Pub Date : 2024-08-19DOI: 10.1007/s11467-024-1434-3
Yu Guo, Yang Zhao, Qiao Ling, Si Zhou, Jijun Zhao
Cluster-assembled materials have long been pursued as they can create some unprecedented and desirable properties. Herein, we assemble a class of one-dimensional (1D) ReNX4 (X = F, Cl, Br and I) and MF5 (M = V, Nb and Ta) nanowires by covalently linking their superatomic clusters. These assembled 1D nanowires exhibit outstanding energetic and dynamic stabilities, and hold sizable spontaneous polarization, low ferroelectric switching barriers and high critical temperature. Their superior ferroelectricity is originated from d0-configuration transition metal ions generated by the hybridization of empty d orbitals of metal atoms and p orbitals of non-metal atoms. These critical insights pave a new avenue to fabricate 1D ferroelectrics toward the development of miniaturized and high-density electronic devices using building blocks as cluster with precise structures and functionalities.
长期以来,人们一直在研究簇组装材料,因为它们可以产生一些前所未有的理想特性。在这里,我们通过共价连接超原子团簇,组装出一类一维(1D)ReNX4(X = F、Cl、Br 和 I)和 MF5(M = V、Nb 和 Ta)纳米线。这些组装好的一维纳米线表现出卓越的能量和动态稳定性,并具有可观的自发极化、低铁电开关势垒和高临界温度。它们卓越的铁电性源于金属原子的空 d 轨道和非金属原子的 p 轨道杂化产生的 d0 配置过渡金属离子。这些重要见解为制造一维铁电体铺平了一条新的道路,从而利用具有精确结构和功能的构件集群,开发出小型化和高密度的电子器件。
{"title":"Strong ferroelectricity in one-dimensional materials self-assembled by superatomic metal halide clusters","authors":"Yu Guo, Yang Zhao, Qiao Ling, Si Zhou, Jijun Zhao","doi":"10.1007/s11467-024-1434-3","DOIUrl":"10.1007/s11467-024-1434-3","url":null,"abstract":"<div><p>Cluster-assembled materials have long been pursued as they can create some unprecedented and desirable properties. Herein, we assemble a class of one-dimensional (1D) ReNX<sub>4</sub> (X = F, Cl, Br and I) and MF<sub>5</sub> (M = V, Nb and Ta) nanowires by covalently linking their superatomic clusters. These assembled 1D nanowires exhibit outstanding energetic and dynamic stabilities, and hold sizable spontaneous polarization, low ferroelectric switching barriers and high critical temperature. Their superior ferroelectricity is originated from <i>d</i><sup>0</sup>-configuration transition metal ions generated by the hybridization of empty <i>d</i> orbitals of metal atoms and <i>p</i> orbitals of non-metal atoms. These critical insights pave a new avenue to fabricate 1D ferroelectrics toward the development of miniaturized and high-density electronic devices using building blocks as cluster with precise structures and functionalities.\u0000</p><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":573,"journal":{"name":"Frontiers of Physics","volume":"19 6","pages":""},"PeriodicalIF":6.5,"publicationDate":"2024-08-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142190171","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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 values of the low-energy constants (LECs) are very important in the chiral perturbation theory. This paper adopts a Bayesian method with the truncation errors to globally fit eight next-to-leading order (NLO) LECs Lri and next-to-next-leading order (NNLO) LECs Cri. With the estimation of the truncation errors, the fitting results of Lri in the NLO and NNLO are very close. The posterior distributions of Cri indicate the boundary-dependent relations of these Cri. Ten Cri are weakly dependent on the boundaries and their values are reliable. The other Cri are required more experimental data to constrain their boundaries. Some linear combinations of Cri are also fitted with more reliable posterior distributions. If one knows some more precise values of Cri, some other Cri can be obtained by these values. With these fitting LECs, most observables provide a good convergence, except for the πK scattering lengths a3/20 and a1/20. An example is also introduced to test the improvement of the method. All the computations indicate that considering the truncation errors can improve the global fit greatly, and more prior information can obtain better fitting results. This fitting method can be extended to the other effective field theories and the perturbation theory.
