Pub Date : 2026-01-23DOI: 10.1016/j.physb.2026.418315
Xingliang Wang , Juchuan Chai , Qiaogang Song , Xinghuan Hu , Chi Yang , Shuying Liao , Yi Huang , Xiaoge Zhang , Shurong Wang
Silver nanoparticles (Ag NPs) possess distinctive characteristics including low resonant losses, minimal parasitic absorption, high specific surface area, and significant surface activity. This study presents an interfacial modification technique utilizing Ag NPs to improve the performance of Cu2ZnSn(S,Se)4(CZTSSe) thin-film solar cells. All devices incorporating Ag NPs exhibited enhanced efficiency, attributable to the light-scattering properties of the NPs that boost photon absorption in the CZTSSe layer, combined with near-field effects that improve the dissociation and collection of photo-generated charge carriers. Notably, the device modified with Ag NPs from a 10 nm Ag layer showed an efficiency increase from 10.2 % to 11.7 %, with the short-circuit current density rising from 37.16 mA/cm2 to 40.41 mA/cm2 and the open-circuit voltage increasing from 467.2 mV to 496.4 mV. This Ag NP-based interfacial modification approach provides a promising pathway for enhancing CZTSSe thin-film photovoltaic devices.
{"title":"Research on the influence of interfacial modification with silver nanoparticles on kesterite thin-film solar cells","authors":"Xingliang Wang , Juchuan Chai , Qiaogang Song , Xinghuan Hu , Chi Yang , Shuying Liao , Yi Huang , Xiaoge Zhang , Shurong Wang","doi":"10.1016/j.physb.2026.418315","DOIUrl":"10.1016/j.physb.2026.418315","url":null,"abstract":"<div><div>Silver nanoparticles (Ag NPs) possess distinctive characteristics including low resonant losses, minimal parasitic absorption, high specific surface area, and significant surface activity. This study presents an interfacial modification technique utilizing Ag NPs to improve the performance of Cu<sub>2</sub>ZnSn(S,Se)<sub>4</sub>(CZTSSe) thin-film solar cells. All devices incorporating Ag NPs exhibited enhanced efficiency, attributable to the light-scattering properties of the NPs that boost photon absorption in the CZTSSe layer, combined with near-field effects that improve the dissociation and collection of photo-generated charge carriers. Notably, the device modified with Ag NPs from a 10 nm Ag layer showed an efficiency increase from 10.2 % to 11.7 %, with the short-circuit current density rising from 37.16 mA/cm<sup>2</sup> to 40.41 mA/cm<sup>2</sup> and the open-circuit voltage increasing from 467.2 mV to 496.4 mV. This Ag NP-based interfacial modification approach provides a promising pathway for enhancing CZTSSe thin-film photovoltaic devices.</div></div>","PeriodicalId":20116,"journal":{"name":"Physica B-condensed Matter","volume":"727 ","pages":"Article 418315"},"PeriodicalIF":2.8,"publicationDate":"2026-01-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146081275","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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 : 2026-01-23DOI: 10.1016/j.physb.2026.418271
Dung Nguyen Trong , Tuan Tran Quoc , Ştefan Ţălu
This study investigates the effects of compositional and thermal factors on the structural properties, phase transitions, and glass transition temperature of Ga1-xInx alloys (x = 0.2, 0.4, 0.5, 0.6, 0.8) using simulation methods. At 300 K, the calculated bond lengths for Ga–Ga, Ga–In, and In–In pairs are approximately 3.25 Å, 3.15 Å, and 3.05 Å, respectively. As the temperature decreases from 300 K to 4 K and the indium concentration increases from 20 % to 80 %, the total number of atoms in the system rises from 5,324 to 27,436. Despite these changes, the average bond length remains relatively stable, fluctuating around 3.15 Å. However, the total bonding energy of the system decreases significantly, contributing to an overall increase in structural smoothness and stability of the alloy. Furthermore, the glass transition temperature (Tg) of the GaIn alloy was determined to be approximately 188 K. These findings offer valuable insights into the temperature- and composition-dependent behavior of GaIn alloys and provide a theoretical foundation for their optimization in advanced semiconductor device applications.
