Peng Xiong
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Research Interests
Peng Xiong has a total of 308 co-authors. Here are the top co-authors by number of shared publications:
Stephan von Molnár
Department of Physics, Florida State University, Tallahassee, Florida 32306, USA
28 shared publications- Jianhua Zhao
Institute of Semiconductors
11 shared publications Jianhua Zhao
State Key Laboratory of Superlattices and Microstructures Institute of Semiconductors Chinese Academy of Sciences Beijing 100083 China
10 shared publications- Prescott Bryant Chase
Department of Biological Science, Florida State University, Tallahassee, FL, USA
9 shared publications Hailong Wang
State Key Laboratory of Superlattices and Microstructures Institute of Semiconductors Chinese Academy of Sciences Beijing 100083 China
8 shared publicationsJun Lu
State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
8 shared publications
Latest Publications
Synthetic Control of Structure and Magnetism in Low‐Dimensional Organic Copper(II) Chloride Hybrids
Low‐dimensional (LD) organic metal halide hybrids (OMHHs) have attracted widespread attention owing to their exceptional structural versatility and emergent photophysical and spin‐dependent properties. While hundreds of LD OMHHs have been reported to date, systematic investigations into how organic cations influence structural dimensionality and magnetic behavior remain limited. Here, we report a steric‐engineering strategy to control structural dimensionality and magnetism in LD OMHHs. By systematically tuning methyl substitution in 1,3‐propanediamine (PDA), we achieve a structural progression from two‐dimensional (2D) Dion‐Jacobson (DJ) and Ruddlesden‐Popper (RP) phases to a mixed one‐dimensional/zero‐dimensional (1D/0D) structure, and ultimately isolated 0D structures in a series of organic copper(II) chloride hybrids. This structural evolution modulates magnetic exchange pathways, giving rise to coexisting ferromagnetic (FM) and antiferromagnetic (AFM) interactions in 2D OMHHs, dual AFM transitions in the mixed‐dimensional (MD) system, and paramagnetic (PM) behavior in 0D compounds. Density functional theory (DFT) calculations reveal spin configurations consistent with experimentally observed magnetic behavior. This work presents a unique approach to precisely controlling the dimensionality and magnetism of OMHHs, paving the way for the rational design of ionically bonded organic–inorganic hybrid materials for spintronic applications.
Synthetic Control of Structure and Magnetism in Low‐Dimensional Organic Copper(II) Chloride Hybrids
Low‐dimensional (LD) organic metal halide hybrids (OMHHs) have attracted widespread attention owing to their exceptional structural versatility and emergent photophysical and spin‐dependent properties. While hundreds of LD OMHHs have been reported to date, systematic investigations into how organic cations influence structural dimensionality and magnetic behavior remain limited. Here, we report a steric‐engineering strategy to control structural dimensionality and magnetism in LD OMHHs. By systematically tuning methyl substitution in 1,3‐propanediamine (PDA), we achieve a structural progression from two‐dimensional (2D) Dion‐Jacobson (DJ) and Ruddlesden‐Popper (RP) phases to a mixed one‐dimensional/zero‐dimensional (1D/0D) structure, and ultimately isolated 0D structures in a series of organic copper(II) chloride hybrids. This structural evolution modulates magnetic exchange pathways, giving rise to coexisting ferromagnetic (FM) and antiferromagnetic (AFM) interactions in 2D OMHHs, dual AFM transitions in the mixed‐dimensional (MD) system, and paramagnetic (PM) behavior in 0D compounds. Density functional theory (DFT) calculations reveal spin configurations consistent with experimentally observed magnetic behavior. This work presents a unique approach to precisely controlling the dimensionality and magnetism of OMHHs, paving the way for the rational design of ionically bonded organic–inorganic hybrid materials for spintronic applications.
