Pub Date : 2026-03-13DOI: 10.1140/epjb/s10051-026-01135-0
L. Craco
Using dynamical mean-field theory (DMFT), we explore the many-particle properties of an extended two-band Hubbard model applicable to 2H-TaSe(_2) superconductor. We reveal the electronic reconstruction of the CDW-Mott state driven by site-diagonal disorder with distinct many-particle excitations. Our results offer new microscopic theory insights into the Mott–Anderson nature of charge carriers and the correlated metallic state which emerges from site-diagonal disorder within the CDW-Mott regime.
{"title":"Theory of two-band metallicity from correlation plus site-diagonal disorder in the CDW-Mott phase of 2H-TaSe(_2)","authors":"L. Craco","doi":"10.1140/epjb/s10051-026-01135-0","DOIUrl":"10.1140/epjb/s10051-026-01135-0","url":null,"abstract":"<p>Using dynamical mean-field theory (DMFT), we explore the many-particle properties of an extended two-band Hubbard model applicable to 2<i>H</i>-TaSe<span>(_2)</span> superconductor. We reveal the electronic reconstruction of the CDW-Mott state driven by site-diagonal disorder with distinct many-particle excitations. Our results offer new microscopic theory insights into the Mott–Anderson nature of charge carriers and the correlated metallic state which emerges from site-diagonal disorder within the CDW-Mott regime.</p>","PeriodicalId":787,"journal":{"name":"The European Physical Journal B","volume":"99 3","pages":""},"PeriodicalIF":1.7,"publicationDate":"2026-03-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epjb/s10051-026-01135-0.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147441827","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-03-13DOI: 10.1140/epjb/s10051-026-01142-1
G. Dimitri Ngantso, M. Karimou, A. Kadiri
We study the magnetic and magnetocaloric properties of an asymmetric ferrimagnetic bilayer composed of spin-1 and spin-1/2 Ising sublattices, including intralayer exchange anisotropies and an antiferromagnetic interlayer coupling. Using Monte Carlo simulations with the Metropolis algorithm, we incorporate anisotropic in-plane interactions, a Blume–Capel single-ion anisotropy acting on the spin-1 layer, and an external magnetic field. Critical temperatures are determined from Binder cumulants, while compensation temperatures are identified from sublattice magnetizations. The temperature derivative of the entropy and isothermal entropy change are evaluated to characterize the magnetocaloric response under weak fields. The results show that anisotropy in the spin-1 layer strongly tunes the compensation point, whereas anisotropy in the spin-1/2 layer mainly affects the stability of the ordered phase. Hysteresis loops exhibit several switching mechanisms, including multi-loop structures, driven by the interplay between anisotropy and interlayer coupling. These findings underline the crucial role of anisotropic exchange and Blume–Capel physics in tailoring magnetocaloric and coercive properties of ferrimagnetic bilayers.
{"title":"Asymmetric ferrimagnetic bilayers with intralayer exchange anisotropy: magnetocaloric and critical properties","authors":"G. Dimitri Ngantso, M. Karimou, A. Kadiri","doi":"10.1140/epjb/s10051-026-01142-1","DOIUrl":"10.1140/epjb/s10051-026-01142-1","url":null,"abstract":"<div><p>We study the magnetic and magnetocaloric properties of an asymmetric ferrimagnetic bilayer composed of spin-1 and spin-1/2 Ising sublattices, including intralayer exchange anisotropies and an antiferromagnetic interlayer coupling. Using Monte Carlo simulations with the Metropolis algorithm, we incorporate anisotropic in-plane interactions, a Blume–Capel single-ion anisotropy acting on the spin-1 layer, and an external magnetic field. Critical temperatures are determined from Binder cumulants, while compensation temperatures are identified from sublattice magnetizations. The temperature derivative of the entropy and isothermal entropy change are evaluated to characterize the magnetocaloric response under weak fields. The results show that anisotropy in the spin-1 layer strongly tunes the compensation point, whereas anisotropy in the spin-1/2 layer mainly affects the stability of the ordered phase. Hysteresis loops exhibit several switching mechanisms, including multi-loop structures, driven by the interplay between anisotropy and interlayer coupling. These findings underline the crucial role of anisotropic exchange and Blume–Capel physics in tailoring magnetocaloric and coercive properties of ferrimagnetic bilayers.</p><h3>Graphical abstract</h3><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":787,"journal":{"name":"The European Physical Journal B","volume":"99 3","pages":""},"PeriodicalIF":1.7,"publicationDate":"2026-03-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147441825","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 : 2026-03-11DOI: 10.1140/epjb/s10051-026-01127-0
Nuno Crokidakis, Lucas Sigaud
Racism remains a persistent societal issue, increasingly amplified by the structure and dynamics of online social networks. In this work, we propose a three-state compartmental model to study the spreading and suppression of racist content, drawing from epidemic-like dynamics and interaction-driven transitions. We analyze the model on fully connected (homogeneous mixing) networks using a set of coupled differential equations, and on Barabási–Albert scale-free and Watts–Strogatz small-world networks through agent-based simulations. The system exhibits three distinct stationary regimes: two racism-free absorbing states and one active phase with persistent racist content. We identify and characterize the phase transitions between these regimes, discuss the role of network topology, and highlight the emergence of absorbing states. Our findings illustrate how statistical physics tools can help uncover the macroscopic consequences of microscopic social interactions in digital environments.