{"title":"Simulation study of structural, phase transition, and glass transition behavior in Ga1-xInx alloys (x = 0.2–0.8)","authors":"Dung Nguyen Trong , Tuan Tran Quoc , Ştefan Ţălu","doi":"10.1016/j.physb.2026.418271","DOIUrl":"10.1016/j.physb.2026.418271","url":null,"abstract":"<div><div>This study investigates the effects of compositional and thermal factors on the structural properties, phase transitions, and glass transition temperature of Ga<sub>1-x</sub>In<sub>x</sub> alloys (x = 0.2, 0.4, 0.5, 0.6, 0.8) using simulation methods. At 300 K, the calculated bond lengths for Ga–Ga, Ga–In, and In–In pairs are approximately 3.25 Å, 3.15 Å, and 3.05 Å, respectively. As the temperature decreases from 300 K to 4 K and the indium concentration increases from 20 % to 80 %, the total number of atoms in the system rises from 5,324 to 27,436. Despite these changes, the average bond length remains relatively stable, fluctuating around 3.15 Å. However, the total bonding energy of the system decreases significantly, contributing to an overall increase in structural smoothness and stability of the alloy. Furthermore, the glass transition temperature (T<sub>g</sub>) of the GaIn alloy was determined to be approximately 188 K. These findings offer valuable insights into the temperature- and composition-dependent behavior of GaIn alloys and provide a theoretical foundation for their optimization in advanced semiconductor device applications.</div></div>","PeriodicalId":20116,"journal":{"name":"Physica B-condensed Matter","volume":"727 ","pages":"Article 418271"},"PeriodicalIF":2.8,"publicationDate":"2026-01-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146081195","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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}
In this study, Ga2O3 doped ZnO-MnO2-SrCO3-based linear resistors were prepared through a sintering process at 1320 °C. The impacts of Ga2O3 doping on the microstructure and electrical properties of the ZnO-based linear resistors were systematically investigated. The results show that doping with a moderate amount of Ga2O3 promotes the growth of ZnO grains, effectively reduces the nonlinear coefficient of resistors and enhances the resistance frequency stability. It also enables the resistivity of the resistors to be adjusted over a wide range. The nonlinear coefficient (α) of the resistor reaches 1.0 when 0.3 mol% Ga2O3 is doped. The resistivity (ρ) reaches the smallest value of 855.31 Ω cm when the 0.5 mol% Ga2O3 is doped. It is about 98.6 % lower than the value at a doping concentration of 0.1 mol% Ga2O3. The doping of Ga2O3 not only improves the linearity of ZnO-based resistors, but also reduces their resistivity to some extent.
{"title":"Impact of Ga2O3 doping on microstructure and electrical properties of novel ZnO-MnO2-SrCO3-based linear resistors","authors":"Xuefang Chen , Lingru Meng , Yunong Liao , Weiqi Zhang , Jinyi Wu , Ruiqing Chu , Zhijun Xu","doi":"10.1016/j.physb.2026.418314","DOIUrl":"10.1016/j.physb.2026.418314","url":null,"abstract":"<div><div>In this study, Ga<sub>2</sub>O<sub>3</sub> doped ZnO-MnO<sub>2</sub>-SrCO<sub>3</sub>-based linear resistors were prepared through a sintering process at 1320 °C. The impacts of Ga<sub>2</sub>O<sub>3</sub> doping on the microstructure and electrical properties of the ZnO-based linear resistors were systematically investigated. The results show that doping with a moderate amount of Ga<sub>2</sub>O<sub>3</sub> promotes the growth of ZnO grains, effectively reduces the nonlinear coefficient of resistors and enhances the resistance frequency stability. It also enables the resistivity of the resistors to be adjusted over a wide range. The nonlinear coefficient (α) of the resistor reaches 1.0 when 0.3 mol% Ga<sub>2</sub>O<sub>3</sub> is doped. The resistivity (ρ) reaches the smallest value of 855.31 Ω cm when the 0.5 mol% Ga<sub>2</sub>O<sub>3</sub> is doped. It is about 98.6 % lower than the value at a doping concentration of 0.1 mol% Ga<sub>2</sub>O<sub>3</sub>. The doping of Ga<sub>2</sub>O<sub>3</sub> not only improves the linearity of ZnO-based resistors, but also reduces their resistivity to some extent.</div></div>","PeriodicalId":20116,"journal":{"name":"Physica B-condensed Matter","volume":"727 ","pages":"Article 418314"},"PeriodicalIF":2.8,"publicationDate":"2026-01-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146081200","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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 : 2026-01-22DOI: 10.1016/j.physb.2026.418309