- Open Access
- 17 June 2026
- Published by Wiley in Small Structures
- Vol. 7 (6)
Mixed‐Dimensional Diammonium Manganese(II) Bromide Hybrid Incorporating 1D Chains and 0D Tetrahedra
Mixed‐dimensional (MD) organic–metal halide hybrids (OMHHs) provide an emerging platform for integrating distinct structure‐dependent optical and magnetic behaviors within a single crystalline phase. While the photophysical properties of conventional low‐dimensional (LD) OMHHs have been widely studied, organic–inorganic hybrids that combine multiple molecular‐level dimensionalities remain largely underexplored. Here, we report a structurally unique MD diammonium manganese(II) bromide hybrid, (TMPDA) 3 (Mn 2 Br 6 )(MnBr 4 ) 2 (TMPDA = N,N,N′,N′‐tetramethyl‐1,3‐propanediammonium), which simultaneously incorporates one‐dimensional (1D) [Mn 2 Br 6 2− ] ∞ chains and zero‐dimensional (0D) MnBr 4 2− tetrahedra within a single crystalline framework. This architecture enables two optical centers to coexist in the same material, yielding excitation‐dependent dual emissions from both the 1D chains and 0D tetrahedra with high photoluminescence quantum efficiencies (PLQEs) of up to 62%. Magnetic measurements reveal weak antiferromagnetic interactions along the 1D chains, arising from Mn···Mn superexchange mediated by bridging bromides. These findings highlight the opportunities offered by MD OMHHs to expand structural and functional tunability beyond traditional LD hybrids, opening new directions for designing multifunctional materials with coupled optical and magnetic properties.
- 17 June 2026
- Published by Wiley in Small Structures
- Vol. 7 (6)
Open AccessMixed‐Dimensional Diammonium Manganese(II) Bromide Hybrid Incorporating 1D Chains and 0D Tetrahedra
Mixed‐dimensional (MD) organic–metal halide hybrids (OMHHs) provide an emerging platform for integrating distinct structure‐dependent optical and magnetic behaviors within a single crystalline phase. While the photophysical properties of conventional low‐dimensional (LD) OMHHs have been widely studied, organic–inorganic hybrids that combine multiple molecular‐level dimensionalities remain largely underexplored. Here, we report a structurally unique MD diammonium manganese(II) bromide hybrid, (TMPDA) 3 (Mn 2 Br 6 )(MnBr 4 ) 2 (TMPDA = N,N,N′,N′‐tetramethyl‐1,3‐propanediammonium), which simultaneously incorporates one‐dimensional (1D) [Mn 2 Br 6 2− ] ∞ chains and zero‐dimensional (0D) MnBr 4 2− tetrahedra within a single crystalline framework. This architecture enables two optical centers to coexist in the same material, yielding excitation‐dependent dual emissions from both the 1D chains and 0D tetrahedra with high photoluminescence quantum efficiencies (PLQEs) of up to 62%. Magnetic measurements reveal weak antiferromagnetic interactions along the 1D chains, arising from Mn···Mn superexchange mediated by bridging bromides. These findings highlight the opportunities offered by MD OMHHs to expand structural and functional tunability beyond traditional LD hybrids, opening new directions for designing multifunctional materials with coupled optical and magnetic properties.
- Open Access
- 14 November 2025
- Published by American Chemical Society (ACS) in ChemRxiv
A Predictive Framework for Discovering Organic Metal Halide Hybrids Beyond Perovskites
Hybrid metal halides have transformed optoelectronics, yet predictive synthesis remains elusive beyond the perovskite family, to which the Goldschmidt tolerance factor offers guidance. Here, we present an open-source platform (https://apollo-omhh.com) that integrates a density functional theory (DFT) database of 7,439 organic metal halide hybrids (OMHHs), derived from 118 experimentally reported compounds spanning diverse electronic structures. Leveraging this dataset and remanent stability theory, we introduce a predictive framework to assess OMHH synthesizability. This framework successfully guided the experimental synthesis of eight previously unreported compounds and achieved 85.2% prediction accuracy across 27 synthesis attempts. This framework is further extended to predict 268 synthesizable OMHHs among 1144 examined OMHHs. Together, these advances establish a data-driven foundation for accelerating the discovery and rational design of hybrid materials beyond perovskite structures.
