mobility in conduction band, but has little impact on the carrier mobility in valence band. The charge transfer of the co-adsorption system is also investigated.
{"title":"Effect of NH3 preadsorption on SO2 adsorption on Hf2CO2 MXene","authors":"Rui-Zhou Zhang, Xiao-Hong Li , Hong-Ling Cui","doi":"10.1016/j.ssc.2024.115667","DOIUrl":"10.1016/j.ssc.2024.115667","url":null,"abstract":"<div><p>Preadsorbing suitable gas molecule on the substrate can effectively improve the adsorption strength of the system. The adsorption properties of preadsorping NH<sub>3</sub> on SO<sub>2</sub>-adsorbed Hf<sub>2</sub>CO<sub>2</sub> monolayer are explored by first-principles calculation. All possible adsorption sites are considered. SO<sub>2</sub> molecule cannot be adsorbed by Hf<sub>2</sub>CO<sub>2</sub> monolayer, while preadsorbing NH<sub>3</sub> can increase the adsorption strength of SO<sub>2</sub>-adsorbed Hf<sub>2</sub>CO<sub>2</sub> monolayer. The adsorption system has the direct semiconductor character and is the reusable SO<sub>2</sub> gas sensor because of short recovery time and the appropriate adsorption strength. Preadsorbing NH<sub>3</sub> can decrease the carrier mobility in conduction band, but has little impact on the carrier mobility in valence band. The charge transfer of the co-adsorption system is also investigated.</p></div>","PeriodicalId":430,"journal":{"name":"Solid State Communications","volume":"392 ","pages":"Article 115667"},"PeriodicalIF":2.1,"publicationDate":"2024-08-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142076641","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-23DOI: 10.1016/j.ssc.2024.115665
Kejiang Fu , Jingjing Wu , Xin Tang
Porous Ag has good electron conductivity and is one of the typical oxygen reduction reaction(ORR) catalysts. In order to investigate the mechanism of porous Ag for ORR, the relaxed structure and detailed partial density of states are determined using density-functional theory. Among multiple possible active sites, the overpotential of porous Ag is 0.50 V, which is better than that of Ag (111) at 0.62 V. After doping Pt and Pd, the overpotentials are 0.47 V and 0.49 V, respectively. Furthermore, the introduction of a transition metal has led to changes in the charge distribution on the catalyst surface, which has resulted in improved catalytic performance. By investigating the synergistic effects between doped transition metals and ORR intermediates, this can facilitate the development of catalysts with higher activity and better stability.
多孔银具有良好的电子传导性,是典型的氧还原反应(ORR)催化剂之一。为了研究多孔银的氧还原反应机理,利用密度泛函理论确定了多孔银的弛豫结构和详细的部分态密度。在多种可能的活性位点中,多孔银的过电位为 0.50 V,优于 Ag (111) 的 0.62 V。此外,过渡金属的引入改变了催化剂表面的电荷分布,从而提高了催化性能。通过研究掺杂过渡金属与 ORR 中间体之间的协同效应,有助于开发出活性更高、稳定性更好的催化剂。
{"title":"A first principles study of the oxygen reduction reaction mechanism on porous Ag and Ag-TM nanostructure","authors":"Kejiang Fu , Jingjing Wu , Xin Tang","doi":"10.1016/j.ssc.2024.115665","DOIUrl":"10.1016/j.ssc.2024.115665","url":null,"abstract":"<div><p>Porous Ag has good electron conductivity and is one of the typical oxygen reduction reaction(ORR) catalysts. In order to investigate the mechanism of porous Ag for ORR, the relaxed structure and detailed partial density of states are determined using density-functional theory. Among multiple possible active sites, the overpotential of porous Ag is 0.50 V, which is better than that of Ag (111) at 0.62 V. After doping Pt and Pd, the overpotentials are 0.47 V and 0.49 V, respectively. Furthermore, the introduction of a transition metal has led to changes in the charge distribution on the catalyst surface, which has resulted in improved catalytic performance. By investigating the synergistic effects between doped transition metals and ORR intermediates, this can facilitate the development of catalysts with higher activity and better stability.</p></div>","PeriodicalId":430,"journal":{"name":"Solid State Communications","volume":"392 ","pages":"Article 115665"},"PeriodicalIF":2.1,"publicationDate":"2024-08-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142058440","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-23DOI: 10.1016/j.ssc.2024.115664
Tarik EL Hafi , Hicham Jabraoui , Omar Bajjou , M'hammed Mazroui , Youssef Lachtioui
This study employs molecular dynamics simulations using the embedded-atom method to investigate the structural and dynamic properties of supercooled liquid silver (Ag) metal under varying external hydrostatic pressures ranging from 0 to 70 GPa. The investigation spans various length scales, analyzing short-to-medium-range order, crystalline order, and fractal dimension to discern patterns that indicate how increased pressure affects atomic arrangements. The results suggest that increased external hydrostatic pressure triggers a shift to more ordered atomic structures characterized by relative atomic positions corresponding to the fcc lattice structure, highlighting the system's heightened sensitivity to pressure conditions. Furthermore, the study reveals pressure-dependent changes in atomic diffusion behavior and shows a reduction in atomic mobility with increasing pressure. In particular, the values of the diffusion coefficient decrease from 3.719 × 10−8 to 1.564 × 10−9 cm2 s−1 for 0 and 70 GPa, respectively, demonstrating the direct influence of pressure on the dynamics of supercooled liquid Ag metal.