Sanober Kanwal , Ahsan Illahi , Amna Nasir , Asif Nawaz Khan , M. Anis-ur-Rehman , Muhammad Kaleem
Perovskite oxides have been extensively studied for optoelectronic applications because of their flexible structure. In this work utilizing the FP-LAPW method in the Wien2K code to examine the double perovskites Na2ReXO6 (X = Al, In) for efficient energy harvesting devices. The structures were relaxed using Perdew-Burke-Ernzerhof (PBE) method's Generalized Gradient Approximation (GGA) and the Tran-Blaha modified Becke-Johnson (TB-mBJ) scheme was employed for accurate electronic properties. Both compounds are structurally and thermodynamically stable, and thermal stability of both compounds was demonstrated through AIMD simulations. These compounds exhibit mechanical stability and the absence of negative frequencies in the phonon dispersion curves confirms their dynamically stability. Analysis of the band structure revealed that the Na2ReXO6 (X = Al, In) perovskites exhibit direct bandgap of 1.243 eV and 1.741 eV respectively. Additionally, significant dielectric response and high absorption coefficients of Na2ReXO6 (X = Al, In) make these compounds optically active in the visible spectrum suggesting their potential for energy harvesting.
{"title":"DFT and AIMD insights into the photo-excited stability of Na2ReXO6 (X=Al, In) perovskites for efficient energy harvesting","authors":"Sanober Kanwal , Ahsan Illahi , Amna Nasir , Asif Nawaz Khan , M. Anis-ur-Rehman , Muhammad Kaleem","doi":"10.1016/j.physb.2026.418309","DOIUrl":"10.1016/j.physb.2026.418309","url":null,"abstract":"<div><div>Perovskite oxides have been extensively studied for optoelectronic applications because of their flexible structure. In this work utilizing the FP-LAPW method in the Wien2K code to examine the double perovskites Na<sub>2</sub>ReXO<sub>6</sub> (X = Al, In) for efficient energy harvesting devices. The structures were relaxed using Perdew-Burke-Ernzerhof (PBE) method's Generalized Gradient Approximation (GGA) and the Tran-Blaha modified Becke-Johnson (TB-mBJ) scheme was employed for accurate electronic properties. Both compounds are structurally and thermodynamically stable, and thermal stability of both compounds was demonstrated through AIMD simulations. These compounds exhibit mechanical stability and the absence of negative frequencies in the phonon dispersion curves confirms their dynamically stability. Analysis of the band structure revealed that the Na<sub>2</sub>ReXO<sub>6</sub> (X = Al, In) perovskites exhibit direct bandgap of 1.243 eV and 1.741 eV respectively. Additionally, significant dielectric response and high absorption coefficients of Na<sub>2</sub>ReXO<sub>6</sub> (X = Al, In) make these compounds optically active in the visible spectrum suggesting their potential for energy harvesting.</div></div>","PeriodicalId":20116,"journal":{"name":"Physica B-condensed Matter","volume":"727 ","pages":"Article 418309"},"PeriodicalIF":2.8,"publicationDate":"2026-01-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146081274","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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 : 2026-01-21DOI: 10.1016/j.physb.2026.418310
Guochu Deng
We systematically investigated crystal-field (CF) excitations of Kramers (Nd3+, Er3+, Yb3+) and non-Kramers (Pr3+, Ho3+) rare-earth ions in REFeO3 using optimized CF simulations. Internal magnetic fields from the Fe3+ and RE3+ sublattices split the ground-state doublets of all Kramers ions, generating low-energy excitations around 1 meV. In non-Kramers systems, low-energy excitations arise only when the ground state forms an accidental pseudo-doublet, as observed for Ho3+ in HoFeO3; such pseudo-doublets exhibit field-induced splitting analogous to Kramers ions. In contrast, true singlet ground states, exemplified by Pr3+, show no zero-field splitting. Strong anisotropies are found in both internal- and external-field responses of the CF excitations in these REFeO3. These results provide a unified explanation for the anomalous Zeeman splitting of CF ground states in REFeO3.