- 14 November 2025
- Published by American Chemical Society (ACS) in ChemRxiv
Open AccessA Predictive Framework for Discovering Organic Metal Halide Hybrids Beyond Perovskites
Hybrid metal halides have transformed optoelectronics, yet predictive synthesis remains elusive beyond the perovskite family, to which the Goldschmidt tolerance factor offers guidance. Here, we present an open-source platform (https://apollo-omhh.com) that integrates a density functional theory (DFT) database of 7,439 organic metal halide hybrids (OMHHs), derived from 118 experimentally reported compounds spanning diverse electronic structures. Leveraging this dataset and remanent stability theory, we introduce a predictive framework to assess OMHH synthesizability. This framework successfully guided the experimental synthesis of eight previously unreported compounds and achieved 85.2% prediction accuracy across 27 synthesis attempts. This framework is further extended to predict 268 synthesizable OMHHs among 1144 examined OMHHs. Together, these advances establish a data-driven foundation for accelerating the discovery and rational design of hybrid materials beyond perovskite structures.
- Open Access
- 4 October 2025
- Published by MDPI AG in Biosensors
- Vol. 15 (10) , 672
Actomyosin-Based Nanodevices for Sensing and Actuation: Bridging Biology and Bioengineering
The actomyosin complex—nature’s dynamic engine composed of actin filaments and myosin motors—is emerging as a versatile tool for bio-integrated nanotechnology. This review explores the growing potential of actomyosin-powered systems in biosensing and actuation applications, highlighting their compatibility with physiological conditions, responsiveness to biochemical and physical cues and modular adaptability. We begin with a comparative overview of natural and synthetic nanomachines, positioning actomyosin as a uniquely scalable and biocompatible platform. We then discuss experimental advances in controlling actomyosin activity through ATP, calcium, heat, light and electric fields, as well as their integration into in vitro motility assays, soft robotics and neural interface systems. Emphasis is placed on longstanding efforts to harness actomyosin as a biosensing element—capable of converting chemical or environmental signals into measurable mechanical or electrical outputs that can be used to provide valuable clinical and basic science information such as functional consequences of disease-associated genetic variants in cardiovascular genes. We also highlight engineering challenges such as stability, spatial control and upscaling, and examine speculative future directions, including emotion-responsive nanodevices. By bridging cell biology and bioengineering, actomyosin-based systems offer promising avenues for real-time sensing, diagnostics and therapeutic feedback in next-generation biosensors.
- 4 October 2025
- Published by MDPI AG in Biosensors
- Vol. 15 (10) , 672
Open AccessActomyosin-Based Nanodevices for Sensing and Actuation: Bridging Biology and Bioengineering
The actomyosin complex—nature’s dynamic engine composed of actin filaments and myosin motors—is emerging as a versatile tool for bio-integrated nanotechnology. This review explores the growing potential of actomyosin-powered systems in biosensing and actuation applications, highlighting their compatibility with physiological conditions, responsiveness to biochemical and physical cues and modular adaptability. We begin with a comparative overview of natural and synthetic nanomachines, positioning actomyosin as a uniquely scalable and biocompatible platform. We then discuss experimental advances in controlling actomyosin activity through ATP, calcium, heat, light and electric fields, as well as their integration into in vitro motility assays, soft robotics and neural interface systems. Emphasis is placed on longstanding efforts to harness actomyosin as a biosensing element—capable of converting chemical or environmental signals into measurable mechanical or electrical outputs that can be used to provide valuable clinical and basic science information such as functional consequences of disease-associated genetic variants in cardiovascular genes. We also highlight engineering challenges such as stability, spatial control and upscaling, and examine speculative future directions, including emotion-responsive nanodevices. By bridging cell biology and bioengineering, actomyosin-based systems offer promising avenues for real-time sensing, diagnostics and therapeutic feedback in next-generation biosensors.