{"title":"Exploring structural and dynamic characteristics of supercooled liquid silver under varying hydrostatic pressures: A molecular dynamics investigation","authors":"Tarik EL Hafi , Hicham Jabraoui , Omar Bajjou , M'hammed Mazroui , Youssef Lachtioui","doi":"10.1016/j.ssc.2024.115664","DOIUrl":"10.1016/j.ssc.2024.115664","url":null,"abstract":"<div><p>This study employs molecular dynamics simulations using the embedded-atom method to investigate the structural and dynamic properties of supercooled liquid silver (Ag) metal under varying external hydrostatic pressures ranging from 0 to 70 GPa. The investigation spans various length scales, analyzing short-to-medium-range order, crystalline order, and fractal dimension to discern patterns that indicate how increased pressure affects atomic arrangements. The results suggest that increased external hydrostatic pressure triggers a shift to more ordered atomic structures characterized by relative atomic positions corresponding to the fcc lattice structure, highlighting the system's heightened sensitivity to pressure conditions. Furthermore, the study reveals pressure-dependent changes in atomic diffusion behavior and shows a reduction in atomic mobility with increasing pressure. In particular, the values of the diffusion coefficient decrease from 3.719 × 10<sup>−8</sup> to 1.564 × 10<sup>−9</sup> cm<sup>2</sup> s<sup>−1</sup> for 0 and 70 GPa, respectively, demonstrating the direct influence of pressure on the dynamics of supercooled liquid Ag metal.</p></div>","PeriodicalId":430,"journal":{"name":"Solid State Communications","volume":"392 ","pages":"Article 115664"},"PeriodicalIF":2.1,"publicationDate":"2024-08-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142076642","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The research findings from a thorough examination of the impact of sintering temperature are presented in this publication on structural, ferroelectric, ferromagnetic and dielectric properties of Mg-doped Bismuth Ferrite. Bi0.88Mg0.12FeO3 (BMFO) was synthesized using a solid-state reaction technique and sintered at three different temperatures: 750 °C, 800 °C and 830 °C. Structural analysis was performed using Rietveld refinement of XRD data, which confirms the presence of perovskite phase with rhombohedral structure in all samples and also changes in lattice parameters that result from sintering temperature changes. The average crystalline size as well as the lattice strain are calculated using the Williamson-Hall method. The loss tangent and dielectric constant have been examined as a function of frequency revealing a considerable improvement in dielectric properties. SEM analysis was performed to identify the microstructural property of the samples. Ferroelectric properties were studied using a P-E loop which confirms the enhancement in the ferroelectric property as sintering temperature increases. The improvement in the multiferroic nature will be discussed in light of the sintering temperature effect on Mg-doped Bismuth Ferrite.