{"title":"Internal and external field effects upon crystal field excitations in REFeO3 (RE = Nd3+, Er3+, Yb3+, Pr3+, and Ho3+)","authors":"Guochu Deng","doi":"10.1016/j.physb.2026.418310","DOIUrl":"10.1016/j.physb.2026.418310","url":null,"abstract":"<div><div>We systematically investigated crystal-field (CF) excitations of Kramers (Nd<sup>3+</sup>, Er<sup>3+</sup>, Yb<sup>3+</sup>) and non-Kramers (Pr<sup>3+</sup>, Ho<sup>3+</sup>) rare-earth ions in REFeO<sub>3</sub> using optimized CF simulations. Internal magnetic fields from the Fe<sup>3+</sup> and RE<sup>3+</sup> sublattices split the ground-state doublets of all Kramers ions, generating low-energy excitations around 1 meV. In non-Kramers systems, low-energy excitations arise only when the ground state forms an accidental pseudo-doublet, as observed for Ho<sup>3+</sup> in HoFeO<sub>3</sub>; such pseudo-doublets exhibit field-induced splitting analogous to Kramers ions. In contrast, true singlet ground states, exemplified by Pr<sup>3+</sup>, show no zero-field splitting. Strong anisotropies are found in both internal- and external-field responses of the CF excitations in these REFeO<sub>3</sub>. These results provide a unified explanation for the anomalous Zeeman splitting of CF ground states in REFeO<sub>3</sub>.</div></div>","PeriodicalId":20116,"journal":{"name":"Physica B-condensed Matter","volume":"726 ","pages":"Article 418310"},"PeriodicalIF":2.8,"publicationDate":"2026-01-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146038237","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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 : 2026-01-21DOI: 10.1016/j.physb.2026.418312
B.N. Varalakshmi , Raveendra Kiran M , Hidayath Ulla
Efficient charge injection and balanced carrier recombination are critical for optimizing OLED performance. This study systematically investigates how the thickness of the electron-accepting interlayer F4TCNQ at the ITO/α-NPD interface governs hole-injection energetics and device efficiency. Devices with configuration ITO/F4TCNQ (0–8 nm)/α-NPD/Alq3/TPBi/LiF/Al were fabricated to examine thickness-dependent modulation of energy alignment and charge dynamics. Controlled F4TCNQ coverage enhances hole injection by tuning the anode work function via surface charge transfer and interfacial dipole formation. An optimal 6 nm interlayer yields a threefold enhancement in current, power, and external quantum efficiencies (4.89 cd A−1, 3.39 lm W−1, and 3.21 %). Thicker layers (>6 nm) induce resistive and non-radiative losses, reducing performance. These findings elucidate the relationship between interfacial dipoles, tunnelling-limited injection, and carrier balance, offering a generalizable approach to molecular-level energy-level engineering for high-efficiency OLEDs.
高效的电荷注入和平衡的载流子复合是优化OLED性能的关键。本研究系统地研究了ITO/α-NPD界面上电子接受层F4TCNQ的厚度对空穴注入能量和器件效率的影响。制备了ITO/F4TCNQ (0-8 nm)/α-NPD/Alq3/TPBi/LiF/Al结构的器件,研究了能量取向和电荷动力学的厚度依赖性调制。可控的F4TCNQ覆盖范围通过表面电荷转移和界面偶极子形成调节阳极功函数来增强空穴注入。最佳的6 nm中间层在电流、功率和外部量子效率方面提高了三倍(4.89 cd a−1,3.39 lm W−1和3.21%)。较厚的层(> 6nm)会导致电阻和非辐射损耗,从而降低性能。这些发现阐明了界面偶极子、隧道限制注入和载流子平衡之间的关系,为高效oled的分子能级工程提供了一种可推广的方法。
{"title":"Exploring F4TCNQ-Induced interlayer modulation of energy alignment and charge dynamics in OLEDs: Initial studies","authors":"B.N. Varalakshmi , Raveendra Kiran M , Hidayath Ulla","doi":"10.1016/j.physb.2026.418312","DOIUrl":"10.1016/j.physb.2026.418312","url":null,"abstract":"<div><div>Efficient charge injection and balanced carrier recombination are critical for optimizing OLED performance. This study systematically investigates how the thickness of the electron-accepting interlayer F<sub>4</sub>TCNQ at the ITO/α-NPD interface governs hole-injection energetics and device efficiency. Devices with configuration ITO/F<sub>4</sub>TCNQ (0–8 nm)/α-NPD/Alq<sub>3</sub>/TPBi/LiF/Al were fabricated to examine thickness-dependent modulation of energy alignment and charge dynamics. Controlled F<sub>4</sub>TCNQ coverage enhances hole injection by tuning the anode work function via surface charge transfer and interfacial dipole formation. An optimal 6 nm interlayer yields a threefold enhancement in current, power, and external quantum efficiencies (4.89 cd A<sup>−1</sup>, 3.39 lm W<sup>−1</sup>, and 3.21 %). Thicker layers (>6 nm) induce resistive and non-radiative losses, reducing performance. These findings elucidate the relationship between interfacial dipoles, tunnelling-limited injection, and carrier balance, offering a generalizable approach to molecular-level energy-level engineering for high-efficiency OLEDs.</div></div>","PeriodicalId":20116,"journal":{"name":"Physica B-condensed Matter","volume":"726 ","pages":"Article 418312"},"PeriodicalIF":2.8,"publicationDate":"2026-01-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146038236","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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 : 2026-01-21DOI: 10.1016/j.physb.2026.418299