{"title":"Bayesian method for fitting the low-energy constants in chiral perturbation theory","authors":"Hao-Xiang Pan, De-Kai Kong, Qiao-Yi Wen, Shao-Zhou Jiang","doi":"10.1007/s11467-024-1430-7","DOIUrl":"10.1007/s11467-024-1430-7","url":null,"abstract":"<div><p>The values of the low-energy constants (LECs) are very important in the chiral perturbation theory. This paper adopts a Bayesian method with the truncation errors to globally fit eight next-to-leading order (NLO) LECs <i>L</i><span>\u0000 <sup><i>r</i></sup><sub><i>i</i></sub>\u0000 \u0000 </span> and next-to-next-leading order (NNLO) LECs <i>C</i><span>\u0000 <sup><i>r</i></sup><sub><i>i</i></sub>\u0000 \u0000 </span>. With the estimation of the truncation errors, the fitting results of <i>L</i><span>\u0000 <sup><i>r</i></sup><sub><i>i</i></sub>\u0000 \u0000 </span> in the NLO and NNLO are very close. The posterior distributions of <i>C</i><span>\u0000 <sup><i>r</i></sup><sub><i>i</i></sub>\u0000 \u0000 </span> indicate the boundary-dependent relations of these <i>C</i><span>\u0000 <sup><i>r</i></sup><sub><i>i</i></sub>\u0000 \u0000 </span>. Ten <i>C</i><span>\u0000 <sup><i>r</i></sup><sub><i>i</i></sub>\u0000 \u0000 </span> are weakly dependent on the boundaries and their values are reliable. The other <i>C</i><span>\u0000 <sup><i>r</i></sup><sub><i>i</i></sub>\u0000 \u0000 </span> are required more experimental data to constrain their boundaries. Some linear combinations of <i>C</i><span>\u0000 <sup><i>r</i></sup><sub><i>i</i></sub>\u0000 \u0000 </span> are also fitted with more reliable posterior distributions. If one knows some more precise values of <i>C</i><span>\u0000 <sup><i>r</i></sup><sub><i>i</i></sub>\u0000 \u0000 </span>, some other <i>C</i><span>\u0000 <sup><i>r</i></sup><sub><i>i</i></sub>\u0000 \u0000 </span> can be obtained by these values. With these fitting LECs, most observables provide a good convergence, except for the <i>πK</i> scattering lengths <i>a</i><span>\u0000 <sup>3/2</sup><sub>0</sub>\u0000 \u0000 </span> and <i>a</i><span>\u0000 <sup>1/2</sup><sub>0</sub>\u0000 \u0000 </span>. An example is also introduced to test the improvement of the method. All the computations indicate that considering the truncation errors can improve the global fit greatly, and more prior information can obtain better fitting results. This fitting method can be extended to the other effective field theories and the perturbation theory.\u0000</p><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":573,"journal":{"name":"Frontiers of Physics","volume":"19 6","pages":""},"PeriodicalIF":6.5,"publicationDate":"2024-08-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s11467-024-1430-7.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142190174","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
The exploration of magnetism in two-dimensional layered materials has attracted extensive research interest. For the monoclinic phase CrI3 with interlayer antiferromagnetism, finding a static and robust way of realizing the intrinsic interlayer ferromagnetic coupling is desirable. In this work, we study the electronic structure and magnetic properties of the nonmagnetic element (e.g., O, S, Se, N, P, As, and C) doped bi-and triple-layer CrI3 systems via first-principles calculations. Our results demonstrate that O, P, S, As, and Se doped CrI3 bilayer can realize interlayer ferromagnetism. Further analysis shows that the interlayer ferromagnetic coupling in the doped few-layer CrI3 is closely related to the formation of localized spinpolarized state around the doped elements. Further study presents that, for As-doped tri-layer CrI3, it can realize interlayer ferromagnetic coupling. This work proves that nonmagnetic element doping can realize the interlayer ferromagnetically-coupled few-layer CrI3 while maintaining its semiconducting characteristics without introducing additional carriers.