{"title":"Effect of sintering temperature on multiferroic properties of Mg-doped Bismuth Ferrite","authors":"Priya Prajapati, Kirti Bera, Renuka Pithiya, Devang Pandya, Akshay Lila, Thaker Amisha, Surojit Bera, Jahnviba Zala, Gautam Patadiya, P.V. Kanjariya","doi":"10.1016/j.ssc.2024.115656","DOIUrl":"10.1016/j.ssc.2024.115656","url":null,"abstract":"<div><p>The research findings from a thorough examination of the impact of sintering temperature are presented in this publication on structural, ferroelectric, ferromagnetic and dielectric properties of Mg-doped Bismuth Ferrite. Bi<sub>0.88</sub>Mg<sub>0.12</sub>FeO<sub>3</sub> (BMFO) was synthesized using a solid-state reaction technique and sintered at three different temperatures: 750 °C, 800 °C and 830 °C. Structural analysis was performed using Rietveld refinement of XRD data, which confirms the presence of perovskite phase with rhombohedral structure in all samples and also changes in lattice parameters that result from sintering temperature changes. The average crystalline size as well as the lattice strain are calculated using the Williamson-Hall method. The loss tangent and dielectric constant have been examined as a function of frequency revealing a considerable improvement in dielectric properties. SEM analysis was performed to identify the microstructural property of the samples. Ferroelectric properties were studied using a P-E loop which confirms the enhancement in the ferroelectric property as sintering temperature increases. The improvement in the multiferroic nature will be discussed in light of the sintering temperature effect on Mg-doped Bismuth Ferrite.</p></div>","PeriodicalId":430,"journal":{"name":"Solid State Communications","volume":"392 ","pages":"Article 115656"},"PeriodicalIF":2.1,"publicationDate":"2024-08-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142012877","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-15DOI: 10.1016/j.ssc.2024.115657
Akansha Thakur, Niladri Sarkar
The role of electron-phonon interaction in band gap shrinkage for some II-VI bulk and low-dimensional semiconductors is investigated in this work. The variation of the energy band gap is studied as a function of temperature using Varshni's, Vina's, and Passler's relations. It is observed that the change in the energy band gap is affected due to the quantum confinement as the dimensionality of these semiconductors is decreased.
{"title":"The effect of quantum confinement and the role of electron-phonon interaction on the band gap shrinkage of some II-VI semiconductors","authors":"Akansha Thakur, Niladri Sarkar","doi":"10.1016/j.ssc.2024.115657","DOIUrl":"10.1016/j.ssc.2024.115657","url":null,"abstract":"<div><p>The role of electron-phonon interaction in band gap shrinkage for some II-VI bulk and low-dimensional semiconductors is investigated in this work. The variation of the energy band gap is studied as a function of temperature using Varshni's, Vina's, and Passler's relations. It is observed that the change in the energy band gap is affected due to the quantum confinement as the dimensionality of these semiconductors is decreased.</p></div>","PeriodicalId":430,"journal":{"name":"Solid State Communications","volume":"392 ","pages":"Article 115657"},"PeriodicalIF":2.1,"publicationDate":"2024-08-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142021097","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-15DOI: 10.1016/j.ssc.2024.115658
Shyamsundar Ghosh
Impact of non-magnetic cationic-substitution on the evolution of structural defects and correlated ferromagnetic and electrical properties are investigated in series of pulsed laser deposited Sn1-xInxO2 (0.0 ≤ x ≤ 0.12) thin films. Beyond the nominal doping concentration of 2 at.% (i.e. x > 0.02), Indium (In)-doped SnO2 film switches to exhibit from n-type to p-type electrical conductivity and simultaneously the magnetization (MS) as well as the Curie temperature (TC) of the films increase significantly. Estimated values of ‘MS’ and ‘TC’ are found to achieve as large as 15.21 emu/cm3 and 540 K respectively when In-doping concentration approaches towards x = 0.08 and afterwards tend to decrease abruptly. Various spectroscopic techniques including Positron Annihilation Lifetime Spectroscopy (PALS) have detected the existence of Sn vacancy (VSn) defects within Sn1-xInxO2 films arise as the effect of In-substitution at Sn site (InSn) under O-rich atmosphere. The estimated positron lifetimes and the increase of line-shape S-parameter confirm the rise of VSn defects which serve as the major source of magnetic moments in non-magnetic host SnO2. Besides, InSn defects introduce excess holes within SnO2 lattice and thereby the magnetic spin-spin RKKY interaction between near-by VSn defects are mediated ferromagetically through the localized holes. For x > 0.08, stabilization of various donor-type defects such as Sn interstitial (Sni), indium interstitial (Ini) actually compensates the acceptors that leads to reduce the effective hole density consequently diminishing the strength of ferromagnetism within SnO2. Hence, tuning of such ferromagnetic and semiconducting properties through non-magnetic cationic substitution in transparent conducting oxides can be very promising in the field of next-generation spintronics.