Vinola Johnson , Vinitha G , Sathish S , M. Tamilelakkiya , T.C. Sabari Girisun , Thiyagarajan M
The Nonlinear Optical properties (NLO) of the PVA/CMC loaded with Lanthanum Praseodymium Aluminate (LaPrAlO3) nanoparticles was investigated via the Z scan setup at Q-switched Nd:YAG laser (i.e) at 532 nm excitation at nanosecond regime. An excellent improvement is noticed in the NLO characteristics of the filler integrated polymer nanocomposites has been reported in comparison to the individual nanofillers. Further the nanofillers exhibits Saturable absorption whereas on integrating it within the polymer matrix it exhibits the features of Reverse Saturable Absorption. This improved NLO features is due to the complex energy band structures that are formed during the synthesis that promote resonant transition to the conduction band via Surface Plasmon Resonance (SPR). Therefore, the RSA observed in the polymer nanocomposites is highly attributed to the Optical Limiting ability of the nanocomposite. This NLO properties are supported and proved through the structural, Vibrational, thermal and linear optical properties.
{"title":"Third order nonlinear optical properties of polymer-perovskite nanocomposites for optical limiter","authors":"Vinola Johnson , Vinitha G , Sathish S , M. Tamilelakkiya , T.C. Sabari Girisun , Thiyagarajan M","doi":"10.1016/j.physb.2026.418299","DOIUrl":"10.1016/j.physb.2026.418299","url":null,"abstract":"<div><div>The Nonlinear Optical properties (NLO) of the PVA/CMC loaded with Lanthanum Praseodymium Aluminate (LaPrAlO<sub>3</sub>) nanoparticles was investigated via the Z scan setup at Q-switched Nd:YAG laser (i.e) at 532 nm excitation at nanosecond regime. An excellent improvement is noticed in the NLO characteristics of the filler integrated polymer nanocomposites has been reported in comparison to the individual nanofillers. Further the nanofillers exhibits Saturable absorption whereas on integrating it within the polymer matrix it exhibits the features of Reverse Saturable Absorption. This improved NLO features is due to the complex energy band structures that are formed during the synthesis that promote resonant transition to the conduction band via Surface Plasmon Resonance (SPR). Therefore, the RSA observed in the polymer nanocomposites is highly attributed to the Optical Limiting ability of the nanocomposite. This NLO properties are supported and proved through the structural, Vibrational, thermal and linear optical properties.</div></div>","PeriodicalId":20116,"journal":{"name":"Physica B-condensed Matter","volume":"727 ","pages":"Article 418299"},"PeriodicalIF":2.8,"publicationDate":"2026-01-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146081193","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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}
In response to the growing demand for efficient room-temperature gas sensors, this study explores the fabrication and characterization of ZnO nanostructured thin films (NTFs) and CuO/ZnO bilayer nanocomposite thin films (NCTFs) using a cost-effective thermal spray pyrolysis technique. Comprehensive analyses, including XRD with Rietveld refinement, FESEM, and UV–Vis spectroscopy, confirmed the crystalline phases, morphology, and optical properties of the films. ZnO films exhibited uniform nanoscale particles with 43.5 % porosity and a band gap of 3.12 eV, while CuO/ZnO films showed larger grains and a wider band gap of 3.85 eV. Gas sensing tests at 303 K revealed that ZnO films offered higher ethanol sensing responses with response and recovery times of 603 s and 217 s, respectively. ZnO thin films are highly suitable for room-temperature gas-sensing applications, whereas CuO/ZnO composite films exhibit superior performance with faster response (474 s) and recovery (225 s) times.