{"title":"Interlayer ferromagnetic coupling in nonmagnetic elements doped CrI3 thin films","authors":"Xuqi Li, Xuyan Chen, Shiyang Sun, Huihui Zhang, Haidan Sang, Xiaonan Wang, Shifei Qi, Zhenhua Qiao","doi":"10.1007/s11467-024-1435-2","DOIUrl":"10.1007/s11467-024-1435-2","url":null,"abstract":"<div><p>The exploration of magnetism in two-dimensional layered materials has attracted extensive research interest. For the monoclinic phase CrI<sub>3</sub> with interlayer antiferromagnetism, finding a static and robust way of realizing the intrinsic interlayer ferromagnetic coupling is desirable. In this work, we study the electronic structure and magnetic properties of the nonmagnetic element (e.g., O, S, Se, N, P, As, and C) doped bi-and triple-layer CrI<sub>3</sub> systems via first-principles calculations. Our results demonstrate that O, P, S, As, and Se doped CrI<sub>3</sub> bilayer can realize interlayer ferromagnetism. Further analysis shows that the interlayer ferromagnetic coupling in the doped few-layer CrI<sub>3</sub> is closely related to the formation of localized spinpolarized state around the doped elements. Further study presents that, for As-doped tri-layer CrI<sub>3</sub>, it can realize interlayer ferromagnetic coupling. This work proves that nonmagnetic element doping can realize the interlayer ferromagnetically-coupled few-layer CrI<sub>3</sub> while maintaining its semiconducting characteristics without introducing additional carriers.\u0000</p><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":573,"journal":{"name":"Frontiers of Physics","volume":"19 6","pages":""},"PeriodicalIF":6.5,"publicationDate":"2024-08-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s11467-024-1435-2.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141923463","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
We investigate the magnetic excitations of the two-dimensional (2D) S = 1/2 trimerized Heisenberg models with intratrimer interaction J1 and intertrimer interaction J2 on four different lattices using a combination of stochastic series expansion quantum Monte Carlo (SSE QMC) and stochastic analytic continuation methods (SAC), complemented by cluster perturbation theory (CPT). These models exhibit quasi-particle-like excitations when g = J2/J1 is weak, characterized by low-energy magnons, intermediate-energy doublons, and high-energy quartons. The low-energy magnons are associated with the magnetic ground states. They can be described by the linear spin wave theory (LSWT) of the effective block spin model and the original spin model. Doublons and quartons emerge from the corresponding internal excitations of the trimers with distinct energy levels, which can be effectively analyzed using perturbative calculation when the ratio of exchange interactions g is weak. In this weak g regime, we observe a clear separation between the magnon and higher-energy spectra. As g increases, doublon and quarton gradually merge into the magnon modes or some continua. Notably, in the Collinear II and trimerized Hexagon lattice, a broad continuum emerges above the single-magnon spectrum, originating from the quasi-1D physics due to the dilute connections between chains. In addition, we also compare our numerical results to the experimental RIXS spectrum and analyze the difference. Our numerical analysis of these 2D trimers yields valuable theoretical predictions and explanations for the inelastic neutron scattering (INS) spectra of 2D magnetic materials featuring trimerized lattices.
我们采用随机序列扩展量子蒙特卡洛(SSE QMC)和随机分析延续方法(SAC),并辅以簇扰动理论(CPT),研究了四种不同晶格上具有内相互作用 J1 和内相互作用 J2 的二维(2D)S = 1/2三元化海森堡模型的磁激发。当 g = J2/J1 很弱时,这些模型表现出准粒子样激发,其特征是低能磁子、中能双子和高能四子。低能磁子与磁基态有关。它们可以用有效块状自旋模型和原始自旋模型的线性自旋波理论(LSWT)来描述。双磁子和四磁子来自具有不同能级的三聚体的相应内部激发,当交换相互作用比 g 很弱时,可以通过微扰计算对它们进行有效分析。在这种弱 g 机制下,我们观察到磁子和高能谱之间存在明显的分离。随着 g 的增大,doublelon 和 quarton 逐渐并入磁子模式或某些连续体。值得注意的是,在 Collinear II 和三元化六边形晶格中,单磁子谱上方出现了一个宽阔的连续体,它源于链之间稀释连接所产生的准一维物理。此外,我们还将数值结果与实验 RIXS 光谱进行了比较,并分析了两者之间的差异。我们对这些二维三聚体的数值分析为具有三聚体晶格的二维磁性材料的非弹性中子散射(INS)谱提供了有价值的理论预测和解释。
{"title":"Magnon, doublon and quarton excitations in 2D S=1/2 trimerized Heisenberg models","authors":"Yue-Yue Chang, Jun-Qing Cheng, Hui Shao, Dao-Xin Yao, Han-Qing Wu","doi":"10.1007/s11467-024-1418-3","DOIUrl":"10.1007/s11467-024-1418-3","url":null,"abstract":"<div><p>We investigate the magnetic excitations of the two-dimensional (2D) <i>S</i> = 1/2 trimerized Heisenberg models with intratrimer interaction <i>J</i><sub>1</sub> and intertrimer interaction <i>J</i><sub>2</sub> on four different lattices using a combination of stochastic series expansion quantum Monte Carlo (SSE QMC) and stochastic analytic continuation methods (SAC), complemented by cluster perturbation theory (CPT). These models exhibit quasi-particle-like excitations when <i>g</i> = <i>J</i><sub>2</sub>/<i>J</i><sub>1</sub> is weak, characterized by low-energy magnons, intermediate-energy doublons, and high-energy quartons. The