- Open Access
- 20 March 2025
- Published by National Academy of Sciences in Proceedings of the National Academy of Sciences
- Vol. 122 (12)
Realizing a topological diode effect on the surface of a topological Kondo insulator
Introducing the concept of topology into material science has sparked a revolution from classic electronic and optoelectronic devices to topological quantum devices. The latter has potential for transferring energy and information with unprecedented efficiency. Here, we demonstrate a topological diode effect on the surface of a three-dimensional material, SmB 6 , a candidate topological Kondo insulator. The diode effect is evidenced by pronounced rectification and photogalvanic effects under electromagnetic modulation and radiation at radio frequency. Our experimental results and modeling suggest that these prominent effects are intimately tied to the spatially inhomogeneous formation of topological surface states (TSS) at the intermediate temperature. This work provides a manner of breaking the mirror symmetry (in addition to the inversion symmetry), resulting in the formation of pn -junctions between puddles of metallic TSS. This effect paves the way for efficient current rectifiers or energy-harvesting devices working down to radio frequency range at low temperature, which could be extended to high temperatures using other topological insulators with large bulk gap.
- 20 March 2025
- Published by National Academy of Sciences in Proceedings of the National Academy of Sciences
- Vol. 122 (12)
Open AccessRealizing a topological diode effect on the surface of a topological Kondo insulator
Introducing the concept of topology into material science has sparked a revolution from classic electronic and optoelectronic devices to topological quantum devices. The latter has potential for transferring energy and information with unprecedented efficiency. Here, we demonstrate a topological diode effect on the surface of a three-dimensional material, SmB 6 , a candidate topological Kondo insulator. The diode effect is evidenced by pronounced rectification and photogalvanic effects under electromagnetic modulation and radiation at radio frequency. Our experimental results and modeling suggest that these prominent effects are intimately tied to the spatially inhomogeneous formation of topological surface states (TSS) at the intermediate temperature. This work provides a manner of breaking the mirror symmetry (in addition to the inversion symmetry), resulting in the formation of pn -junctions between puddles of metallic TSS. This effect paves the way for efficient current rectifiers or energy-harvesting devices working down to radio frequency range at low temperature, which could be extended to high temperatures using other topological insulators with large bulk gap.
- 5 November 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 110 (17) , 174502
Superconducting fluctuations and paraconductivity in ultrathin amorphous Pb films near superconductor-insulator transitions
Superconductivity in two dimensions has attracted renewed interest in the context of two-dimensional (2D) van der Waals materials. Key questions remain regarding the nature and manifestations of the superconductivity in these materials. One open question is whether superconducting fluctuations in such 2D systems can be described by the classic Aslamazov-Larkin (A-L) equation. While the A-L model has long been found to accurately describe the paraconductivity of some conventional 2D superconductors, its applicability in ultrathin limit near the superconductor-insulator transition (SIT) has not been established. Here, we report a systematic study of superconducting fluctuation and paraconductivity in ultrathin 2D amorphous Pb films near the SIT. Pb films were incrementally deposited, and the electrical measurements were performed in situ at each thickness in a dilution refrigerator, resulting in a series of sheet resistance curves $[{R}_{\ensuremath{\square}}(T)]$ across the SIT. Paramagnetic impurities (Cr) were then deposited on the same superconducting film, driving it back to the insulating state and yielding another set of ${R}_{\ensuremath{\square}}$($T$). Both types of ${R}_{\ensuremath{\square}}$($T$) curves were analyzed with the A-L equation. At all film thicknesses (and ${T}_{C}$'s), we observed a background paraconductivity significantly greater than the A-L value. As the film thickness decreases and the SIT is approached, the paraconductivity increases precipitously, reaching more than an order of magnitude higher than that of the A-L value at the immediate vicinity of the SIT. Accompanying the presence of excess paraconductivity and its increase with decreasing thickness, the paraconductivity exhibits exponential scaling with $T$ above ${T}_{C}$, whose temperature range and slope show concomitant variations with decreasing film thickness. In contrast, suppression of ${T}_{C}$ by magnetic impurity results in much weaker increase of the excess paraconductivity and little change in the temperature range and slope of the exponential $T$ scaling. These observations are consistent with the presence of emergent localized superconducting pairing above ${T}_{C}$ in the strongly disordered, morphologically nominally uniform amorphous films. The spatially localized superconductivity likely causes excess paraconductivity beyond the A-L theory and percolative superconducting transitions. Such electronic inhomogeneities proliferate with decreasing film thickness, especially near the SIT.