{"title":"ZnO and CuO/ZnO nanostructured thin films via thermal spray pyrolysis for ethanol sensing at room temperature: A cost-effective approach","authors":"Tusar Saha , Selina Akter Lucky , Mehnaz Sharmin , Jiban Podder","doi":"10.1016/j.physb.2026.418300","DOIUrl":"10.1016/j.physb.2026.418300","url":null,"abstract":"<div><div>In response to the growing demand for efficient room-temperature gas sensors, this study explores the fabrication and characterization of ZnO nanostructured thin films (NTFs) and CuO/ZnO bilayer nanocomposite thin films (NCTFs) using a cost-effective thermal spray pyrolysis technique. Comprehensive analyses, including XRD with Rietveld refinement, FESEM, and UV–Vis spectroscopy, confirmed the crystalline phases, morphology, and optical properties of the films. ZnO films exhibited uniform nanoscale particles with 43.5 % porosity and a band gap of 3.12 eV, while CuO/ZnO films showed larger grains and a wider band gap of 3.85 eV. Gas sensing tests at 303 K revealed that ZnO films offered higher ethanol sensing responses with response and recovery times of 603 s and 217 s, respectively. ZnO thin films are highly suitable for room-temperature gas-sensing applications, whereas CuO/ZnO composite films exhibit superior performance with faster response (474 s) and recovery (225 s) times.</div></div>","PeriodicalId":20116,"journal":{"name":"Physica B-condensed Matter","volume":"727 ","pages":"Article 418300"},"PeriodicalIF":2.8,"publicationDate":"2026-01-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146081197","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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 : 2026-01-20DOI: 10.1016/j.physb.2026.418307
Jia-Wang Tan, Zi-Song Zhang, Ren Wen, Jia-Jian He, Yi-Bo Zhou, Xiaoqing Deng, Lin Sun
In recent decades, wide bandgap semiconductors have attracted considerable attention due to their unique electrical properties. This study focuses on two such materials, SiC and Ga2S3, and employs the generalized lattice matching (GLM) approach to construct two van der Waals heterostructures. Computational results indicate that both heterojunctions exhibit type II band alignment with different band gaps, 1.55 (2.13) eV for M1 and 0.55 (0.93) eV for M2 with PBE (HSE06) methods. The electronic properties of the heterojunctions, including bandgap magnitude (Eg), direct/indirect nature, and band alignment type (type II or type I), can be efficiently modulated through applied electric fields and vertical strain, enabling dynamic control over their functional behavior. Additionally, the heterojunction exhibits a high optical absorption coefficient exceeding 105 and achieves a photoconversion efficiency of 21.11 %, while also satisfying the thermodynamic requirements for photocatalytic water splitting at pH = 0. These outstanding attributes underscore its strong potential for applications in photocatalytic water splitting, energy conversion, and storage, positioning it as a promising candidate material for high-performance optoelectronic devices and efficient photocatalysts.