low-energy magnons are associated with the magnetic ground states. They can be described by the linear spin wave theory (LSWT) of the effective block spin model and the original spin model. Doublons and quartons emerge from the corresponding internal excitations of the trimers with distinct energy levels, which can be effectively analyzed using perturbative calculation when the ratio of exchange interactions <i>g</i> is weak. In this weak <i>g</i> regime, we observe a clear separation between the magnon and higher-energy spectra. As <i>g</i> increases, doublon and quarton gradually merge into the magnon modes or some continua. Notably, in the Collinear II and trimerized Hexagon lattice, a broad continuum emerges above the single-magnon spectrum, originating from the quasi-1D physics due to the dilute connections between chains. In addition, we also compare our numerical results to the experimental RIXS spectrum and analyze the difference. Our numerical analysis of these 2D trimers yields valuable theoretical predictions and explanations for the inelastic neutron scattering (INS) spectra of 2D magnetic materials featuring trimerized lattices.</p><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":573,"journal":{"name":"Frontiers of Physics","volume":"19 6","pages":""},"PeriodicalIF":6.5,"publicationDate":"2024-07-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141780310","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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 simplicity and low-cost way to improve qualitative and quantitative analytical performance has always been a crucial concern for laser-induced breakdown spectroscopy (LIBS), and many scientists have been engaged in this evolving research direction. In this review, we investigated an update on recent developments in light-field modulated operation in LIBS. It covered a brief description of LIBS, optical polarization, and beam shaping. Here, the optical polarization is divided into laser beam polarization and plasma polarization. In addition, the methodology and development of light-field modulated LIBS were summarized and discussed. Finally, the existing problems with light-field modulated LIBS were presented, along with some of their own insights and the future direction of their development. This review will provide a guideline for LIBS researchers with basic knowledge, which is very useful in the signal optimization of LIBS research and applications.
{"title":"Recent advances of light-field modulated operation in laser-induced breakdown spectroscopy","authors":"Shangyong Zhao, Yuchen Zhao, Yujia Dai, Ziyuan Liu, Huihui Zha, Xun Gao","doi":"10.1007/s11467-024-1436-1","DOIUrl":"10.1007/s11467-024-1436-1","url":null,"abstract":"<div><p>The simplicity and low-cost way to improve qualitative and quantitative analytical performance has always been a crucial concern for laser-induced breakdown spectroscopy (LIBS), and many scientists have been engaged in this evolving research direction. In this review, we investigated an update on recent developments in light-field modulated operation in LIBS. It covered a brief description of LIBS, optical polarization, and beam shaping. Here, the optical polarization is divided into laser beam polarization and plasma polarization. In addition, the methodology and development of light-field modulated LIBS were summarized and discussed. Finally, the existing problems with light-field modulated LIBS were presented, along with some of their own insights and the future direction of their development. This review will provide a guideline for LIBS researchers with basic knowledge, which is very useful in the signal optimization of LIBS research and applications.\u0000</p><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":573,"journal":{"name":"Frontiers of Physics","volume":"19 6","pages":""},"PeriodicalIF":6.5,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141780309","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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 : 2024-07-25DOI: 10.1007/s11467-024-1432-5
Julienne Impundu, Wenxiang Wang, Zheng Wei, Yushi Xu, Yu Wang, Jiawang You, Wenbin Huang, Yong Jun Li, Lianfeng Sun
Carbon nanotubes (CNTs) have garnered significant attention due to their remarkable electronic and magnetic properties. In this research, we introduced multiwalled carbon nanotubes covered with tantalum (MWNTs/Ta) to systematically modulate the magnetoresistive properties of the MWNTs/Ta hybrid nanostructures. We observed distinct changes in both positive and negative magnetoresistances of MWNTs/Ta across a broad temperature range using a physical property measurement system and a four-terminal method. This study on temperature-dependent magnetoresistive behavior of the MWNTs/Ta sheds light on the fundamental properties of carbon-based materials and holds promise for practical applications in the field of spintronic devices.