{"title":"Nonequilibrium phase transitions in a racism-spreading model with interaction-driven dynamics","authors":"Nuno Crokidakis, Lucas Sigaud","doi":"10.1140/epjb/s10051-026-01127-0","DOIUrl":"10.1140/epjb/s10051-026-01127-0","url":null,"abstract":"<p>Racism remains a persistent societal issue, increasingly amplified by the structure and dynamics of online social networks. In this work, we propose a three-state compartmental model to study the spreading and suppression of racist content, drawing from epidemic-like dynamics and interaction-driven transitions. We analyze the model on fully connected (homogeneous mixing) networks using a set of coupled differential equations, and on Barabási–Albert scale-free and Watts–Strogatz small-world networks through agent-based simulations. The system exhibits three distinct stationary regimes: two racism-free absorbing states and one active phase with persistent racist content. We identify and characterize the phase transitions between these regimes, discuss the role of network topology, and highlight the emergence of absorbing states. Our findings illustrate how statistical physics tools can help uncover the macroscopic consequences of microscopic social interactions in digital environments.</p>","PeriodicalId":787,"journal":{"name":"The European Physical Journal B","volume":"99 3","pages":""},"PeriodicalIF":1.7,"publicationDate":"2026-03-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epjb/s10051-026-01127-0.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147441254","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
This study systematically investigates the modulation of deep strain-induced indirect-to-direct bandgap transition in boron arsenide (BAs) using first-principles calculations. Uniaxial tensile and compressive strains are applied along [001], [110], and [111] directions to explore the electronic structure evolution. Results show that compressive strains along all three directions cause linear decreases in the bandgap until metallic transition, while tensile strains exhibit anisotropic behaviors. Notably, stretching along [111] direction triggers an indirect-to-direct bandgap transition at a critical strain of 0.12: the conduction band energy at (Gamma ) point decreases faster than that near X point, leading to the bottom of the conduction band shifting from X to (Gamma ) point. The density of states analysis confirms that the Fermi surface electrons are primarily contributed by B and As p-electrons, remaining unchanged during the bandgap transition. This work provides theoretical insights for strain-engineered optoelectronic applications of BAs.
{"title":"Indirect to direct bandgap transition in BAs through deep elastic uniaxial strain","authors":"Shuchao Zhang, Peng Gu, Sheng Ding, Bangzhao Wang, Junsen Gao, Lijian Chen, Yijian Ge, Shukuan Guo","doi":"10.1140/epjb/s10051-026-01151-0","DOIUrl":"10.1140/epjb/s10051-026-01151-0","url":null,"abstract":"<p>This study systematically investigates the modulation of deep strain-induced indirect-to-direct bandgap transition in boron arsenide (BAs) using first-principles calculations. Uniaxial tensile and compressive strains are applied along [001], [110], and [111] directions to explore the electronic structure evolution. Results show that compressive strains along all three directions cause linear decreases in the bandgap until metallic transition, while tensile strains exhibit anisotropic behaviors. Notably, stretching along [111] direction triggers an indirect-to-direct bandgap transition at a critical strain of 0.12: the conduction band energy at <span>(Gamma )</span> point decreases faster than that near X point, leading to the bottom of the conduction band shifting from X to <span>(Gamma )</span> point. The density of states analysis confirms that the Fermi surface electrons are primarily contributed by B and As <i>p</i>-electrons, remaining unchanged during the bandgap transition. This work provides theoretical insights for strain-engineered optoelectronic applications of BAs.</p>","PeriodicalId":787,"journal":{"name":"The European Physical Journal B","volume":"99 3","pages":""},"PeriodicalIF":1.7,"publicationDate":"2026-03-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147441252","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 : 2026-03-11DOI: 10.1140/epjb/s10051-026-01148-9
D. Sekyi-Arthur, K. W. Adu, K. A. Dompreh, E. Atioyire, S. Y. Mensah, B. Afoakwa
Herein, we report on self-sustaining acoustoelectric direct current oscillations in fluorine-doped single-walled carbon nanotubes stimulated by a strong internal electric field. The study is carried out in the hypersound regime, where carrier transport is confined to the lowest electronic miniband, leading to enhanced nonlinear and non-monotonic acoustoelectric current response. The carrier dynamics predicted by the model are consistent with experimentally observed oscillatory acoustoelectric current in a graphene-based acoustoelectric switch. The oscillatory behavior is shown to originate from spatial charge instabilities and field-induced Bloch-like carrier dynamics, occurring in the absence of an external resonator. The resulting non-uniform space-charge distribution, together with Bloch-reflected carrier motion, is identified as the dominant mechanism responsible for terahertz radiation generation. In addition, the dynamic interplay between acoustic phonons and charge carriers suggests the possibility of suppressing electric domain formation and realizing acoustic Bloch gain. These results demonstrate that fluorine-doped single-walled carbon nanotubes can operate efficiently at elevated temperatures and are promising candidates for high-frequency electronic and optoelectronic applications extending into the submillimeter-wave regime.