- 5 November 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 110 (17) , 174502
Superconducting fluctuations and paraconductivity in ultrathin amorphous Pb films near superconductor-insulator transitions
Superconductivity in two dimensions has attracted renewed interest in the context of two-dimensional (2D) van der Waals materials. Key questions remain regarding the nature and manifestations of the superconductivity in these materials. One open question is whether superconducting fluctuations in such 2D systems can be described by the classic Aslamazov-Larkin (A-L) equation. While the A-L model has long been found to accurately describe the paraconductivity of some conventional 2D superconductors, its applicability in ultrathin limit near the superconductor-insulator transition (SIT) has not been established. Here, we report a systematic study of superconducting fluctuation and paraconductivity in ultrathin 2D amorphous Pb films near the SIT. Pb films were incrementally deposited, and the electrical measurements were performed in situ at each thickness in a dilution refrigerator, resulting in a series of sheet resistance curves $[{R}_{\ensuremath{\square}}(T)]$ across the SIT. Paramagnetic impurities (Cr) were then deposited on the same superconducting film, driving it back to the insulating state and yielding another set of ${R}_{\ensuremath{\square}}$($T$). Both types of ${R}_{\ensuremath{\square}}$($T$) curves were analyzed with the A-L equation. At all film thicknesses (and ${T}_{C}$'s), we observed a background paraconductivity significantly greater than the A-L value. As the film thickness decreases and the SIT is approached, the paraconductivity increases precipitously, reaching more than an order of magnitude higher than that of the A-L value at the immediate vicinity of the SIT. Accompanying the presence of excess paraconductivity and its increase with decreasing thickness, the paraconductivity exhibits exponential scaling with $T$ above ${T}_{C}$, whose temperature range and slope show concomitant variations with decreasing film thickness. In contrast, suppression of ${T}_{C}$ by magnetic impurity results in much weaker increase of the excess paraconductivity and little change in the temperature range and slope of the exponential $T$ scaling. These observations are consistent with the presence of emergent localized superconducting pairing above ${T}_{C}$ in the strongly disordered, morphologically nominally uniform amorphous films. The spatially localized superconductivity likely causes excess paraconductivity beyond the A-L theory and percolative superconducting transitions. Such electronic inhomogeneities proliferate with decreasing film thickness, especially near the SIT.- 10 July 2024
- Published by Wiley in Advanced Materials
- Vol. 36 (36) , e2406347
Chirality‐Induced Magnet‐Free Spin Generation in a Semiconductor
Electrical generation and transduction of polarized electron spins in semiconductors (SCs) are of central interest in spintronics and quantum information science. While spin generation in SCs is frequently realized via electrical injection from a ferromagnet (FM), there are significant advantages in nonmagnetic pathways of creating spin polarization. One such pathway exploits the interplay of electron spin with chirality in electronic structures or real space. Here, utilizing chirality‐induced spin selectivity (CISS), the efficient creation of spin accumulation in n‐doped GaAs via electric current injection from a normal metal (Au) electrode through a self‐assembled monolayer (SAM) of chiral molecules (α‐helix l‐polyalanine, AHPA‐L), is demonstrated. The resulting spin polarization is detected as a Hanle effect in the n‐GaAs, which is found to obey a distinct universal scaling with temperature and bias current consistent with chirality‐induced spin accumulation. The experiment constitutes a definitive observation of CISS in a fully nonmagnetic device structure and demonstration of its ability to generate spin accumulation in a conventional SC. The results thus place key constraints on the physical mechanism of CISS and present a new scheme for magnet‐free SC spintronics.