{"title":"Temperature dependence of positive and negative magnetoresistances of tantalum-covered multiwalled carbon nanotubes","authors":"Julienne Impundu, Wenxiang Wang, Zheng Wei, Yushi Xu, Yu Wang, Jiawang You, Wenbin Huang, Yong Jun Li, Lianfeng Sun","doi":"10.1007/s11467-024-1432-5","DOIUrl":"10.1007/s11467-024-1432-5","url":null,"abstract":"<div><p>Carbon nanotubes (CNTs) have garnered significant attention due to their remarkable electronic and magnetic properties. In this research, we introduced multiwalled carbon nanotubes covered with tantalum (MWNTs/Ta) to systematically modulate the magnetoresistive properties of the MWNTs/Ta hybrid nanostructures. We observed distinct changes in both positive and negative magnetoresistances of MWNTs/Ta across a broad temperature range using a physical property measurement system and a four-terminal method. This study on temperature-dependent magnetoresistive behavior of the MWNTs/Ta sheds light on the fundamental properties of carbon-based materials and holds promise for practical applications in the field of spintronic devices.</p><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":573,"journal":{"name":"Frontiers of Physics","volume":"19 6","pages":""},"PeriodicalIF":6.5,"publicationDate":"2024-07-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141780311","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Bilayer (BL) transition metal dichalcogenides (TMDs) are important materials in valleytronics and twistronics. Here we study terahertz (THz) magneto-optical (MO) properties of n-type 2H-stacking BL molybdenum sulfide (MoS2) on sapphire substrate grown by chemical vapor deposition. The AFM, Raman spectroscopy and photoluminescence are used for characterization of the samples. Applying THz time-domain spectroscopy (TDS), in combination with polarization test and the presence of magnetic field in Faraday geometry, THz MO transmissions through the sample are measured from 0 to 8 T at 80 K. The complex right- and left-handed circular MO conductivities for 2H-stacking BL MoS2 are obtained. Through fitting the experimental results with theoretical formula of MO conductivities for an electron gas, generalized by us previously through the inclusion of photon-induced electronic backscattering effect, we are able to determine magneto-optically the key electronic parameters of BL MoS2, such as the electron density ne, the electronic relaxation time τ, the electronic localization factor c and, particularly, the effective electron mass m* around Q-point in between the K- and Γ-point in the electronic band structure. The dependence of these parameters upon magnetic field is examined and analyzed. This is a pioneering experimental work to measure m* around the Q-point in 2H-stacking BL MoS2 and the experimental value is very close to that obtained theoretically. We find that ne/τ/ ∣ c ∣ /m* in 2H-stacking BL MoS2 decreases/increases/decreases/increases with increasing magnetic field. The results obtained from this study can be benefit to us in gaining an in-depth understanding of the electronic and optoelectronic properties of BL TMD systems.