{"title":"Self-sustained acoustoelectric oscillations in fluorine-doped carbon nanotubes under strong electric fields","authors":"D. Sekyi-Arthur, K. W. Adu, K. A. Dompreh, E. Atioyire, S. Y. Mensah, B. Afoakwa","doi":"10.1140/epjb/s10051-026-01148-9","DOIUrl":"10.1140/epjb/s10051-026-01148-9","url":null,"abstract":"<p>Herein, we report on self-sustaining acoustoelectric direct current oscillations in fluorine-doped single-walled carbon nanotubes stimulated by a strong internal electric field. The study is carried out in the hypersound regime, where carrier transport is confined to the lowest electronic miniband, leading to enhanced nonlinear and non-monotonic acoustoelectric current response. The carrier dynamics predicted by the model are consistent with experimentally observed oscillatory acoustoelectric current in a graphene-based acoustoelectric switch. The oscillatory behavior is shown to originate from spatial charge instabilities and field-induced Bloch-like carrier dynamics, occurring in the absence of an external resonator. The resulting non-uniform space-charge distribution, together with Bloch-reflected carrier motion, is identified as the dominant mechanism responsible for terahertz radiation generation. In addition, the dynamic interplay between acoustic phonons and charge carriers suggests the possibility of suppressing electric domain formation and realizing acoustic Bloch gain. These results demonstrate that fluorine-doped single-walled carbon nanotubes can operate efficiently at elevated temperatures and are promising candidates for high-frequency electronic and optoelectronic applications extending into the submillimeter-wave regime.</p>","PeriodicalId":787,"journal":{"name":"The European Physical Journal B","volume":"99 3","pages":""},"PeriodicalIF":1.7,"publicationDate":"2026-03-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147441253","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 : 2026-03-10DOI: 10.1140/epjb/s10051-026-01145-y
S. Akshay Kalyan, K. Kamalakkannan, Mukesh Ranjan, N. Kanagathara
The dielectric and charge-transport properties of an organic single crystal, melaminium glycolate hemihydrate (MGHM), were systematically investigated using broadband dielectric, impedance, modulus, electronic polarizability, and confocal Raman spectroscopic techniques. Dielectric measurements were performed in the frequency range of 1 Hz to 20 MHz at temperatures between 293 to 373 K which reveals the dielectric constant (εr) and dielectric loss (tan δ) decrease with frequency, showing normal dielectric behaviour characteristics of dipolar relaxation. At higher temperatures (353 K and 373 K), a pronounced enhancement of εr at low frequencies accompanied by well-defined sharp dielectric loss peaks, indicates the strong space charge polarization and thermally activated relaxation. These features are consistent with Maxwell–Wagner interfacial polarization and enhanced electrical conduction at elevated temperatures. Impedance spectroscopic analysis carried out over the temperature range 293–373 K shows high impedance and distinct relaxation features at lower temperatures, arising from interfacial or defect-related contributions and electrode polarization effects. With increasing temperature, impedance decreases markedly due to thermally activated charge carriers, and the associated relaxation peaks shift toward higher frequencies. Nyquist plots confirm a transition in conduction mechanism from grain-boundary-dominated transport at lower temperatures to bulk-grain-dominated conduction at higher temperatures. At 373 K, the significantly reduced impedance indicates highly conductive behaviour. Modulus spectroscopy further supports thermally activated relaxation, with the real (M′) and imaginary (M″) components exhibiting relaxation peaks that systematically shift to higher frequencies with increasing temperature. Phase angle (Bode) plots show two distinct relaxation processes at lower temperatures (293–333 K), attributed to dipolar polarization and interfacial boundary effects, whereas a single broad relaxation dominates at higher temperatures (353–373 K), indicating conduction-controlled dynamics.. Electronic polarizability evaluated using Penn analysis, the Clausius–Mossotti relation, and the optical band-gap method demonstrates a clear temperature dependence, with polarizability decreasing initially and reaching a maximum at 373 K. Confocal Raman studies reveal temperature-induced enhancement in phonon intensities, indicating lattice relaxation. The emergence of second-order vibrational modes near ~ 2921 cm−1 signifies increased lattice ordering, while the temperature-dependent shift of the prominent triazine breathing mode around ~ 690 cm−1 correlates directly with thermally activated charge transport.