在一系列脉冲激光沉积的 Sn1-xInxO2 (0.0 ≤ x ≤ 0.12) 薄膜中,研究了非磁性阳离子替代对结构缺陷演变以及相关铁磁性和电特性的影响。当标称掺杂浓度超过 2 at.%(即 x >0.02)时,掺铟二氧化锡薄膜的导电性会从 n 型转变为 p 型,同时薄膜的磁化率(MS)和居里温度(TC)也会显著增加。当铟掺杂浓度接近 x = 0.08 时,"MS "和 "TC "的估计值分别达到 15.21 emu/cm3 和 540 K,之后则骤然下降。包括正电子湮没寿命光谱(PALS)在内的各种光谱技术检测到 Sn1-xInxO2 薄膜中存在 Sn 空位(VSn)缺陷,这是由于在富 O 气氛下 Sn 位点(InSn)的 In 取代效应造成的。估算的正电子寿命和线形 S 参数的增加证实了 VSn 缺陷的增加,它是非磁性主 SnO2 中磁矩的主要来源。此外,InSn 缺陷在 SnO2 晶格中引入了过剩的空穴,因此近邻 VSn 缺陷之间的磁性自旋-自旋 RKKY 相互作用通过局部空穴以铁磁方式介导。当 x > 0.08 时,各种供体型缺陷(如锡间隙(Sni)、铟间隙(Ini))的稳定实际上补偿了受体,导致有效空穴密度降低,从而减弱了二氧化锡内部的铁磁性强度。因此,通过透明导电氧化物中的非磁性阳离子取代来调整这种铁磁性和半导体特性,在下一代自旋电子学领域大有可为。
{"title":"Impact of evolution of structural defects on the ferromagnetic and electrical properties of laser deposited Indium-doped SnO2 thin films","authors":"Shyamsundar Ghosh","doi":"10.1016/j.ssc.2024.115658","DOIUrl":"10.1016/j.ssc.2024.115658","url":null,"abstract":"<div><p>Impact of non-magnetic cationic-substitution on the evolution of structural defects and correlated ferromagnetic and electrical properties are investigated in series of pulsed laser deposited Sn<sub>1-x</sub>In<sub>x</sub>O<sub>2</sub> (0.0 ≤ x ≤ 0.12) thin films. Beyond the nominal doping concentration of 2 at.% (i.e. x > 0.02), Indium (In)-doped SnO<sub>2</sub> film switches to exhibit from n-type to p-type electrical conductivity and simultaneously the magnetization (<em>M</em><sub>S</sub>) as well as the Curie temperature (<em>T</em><sub>C</sub>) of the films increase significantly. Estimated values of ‘<em>M</em><sub>S</sub>’ and ‘<em>T</em><sub>C</sub>’ are found to achieve as large as 15.21 emu/cm<sup>3</sup> and 540 K respectively when In-doping concentration approaches towards x = 0.08 and afterwards tend to decrease abruptly. Various spectroscopic techniques including Positron Annihilation Lifetime Spectroscopy (PALS) have detected the existence of Sn vacancy (<em>V</em><sub>Sn</sub>) defects within Sn<sub>1-x</sub>In<sub>x</sub>O<sub>2</sub> films arise as the effect of In-substitution at Sn site (<em>In</em><sub>Sn</sub>) under O-rich atmosphere. The estimated positron lifetimes and the increase of line-shape <em>S</em>-parameter confirm the rise of <em>V</em><sub><em>Sn</em></sub> defects which serve as the major source of magnetic moments in non-magnetic host SnO<sub>2</sub>. Besides, <em>In</em><sub>Sn</sub> defects introduce excess holes within SnO<sub>2</sub> lattice and thereby the magnetic spin-spin RKKY interaction between near-by <em>V</em><sub>Sn</sub> defects are mediated ferromagetically through the localized holes. For x > 0.08, stabilization of various donor-type defects such as Sn interstitial (<em>Sn</em><sub>i</sub>), indium interstitial (<em>In</em><sub><em>i</em></sub>) actually compensates the acceptors that leads to reduce the effective hole density consequently diminishing the strength of ferromagnetism within SnO<sub>2</sub>. Hence, tuning of such ferromagnetic and semiconducting properties through non-magnetic cationic substitution in transparent conducting oxides can be very promising in the field of next-generation spintronics.</p></div>","PeriodicalId":430,"journal":{"name":"Solid State Communications","volume":"392 ","pages":"Article 115658"},"PeriodicalIF":2.1,"publicationDate":"2024-08-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142012878","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Nowadays, double perovskites for renewable energy are emerging materials because of their interesting properties such as simple and stable crystal structure. In our study, we theoretically explored the optoelectronic along with mechanical and thermoelectric characteristics of A2InAsO6 (A = Sr, Ba) using density functional theory and semi-classical Boltzmann theory followed by WIEN2k code. The thermodynamic and structural stabilities are determined based on the cohesive energy, enthalpy of formation and tolerance factor. The ductile and brittle behaviour has been checked by Pugh's ratios. The measured values of narrow direct energy band gaps are 0.70 eV for Sr2InAsO6, and 0.18 eV for Ba2InAsO6 with TB-mBJ approximation. These compositions are potentially used in optoelectronic applications because their electronic characteristics are tuneable. In the energy range 0–12 eV, the compositions under consideration exhibit a single-peaked response while the replacement of cation Sr with Ba caused a shift in optical structures towards lower energies. These compositions are also suitable for thermoelectric systems as they possess high values of the figure of merits at room temperature and the measured values 0.049 eV for Sr2InAsO6, and 0.10 eV for Ba2InSbO6 are recorded.