双层(BL)过渡金属二卤化物(TMD)是谷光和双电子学中的重要材料。在此,我们研究了通过化学气相沉积法在蓝宝石衬底上生长的 n 型 2H 叠层 BL 硫化钼(MoS2)的太赫兹(THz)磁光(MO)特性。样品的表征采用了原子力显微镜、拉曼光谱和光致发光技术。应用太赫兹时域光谱(TDS),结合极化测试和法拉第几何中的磁场存在,测量了样品在 80 K 下从 0 到 8 T 的太赫兹 MO 透射率。通过将实验结果与我们之前通过加入光子诱导的电子反向散射效应而归纳出的电子气 MO 导率理论公式进行拟合,我们能够通过磁光确定 BL MoS2 的关键电子参数,如电子密度 ne、电子弛豫时间 τ、电子局域因子 c,尤其是电子带结构中介于 K 点和Γ点之间的 Q 点附近的有效电子质量 m*。研究分析了这些参数对磁场的依赖性。这是一项测量 2H 叠层 BL MoS2 中 Q 点附近 m* 的开创性实验工作,实验值与理论值非常接近。我们发现 2H 叠层 BL MoS2 中的 ne/τ/ ∣ c ∣ /m* 随着磁场的增加而减小/增大/减小/增大。这项研究的结果有助于我们深入了解 BL TMD 系统的电子和光电特性。
{"title":"Key electronic parameters of 2H-stacking bilayer MoS2 on sapphire substrate determined by terahertz magneto-optical measurement in Faraday geometry","authors":"Xingjia Cheng, Wen Xu, Hua Wen, Jing Zhang, Heng Zhang, Haowen Li, Francois M. Peeters","doi":"10.1007/s11467-024-1425-4","DOIUrl":"10.1007/s11467-024-1425-4","url":null,"abstract":"<div><p>Bilayer (BL) transition metal dichalcogenides (TMDs) are important materials in valleytronics and twistronics. Here we study terahertz (THz) magneto-optical (MO) properties of n-type 2<i>H</i>-stacking BL molybdenum sulfide (MoS<sub>2</sub>) on sapphire substrate grown by chemical vapor deposition. The AFM, Raman spectroscopy and photoluminescence are used for characterization of the samples. Applying THz time-domain spectroscopy (TDS), in combination with polarization test and the presence of magnetic field in Faraday geometry, THz MO transmissions through the sample are measured from 0 to 8 T at 80 K. The complex right- and left-handed circular MO conductivities for 2<i>H</i>-stacking BL MoS<sub>2</sub> are obtained. Through fitting the experimental results with theoretical formula of MO conductivities for an electron gas, generalized by us previously through the inclusion of photon-induced electronic backscattering effect, we are able to determine magneto-optically the key electronic parameters of BL MoS<sub>2</sub>, such as the electron density <i>n</i><sub><i>e</i></sub>, the electronic relaxation time <i>τ</i>, the electronic localization factor <i>c</i> and, particularly, the effective electron mass <i>m*</i> around <i>Q</i>-point in between the <i>K</i>- and Γ-point in the electronic band structure. The dependence of these parameters upon magnetic field is examined and analyzed. This is a pioneering experimental work to measure <i>m*</i> around the <i>Q</i>-point in 2<i>H</i>-stacking BL MoS<sub>2</sub> and the experimental value is very close to that obtained theoretically. We find that <i>n</i><sub><i>e</i></sub>/<i>τ</i>/ ∣ <i>c</i> ∣ /<i>m*</i> in 2<i>H</i>-stacking BL MoS<sub>2</sub> decreases/increases/decreases/increases with increasing magnetic field. The results obtained from this study can be benefit to us in gaining an in-depth understanding of the electronic and optoelectronic properties of BL TMD systems.\u0000</p><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":573,"journal":{"name":"Frontiers of Physics","volume":"19 6","pages":""},"PeriodicalIF":6.5,"publicationDate":"2024-07-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141826132","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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 : 2024-07-18DOI: 10.1007/s11467-024-1431-6
Yi Ding, Yanli Wang
As the homologous compounds of MoSi2N4, the MoSi2N4(MoN)n monolayers have been synthesized in a recent experiment. These systems consist of homogeneous metal nitride multilayers sandwiched between two SiN surfaces, which extends the septuple-atomic-layer MSi2N4 system to ultra-thick MSi2N4(MN)n forms. In this paper, we perform a first-principles study on the MoSi2N4(FeN) monolayer, which is constructed by iron molybdenum nitride intercalated into the SiN layers. As a cousin of MoSi2N4(MoN), this double transition-metal system exhibits robust structural stability from the energetic, mechanical, dynamical and thermal perspectives. Different from the MoSi2N4(MoN) one, the MoSi2N4(FeN) monolayer possesses intrinsic ferromagnetism and presents a bipolar magnetic semiconducting behaviour. The ferromagnetism can be further enhanced by the surface hydrogenation, which raises the Curie temperature to 310 K around room temperature. More interestingly, the hydrogenated MoSi2N4(FeN) monolayer exhibits a quantum anomalous Hall (QAH) insulating behaviour with a sizeable nontrivial band gap of 0.23 eV. The nontrivial topological character can be well described by a two-band k · p model, confirming a non-zero Chern number of C = 1. Similar bipolar magnetic semiconducting feature and hydrogenation-induced QAH state are also present in the WSi2N4(FeN) monolayer. Our study demonstrates that the double transition-metal MSi2N4(M′N) system will be a fertile platform to achieve fascinating spintronic and topological properties.