{"title":"SiC/Ga2S3 heterostructures: A versatile platform for high-efficiency photovoltaics and photodetection","authors":"Jia-Wang Tan, Zi-Song Zhang, Ren Wen, Jia-Jian He, Yi-Bo Zhou, Xiaoqing Deng, Lin Sun","doi":"10.1016/j.physb.2026.418307","DOIUrl":"10.1016/j.physb.2026.418307","url":null,"abstract":"<div><div>In recent decades, wide bandgap semiconductors have attracted considerable attention due to their unique electrical properties. This study focuses on two such materials, SiC and Ga<sub>2</sub>S<sub>3</sub>, and employs the generalized lattice matching (GLM) approach to construct two van der Waals heterostructures. Computational results indicate that both heterojunctions exhibit type II band alignment with different band gaps, 1.55 (2.13) eV for M1 and 0.55 (0.93) eV for M2 with PBE <strong>(</strong>HSE06) methods. The electronic properties of the heterojunctions, including bandgap magnitude (E<sub>g</sub>), direct/indirect nature, and band alignment type (type II or type I), can be efficiently modulated through applied electric fields and vertical strain, enabling dynamic control over their functional behavior. Additionally, the heterojunction exhibits a high optical absorption coefficient exceeding 10<sup>5</sup> and achieves a photoconversion efficiency of 21.11 %, while also satisfying the thermodynamic requirements for photocatalytic water splitting at pH = 0. These outstanding attributes underscore its strong potential for applications in photocatalytic water splitting, energy conversion, and storage, positioning it as a promising candidate material for high-performance optoelectronic devices and efficient photocatalysts.</div></div>","PeriodicalId":20116,"journal":{"name":"Physica B-condensed Matter","volume":"727 ","pages":"Article 418307"},"PeriodicalIF":2.8,"publicationDate":"2026-01-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146081202","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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}
Here, the electronic, optical and thermoelectric transport properties are studied using DFT for the bulk and the monolayer α-In2Se3. The electronic bandgap is observed to be 1.36 eV for the monolayer and 1.25 eV for the bulk α-In2Se3 using HSE06 hybrid functional. The optical properties such as the dielectric constant, absorption coefficient, refractive index, birefringence, reflectivity, energy loss functions and optical conductivity were also studied for the bulk and the monolayer of α-In2Se3. It was also observed that bulk α-In2Se3 exhibits a Seebeck coefficient of 850 μV/K and 1056 μV/K for monolayer α-In2Se3 at 300 K indicating it as a potential room temperature layered thermoelectric material. Further, the electronic part of figure of merit, ZTe found to reach 103 for monolayer α-In2Se3 and 104 for bulk α-In2Se3 at 300 K. Further, the total figure of merit, ZT was found to be 1.64 for the n-type monolayer α-In2Se3 at 300 K. The present work highlights the promising application of α-In2Se3 in next generation sub-nm scale optoelectronic and thermoelectric devices.
{"title":"Investigation of layer-dependent electronic, optical and thermoelectric transport properties of α-In2Se3 based on first principles calculations","authors":"Chanchal Jeengar , Tahir Ahmad , Kajal Jindal , Anjali Sharma , Sonia Chahar Srivastava , Monika Tomar , Pradip Kumar Jha","doi":"10.1016/j.physb.2026.418308","DOIUrl":"10.1016/j.physb.2026.418308","url":null,"abstract":"<div><div>Here, the electronic, optical and thermoelectric transport properties are studied using DFT for the bulk and the monolayer α-In<sub>2</sub>Se<sub>3</sub>. The electronic bandgap is observed to be 1.36 eV for the monolayer and 1.25 eV for the bulk α-In<sub>2</sub>Se<sub>3</sub> using HSE06 hybrid functional. The optical properties such as the dielectric constant, absorption coefficient, refractive index, birefringence, reflectivity, energy loss functions and optical conductivity were also studied for the bulk and the monolayer of α-In<sub>2</sub>Se<sub>3</sub>. It was also observed that bulk α-In<sub>2</sub>Se<sub>3</sub> exhibits a Seebeck coefficient of 850 μV/K and 1056 μV/K for monolayer α-In<sub>2</sub>Se<sub>3</sub> at 300 K indicating it as a potential room temperature layered thermoelectric material. Further, the electronic part of figure of merit, ZT<sub>e</sub> found to reach 103 for monolayer α-In<sub>2</sub>Se<sub>3</sub> and 104 for bulk α-In<sub>2</sub>Se<sub>3</sub> at 300 K. Further, the total figure of merit, ZT was found to be 1.64 for the n-type monolayer α-In<sub>2</sub>Se<sub>3</sub> at 300 K. The present work highlights the promising application of α-In<sub>2</sub>Se<sub>3</sub> in next generation sub-nm scale optoelectronic and thermoelectric devices.</div></div>","PeriodicalId":20116,"journal":{"name":"Physica B-condensed Matter","volume":"726 ","pages":"Article 418308"},"PeriodicalIF":2.8,"publicationDate":"2026-01-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146038239","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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}