如今,用于可再生能源的双过氧化物因其简单稳定的晶体结构等有趣的特性而成为新兴材料。在我们的研究中,我们使用密度泛函理论和半经典玻尔兹曼理论以及 WIEN2k 代码,从理论上探讨了 A2InAsO6(A = Sr、Ba)的光电特性以及机械和热电特性。根据内聚能、形成焓和容限因子确定了热力学和结构稳定性。韧性和脆性行为已通过 Pugh 比率进行了检验。根据 TB-mBJ 近似法,Sr2InAsO6 的窄直接能带隙测量值为 0.70 eV,Ba2InAsO6 为 0.18 eV。由于这些成分的电子特性是可调的,因此可用于光电应用。在 0-12 eV 的能量范围内,所考虑的成分表现出单峰响应,而用 Ba 取代阳离子 Sr 会导致光学结构向低能量方向移动。这些成分也适用于热电系统,因为它们在室温下具有较高的优点值,Sr2InAsO6 的测量值为 0.049 eV,Ba2InSbO6 的测量值为 0.10 eV。
{"title":"Exploring the physical properties of novel double perovskites A2InAsO6 (A=Sr, Ba) for renewable energy applications: Ab-initio calculations","authors":"Anjali Kumari , Jisha Annie Abraham , Mumtaz Manzoor , Abhishek Kumar Mishra , Ayman A. Ghfar , Yedluri Anil Kumar , Ramesh Sharma","doi":"10.1016/j.ssc.2024.115654","DOIUrl":"10.1016/j.ssc.2024.115654","url":null,"abstract":"<div><p>Nowadays, double perovskites for renewable energy are emerging materials because of their interesting properties such as simple and stable crystal structure. In our study, we theoretically explored the optoelectronic along with mechanical and thermoelectric characteristics of A<sub>2</sub>InAsO<sub>6</sub> (A = Sr, Ba) using density functional theory and semi-classical Boltzmann theory followed by WIEN2k code. The thermodynamic and structural stabilities are determined based on the cohesive energy, enthalpy of formation and tolerance factor. The ductile and brittle behaviour has been checked by Pugh's ratios. The measured values of narrow direct energy band gaps are 0.70 eV for Sr<sub>2</sub>InAsO<sub>6</sub>, and 0.18 eV for Ba<sub>2</sub>InAsO<sub>6</sub> with TB-mBJ approximation. These compositions are potentially used in optoelectronic applications because their electronic characteristics are tuneable. In the energy range 0–12 eV, the compositions under consideration exhibit a single-peaked response while the replacement of cation Sr with Ba caused a shift in optical structures towards lower energies. These compositions are also suitable for thermoelectric systems as they possess high values of the figure of merits at room temperature and the measured values 0.049 eV for Sr<sub>2</sub>InAsO<sub>6</sub>, and 0.10 eV for Ba<sub>2</sub>InSbO<sub>6</sub> are recorded.</p></div>","PeriodicalId":430,"journal":{"name":"Solid State Communications","volume":"392 ","pages":"Article 115654"},"PeriodicalIF":2.1,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142076651","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}