作为 MoSi2N4 的同源化合物,MoSi2N4(MoN)n 单层在最近的实验中被合成出来。这些体系由夹在两个 SiN 表面之间的同质金属氮化物多层组成,从而将七原子层 MSi2N4 体系扩展到超厚 MSi2N4(MN)n 形式。在本文中,我们对 MoSi2N4(FeN)单层进行了第一性原理研究,该单层是由氮化钼铁夹杂在氮化硅层中构成的。作为 MoSi2N4(MoN)的表亲,这种双过渡金属体系从能量、机械、动力学和热学角度来看都表现出强大的结构稳定性。与 MoSi2N4(MoN)不同,MoSi2N4(FeN)单层具有内在铁磁性,并呈现出双极磁性半导体行为。表面氢化可进一步增强铁磁性,使居里温度升至室温附近的 310 K。更有趣的是,氢化的 MoSi2N4(FeN)单层表现出量子反常霍尔(QAH)绝缘特性,其非对称带隙高达 0.23 eV。这种非对称拓扑特性可以用双带 k - p 模型很好地描述,证实了 C = 1 的非零切尔诺数。类似的双极磁性半导体特征和氢化诱导的 QAH 状态也出现在 WSi2N4(FeN)单层中。我们的研究表明,双过渡金属 MSi2N4(M′N) 体系将是实现迷人的自旋电子学和拓扑特性的肥沃平台。
{"title":"First-principles investigation of two-dimensional iron molybdenum nitride: A double transition-metal cousin of MoSi2N4(MoN) monolayer with distinctive electronic and topological properties","authors":"Yi Ding, Yanli Wang","doi":"10.1007/s11467-024-1431-6","DOIUrl":"10.1007/s11467-024-1431-6","url":null,"abstract":"<div><p>As the homologous compounds of MoSi<sub>2</sub>N<sub>4</sub>, the MoSi<sub>2</sub>N<sub>4</sub>(MoN)<sub><i>n</i></sub> monolayers have been synthesized in a recent experiment. These systems consist of homogeneous metal nitride multilayers sandwiched between two SiN surfaces, which extends the septuple-atomic-layer MSi<sub>2</sub>N<sub>4</sub> system to ultra-thick MSi<sub>2</sub>N<sub>4</sub>(MN)<sub><i>n</i></sub> forms. In this paper, we perform a first-principles study on the MoSi<sub>2</sub>N<sub>4</sub>(FeN) monolayer, which is constructed by iron molybdenum nitride intercalated into the SiN layers. As a cousin of MoSi<sub>2</sub>N<sub>4</sub>(MoN), this double transition-metal system exhibits robust structural stability from the energetic, mechanical, dynamical and thermal perspectives. Different from the MoSi<sub>2</sub>N<sub>4</sub>(MoN) one, the MoSi<sub>2</sub>N<sub>4</sub>(FeN) monolayer possesses intrinsic ferromagnetism and presents a bipolar magnetic semiconducting behaviour. The ferromagnetism can be further enhanced by the surface hydrogenation, which raises the Curie temperature to 310 K around room temperature. More interestingly, the hydrogenated MoSi<sub>2</sub>N<sub>4</sub>(FeN) monolayer exhibits a quantum anomalous Hall (QAH) insulating behaviour with a sizeable nontrivial band gap of 0.23 eV. The nontrivial topological character can be well described by a two-band <i>k · p</i> model, confirming a non-zero Chern number of <i>C</i> = 1. Similar bipolar magnetic semiconducting feature and hydrogenation-induced QAH state are also present in the WSi<sub>2</sub>N<sub>4</sub>(FeN) monolayer. Our study demonstrates that the double transition-metal MSi<sub>2</sub>N<sub>4</sub>(M′N) system will be a fertile platform to achieve fascinating spintronic and topological properties.\u0000</p><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":573,"journal":{"name":"Frontiers of Physics","volume":"19 6","pages":""},"PeriodicalIF":6.5,"publicationDate":"2024-07-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141827052","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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 : 2024-07-17DOI: 10.1007/s11467-024-1423-6