{"title":"Temperature-dependent dielectric relaxation and Raman phonon correlation in melaminium glycolate hemihydrate","authors":"S. Akshay Kalyan, K. Kamalakkannan, Mukesh Ranjan, N. Kanagathara","doi":"10.1140/epjb/s10051-026-01145-y","DOIUrl":"10.1140/epjb/s10051-026-01145-y","url":null,"abstract":"<div><p>The dielectric and charge-transport properties of an organic single crystal, melaminium glycolate hemihydrate (MGHM), were systematically investigated using broadband dielectric, impedance, modulus, electronic polarizability, and confocal Raman spectroscopic techniques. Dielectric measurements were performed in the frequency range of 1 Hz to 20 MHz at temperatures between 293 to 373 K which reveals the dielectric constant (<i>ε</i><sub><i>r</i></sub>) and dielectric loss (tan <i>δ</i>) decrease with frequency, showing normal dielectric behaviour characteristics of dipolar relaxation. At higher temperatures (353 K and 373 K), a pronounced enhancement of <i>ε</i><sub><i>r</i></sub> at low frequencies accompanied by well-defined sharp dielectric loss peaks, indicates the strong space charge polarization and thermally activated relaxation. These features are consistent with Maxwell–Wagner interfacial polarization and enhanced electrical conduction at elevated temperatures. Impedance spectroscopic analysis carried out over the temperature range 293–373 K shows high impedance and distinct relaxation features at lower temperatures, arising from interfacial or defect-related contributions and electrode polarization effects. With increasing temperature, impedance decreases markedly due to thermally activated charge carriers, and the associated relaxation peaks shift toward higher frequencies. Nyquist plots confirm a transition in conduction mechanism from grain-boundary-dominated transport at lower temperatures to bulk-grain-dominated conduction at higher temperatures. At 373 K, the significantly reduced impedance indicates highly conductive behaviour. Modulus spectroscopy further supports thermally activated relaxation, with the real (<i>M</i>′) and imaginary (<i>M</i>″) components exhibiting relaxation peaks that systematically shift to higher frequencies with increasing temperature. Phase angle (Bode) plots show two distinct relaxation processes at lower temperatures (293–333 K), attributed to dipolar polarization and interfacial boundary effects, whereas a single broad relaxation dominates at higher temperatures (353–373 K), indicating conduction-controlled dynamics.. Electronic polarizability evaluated using Penn analysis, the Clausius–Mossotti relation, and the optical band-gap method demonstrates a clear temperature dependence, with polarizability decreasing initially and reaching a maximum at 373 K. Confocal Raman studies reveal temperature-induced enhancement in phonon intensities, indicating lattice relaxation. The emergence of second-order vibrational modes near ~ 2921 cm<sup>−1</sup> signifies increased lattice ordering, while the temperature-dependent shift of the prominent triazine breathing mode around ~ 690 cm<sup>−1</sup> correlates directly with thermally activated charge transport.</p><h3>Graphical abstract</h3><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":787,"journal":{"name":"The European Physical Journal B","volume":"99 3","pages":""},"PeriodicalIF":1.7,"publicationDate":"2026-03-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147441302","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 : 2026-03-09DOI: 10.1140/epjb/s10051-026-01146-x
Archit Dhingra, M. Zaid Zaz
Spin crossover (SCO) complexes are highly promising candidates for a myriad of potential applications in room-temperature electronics; however, as it stands, establishing a clear connection between their spin-state switching and transport properties has been far from trivial. In this perspective, an effort to unravel the underlying charge transport mechanism in these SCO complexes, via a general theory, is made. The theory presented herein is aimed at providing a unifying picture that explains the widely different trends observed in the spin-crossover-dependent carrier transport properties in the SCO molecular thin-film systems.