- 10 July 2024
- Published by Wiley in Advanced Materials
- Vol. 36 (36) , e2406347
Chirality‐Induced Magnet‐Free Spin Generation in a Semiconductor
Electrical generation and transduction of polarized electron spins in semiconductors (SCs) are of central interest in spintronics and quantum information science. While spin generation in SCs is frequently realized via electrical injection from a ferromagnet (FM), there are significant advantages in nonmagnetic pathways of creating spin polarization. One such pathway exploits the interplay of electron spin with chirality in electronic structures or real space. Here, utilizing chirality‐induced spin selectivity (CISS), the efficient creation of spin accumulation in n‐doped GaAs via electric current injection from a normal metal (Au) electrode through a self‐assembled monolayer (SAM) of chiral molecules (α‐helix l‐polyalanine, AHPA‐L), is demonstrated. The resulting spin polarization is detected as a Hanle effect in the n‐GaAs, which is found to obey a distinct universal scaling with temperature and bias current consistent with chirality‐induced spin accumulation. The experiment constitutes a definitive observation of CISS in a fully nonmagnetic device structure and demonstration of its ability to generate spin accumulation in a conventional SC. The results thus place key constraints on the physical mechanism of CISS and present a new scheme for magnet‐free SC spintronics.
- Open Access
Chirality-Induced Magnet-Free Spin Generation in a Semiconductor
Electrical generation and transduction of polarized electron spins in semiconductors are of central interest in spintronics and quantum information science. While spin generation in semiconductors has been frequently realized via electrical injection from a ferromagnet, there are significant advantages in nonmagnetic pathways of creating spin polarization. One such pathway exploits the interplay of electron spin with chirality in electronic structures or real space. Here, utilizing chirality-induced spin selectivity (CISS), we demonstrate efficient creation of spin accumulation in n-doped GaAs via electric current injection from a normal metal (Au) electrode through a self-assembled monolayer of chiral molecules (α-helix L-polyalanine, AHPA-L). The resulting spin polarization is detected as a Hanle effect in the n-GaAs, which is found to obey a distinct universal scaling with temperature and bias current consistent with chirality-induced spin accumulation. The experiment constitutes a definitive observation of CISS in a fully nonmagnetic device structure and demonstration of its ability to generate spin accumulation in a conventional semiconductor. The results thus place key constraints on the physical mechanism of CISS and present a new scheme for magnet-free semiconductor spintronics.
Open AccessChirality-Induced Magnet-Free Spin Generation in a Semiconductor
Electrical generation and transduction of polarized electron spins in semiconductors are of central interest in spintronics and quantum information science. While spin generation in semiconductors has been frequently realized via electrical injection from a ferromagnet, there are significant advantages in nonmagnetic pathways of creating spin polarization. One such pathway exploits the interplay of electron spin with chirality in electronic structures or real space. Here, utilizing chirality-induced spin selectivity (CISS), we demonstrate efficient creation of spin accumulation in n-doped GaAs via electric current injection from a normal metal (Au) electrode through a self-assembled monolayer of chiral molecules (α-helix L-polyalanine, AHPA-L). The resulting spin polarization is detected as a Hanle effect in the n-GaAs, which is found to obey a distinct universal scaling with temperature and bias current consistent with chirality-induced spin accumulation. The experiment constitutes a definitive observation of CISS in a fully nonmagnetic device structure and demonstration of its ability to generate spin accumulation in a conventional semiconductor. The results thus place key constraints on the physical mechanism of CISS and present a new scheme for magnet-free semiconductor spintronics.