Desheng Cai, Yumin Xia, Pengju Li, Kun Xie, Yuzhou Liu, Yitong Gu, Gan Yu, Changgan Zeng, Ping Cui, Shengyong Qin
Cobalt pnictides have been theoretically proposed to be attractive candidates for high-temperature superconductors. Additionally, monolayered CoX (X = As, Sb, Bi) on SrTiO3 systems present a potential new platform for realizing topological superconductors in the two-dimensional limit, due to their nontrivial band topology. To this end, we have successfully fabricated high-quality CoBi nanoislands on SrTiO3 (001) substrates by molecular beam epitaxy followed by an investigation of their atomic structure and electronic properties via in situ scanning tunneling microscopy/spectroscopy. Beyond the previously predicted lattice with a = b = 3.5 Å, 2 × 1 dimer row was observed in this study. Furthermore, our results reveal that the topography of CoBi islands is strongly influenced by various growth conditions, such as substrate temperature, the flux ratio between Co and Bi, and the annealing process. This study paves the way for further explorations of the superconductivity and topological properties of cobalt pnictide systems.
从理论上讲,铌钴化物是具有吸引力的高温超导体候选材料。此外,SrTiO3 系统上的单层 CoX(X = As、Sb、Bi)由于其非三维带拓扑结构,为实现二维极限拓扑超导体提供了一个潜在的新平台。为此,我们通过分子束外延技术在 SrTiO3 (001) 基底上成功制备了高质量的 CoBi 纳米岛,并通过原位扫描隧道显微镜/光谱仪对其原子结构和电子特性进行了研究。除了先前预测的 a = b = 3.5 Å 晶格外,本研究还观察到 2 × 1 二聚体行。此外,我们的研究结果表明,钴铋岛的形貌受到各种生长条件的强烈影响,如衬底温度、钴和铋之间的通量比以及退火过程。这项研究为进一步探索锑化钴系统的超导和拓扑特性铺平了道路。
{"title":"Multi-conditioned controlled growth of CoBi nanostructures on SrTiO3","authors":"Desheng Cai, Yumin Xia, Pengju Li, Kun Xie, Yuzhou Liu, Yitong Gu, Gan Yu, Changgan Zeng, Ping Cui, Shengyong Qin","doi":"10.1007/s11467-024-1423-6","DOIUrl":"10.1007/s11467-024-1423-6","url":null,"abstract":"<div><p>Cobalt pnictides have been theoretically proposed to be attractive candidates for high-temperature superconductors. Additionally, monolayered CoX (X = As, Sb, Bi) on SrTiO<sub>3</sub> systems present a potential new platform for realizing topological superconductors in the two-dimensional limit, due to their nontrivial band topology. To this end, we have successfully fabricated high-quality CoBi nanoislands on SrTiO<sub>3</sub> (001) substrates by molecular beam epitaxy followed by an investigation of their atomic structure and electronic properties via in situ scanning tunneling microscopy/spectroscopy. Beyond the previously predicted lattice with <i>a</i> = <i>b</i> = 3.5 Å, 2 × 1 dimer row was observed in this study. Furthermore, our results reveal that the topography of CoBi islands is strongly influenced by various growth conditions, such as substrate temperature, the flux ratio between Co and Bi, and the annealing process. This study paves the way for further explorations of the superconductivity and topological properties of cobalt pnictide systems.\u0000</p><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":573,"journal":{"name":"Frontiers of Physics","volume":"19 6","pages":""},"PeriodicalIF":6.5,"publicationDate":"2024-07-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141828344","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}