- 20 February 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 109 (6) , 064510
Pressure-induced surface superconductivity in the noncentrosymmetric superconductor : Pressure-dependent point-contact Andreev spectroscopyA notable characteristic of , a prototypical noncentrosymmetric superconductor (NCS), is that its superconductivity can be modulated through a structural transition under hydrostatic pressure [Kaluarachchi et al. Phys. Rev. B 95, 224508 (2017)]. Here we report on a combined pressure-sensitive point-contact Andreev reflection (PCAR) spectroscopy with bulk resistance measurements on , to elucidate the nature of the surface and bulk superconductivity and their evolution with hydrostatic pressure. It is found that in a high-pressure region the superconducting gap opening temperature is significantly lower than the bulk resistive transition temperature , revealing a clear experimental signature of surface-bulk separation associated with enhanced antisymmetric spin-orbit coupling (ASOC). The PCAR spectra, reflecting the superconducting surface state, are analyzed with two-dimensional Blonder-Tinkham-Klapwijk theory, yielding an isotropic -wave full BCS gap in the strong-coupling regime. These results suggest the coexistence of full gap -wave superconductivity and topological surface states in , indicating that this NSC superconductor with significantly enhanced ASOC may offer a solid platform to investigate the topological aspect in the superconducting condensate.- 20 February 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 109 (6) , 064510
Pressure-induced surface superconductivity in the noncentrosymmetric superconductor : Pressure-dependent point-contact Andreev spectroscopyA notable characteristic of , a prototypical noncentrosymmetric superconductor (NCS), is that its superconductivity can be modulated through a structural transition under hydrostatic pressure [Kaluarachchi et al. Phys. Rev. B 95, 224508 (2017)]. Here we report on a combined pressure-sensitive point-contact Andreev reflection (PCAR) spectroscopy with bulk resistance measurements on , to elucidate the nature of the surface and bulk superconductivity and their evolution with hydrostatic pressure. It is found that in a high-pressure region the superconducting gap opening temperature is significantly lower than the bulk resistive transition temperature , revealing a clear experimental signature of surface-bulk separation associated with enhanced antisymmetric spin-orbit coupling (ASOC). The PCAR spectra, reflecting the superconducting surface state, are analyzed with two-dimensional Blonder-Tinkham-Klapwijk theory, yielding an isotropic -wave full BCS gap in the strong-coupling regime. These results suggest the coexistence of full gap -wave superconductivity and topological surface states in , indicating that this NSC superconductor with significantly enhanced ASOC may offer a solid platform to investigate the topological aspect in the superconducting condensate.- Top Cited PapersOpen Access
- 24 August 2023
- Published by Springer Nature in Nature Communications
- Vol. 14 (1) , 1-9
Interplay of structural chirality, electron spin and topological orbital in chiral molecular spin valves
Chirality has been a property of central importance in physics, chemistry and biology for more than a century. Recently, electrons were found to become spin polarized after transmitting through chiral molecules, crystals, and their hybrids. This phenomenon, called chirality-induced spin selectivity (CISS), presents broad application potentials and far-reaching fundamental implications involving intricate interplays among structural chirality, topological states, and electronic spin and orbitals. However, the microscopic picture of how chiral geometry influences electronic spin remains elusive, given the negligible spin-orbit coupling (SOC) in organic molecules. In this work, we address this issue via a direct comparison of magnetoconductance (MC) measurements on magnetic semiconductor-based chiral molecular spin valves with normal metal electrodes of contrasting SOC strengths. The experiment reveals that a heavy-metal electrode provides SOC to convert the orbital polarization induced by the chiral molecular structure to spin polarization. Our results illustrate the essential role of SOC in the metal electrode for the CISS spin valve effect. A tunneling model with a magnetochiral modulation of the potential barrier is shown to quantitatively account for the unusual transport behavior.
- 24 August 2023
- Published by Springer Nature in Nature Communications
- Vol. 14 (1) , 1-9
Top Cited PapersOpen AccessInterplay of structural chirality, electron spin and topological orbital in chiral molecular spin valves
Chirality has been a property of central importance in physics, chemistry and biology for more than a century. Recently, electrons were found to become spin polarized after transmitting through chiral molecules, crystals, and their hybrids. This phenomenon, called chirality-induced spin selectivity (CISS), presents broad application potentials and far-reaching fundamental implications involving intricate interplays among structural chirality, topological states, and electronic spin and orbitals. However, the microscopic picture of how chiral geometry influences electronic spin remains elusive, given the negligible spin-orbit coupling (SOC) in organic molecules. In this work, we address this issue via a direct comparison of magnetoconductance (MC) measurements on magnetic semiconductor-based chiral molecular spin valves with normal metal electrodes of contrasting SOC strengths. The experiment reveals that a heavy-metal electrode provides SOC to convert the orbital polarization induced by the chiral molecular structure to spin polarization. Our results illustrate the essential role of SOC in the metal electrode for the CISS spin valve effect. A tunneling model with a magnetochiral modulation of the potential barrier is shown to quantitatively account for the unusual transport behavior.