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Research on spatial frequency shift super-resolution imaging based on evanescent wave illumination 基于倏逝波照明的空间频移超分辨成像研究
Pub Date : 2023-01-01 DOI: 10.7498/aps.72.20230934
None Ling Jin-Zhong, None Guo Jin-Kun, None Wang Yu-cheng, None Liu Xin, None Wang Xiao-rui
In spite of the success of fluorescence microscopes (such as STED, STORM and PALM) in biomedical field, which have realized nanometer scale imaging resolution and promoted the great development of bio-medicine, the super-resolution imaging method for non-fluorescent sample is still scarce, and the resolution still has a big gap to nanometer scale. Among existing methods, structured illumination microscopy, PSF engineering, super-oscillatory lens and microsphere assisted nanoscopy are more mature and widely applied. However, limited by the theory itself or engineering practice, the resolution of these approaches is hard to break through 50 nm, which restricts their application in many fields.
Enlightened by synthetic aperture technique, researchers proposed spatial frequency shift super-resolution microscopy through shifting and combining the spatial frequency spectrum of imaging target, which is a promising super-resolution imaging scheme as its resolution limit could be broken through continually. Currently, due to the restriction of the refractive index of optical materials, the wavelength of illumination evanescent wave is hard to be shorten when generated at prism surface via total internal reflection, which determines the highest resolution of this spatial frequency shift super-resolution imaging system. Another deficiency of this scheme is the difference of imaging resolution in different directions, as only in the direction along the wave vector of illumination evanescent wave, the image has the highest resolution; while in the direction perpendicular to it, the image has the lowest resolution, as same as that obtained by far-field illumination.
In order to solve the above thorny questions, a new model for evanescent wave generation has been proposed, which could generate omnidirectional evanescent wave with arbitrary wavelength based the phase modulation of nano-structure, and solve the both problem in imaging system at the same time. To verify the possibility of our scheme, we set up a complete simulation model for spatial frequency shift imaging scheme, which includes three parts:the generation of evanescent wave and its interaction with the nano-structures at imaging target, with could be simulated with FDTD algorithm; the propagation of light field from near-field to far-field, from the sample surface to the focal plane of objective lens, which could be calculated with angular spectrum theory; the propagation of light field from the focal place to the image plane, which could be calculated with Chirp-Z transform.
With this complete simulation model, we compared the resolution of microscopy illuminated by evanescent wave and propagating wave, firstly. The results verified the super-resolution imaging ability of evanescent wave illumination, and also demonstrated the influence of refractive index of prism, as higher refractive index makes shorter wavelength of evanescent wave and higher resolution of spatial frequency shift
尽管荧光显微镜(如STED、STORM和PALM)在生物医学领域取得了成功,实现了纳米级成像分辨率,促进了生物医学的巨大发展,但非荧光样品的超分辨率成像方法仍然稀缺,分辨率与纳米级仍有很大差距。在现有的方法中,结构照明显微镜、PSF工程、超振荡透镜和微球辅助纳米显微镜技术较为成熟,应用较为广泛。然而,受理论本身或工程实践的限制,这些方法的分辨率很难突破50 nm,这限制了它们在许多领域的应用。<br/>在合成孔径技术的启发下,研究人员通过移动和组合成像目标的空间频谱,提出了空间频移超分辨率显微镜。它的分辨率极限可以不断突破,是一种很有前途的超分辨率成像方案。目前,由于光学材料折射率的限制,在棱镜表面经全内反射产生的照明倏逝波波长难以缩短,这决定了该空间频移超分辨成像系统的最高分辨率。该方案的另一个不足是成像分辨率在不同方向上存在差异,只有在照明倏逝波的波矢量方向上,图像的分辨率才最高;为解决上述棘手的问题,本文提出了一种新的倏逝波产生模型,该模型可以基于纳米结构的相位调制产生任意波长的全向倏逝波,同时解决了成像系统中的这两个问题。为了验证该方案的可行性,我们建立了一个完整的空间频移成像方案的仿真模型,该模型包括三个部分:倏逝波的产生及其与成像目标纳米结构的相互作用,可以用FDTD算法进行模拟;光场从近场到远场,从样品表面到物镜焦平面的传播,可以用角谱理论计算;用Chirp-Z变换可以计算出光场从焦点到像面的传播。<br/>在这个完整的仿真模型下,我们首先比较了倏逝波和传播波照射下显微镜的分辨率。结果验证了倏逝波照明的超分辨成像能力,同时也证明了棱镜折射率的影响,折射率越高,倏逝波波长越短,空间频移成像系统的分辨率越高。其次,我们演示了三棒成像目标旋转不同方向时在一系列方向上的分辨率差异。结果表明,成像分辨率最高的方向为照明倏逝波矢量方向,成像分辨率最低的方向为垂直于照明倏逝波矢量方向。最后,对纳米结构产生的倏逝波进行了模拟,验证了其波长特性和矢量方向特性。当应用于近场照明超分辨成像时,全向倏逝波解决了棱镜表面全内反射模型存在的这两个问题。因此,我们方案的优点是成像分辨率更高,成像速度更快,不需要多方向多次成像,无需图像后处理。我们的研究为空间频移超分辨率成像开辟了一个新的视角,为其应用奠定了理论基础。
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引用次数: 0
Spin-polarized transport properties in diluted-magnetic-semiconductor/semiconductor superlattices under light-field assisted 光场辅助下稀磁半导体/半导体超晶格的自旋极化输运性质
Pub Date : 2023-01-01 DOI: 10.7498/aps.72.20230935
None Li Chun-Lei, None Zheng Jun, None Wang Xiao-Ming, None Xu Yan
Based on the single electron effective mass approximation theory and the transfer-matrix method, the spin polarized transport properties of electrons in a diluted-magnetic-semiconductor/semiconductor superlattice are studied. The influence of a light-field and a magnetic-field on spin polarized transport and the tunneling time in the superlattice structure are discussed in more detail. The results show that, due to the sp-d electron interaction between conduction band electrons and doped Mn ions, giant Zeeman splitting occurs. It is shown that a significant spin-dependent transmission and the position and width of the resonant-transmission-band of spin-dependent electron can be manipulated by adjusting the magnetic- and light-field. Considering the light field irradiation, the resonance band of electron is deformed and broadened with the increase of the light field intensity. For the case of a strong magnetic field, the transmission coefficient (TC) in the low-energy region is almost zero when the light field is not added, but with the increase of light intensity, the TC increased significantly in the zone increases significantly, that is, a quasi-bound band appears. These features are due to the energy exchange between electrons and the light field when electrons tunnel through the superlattice structure under light irradiation. In addition, light and magnetic fields can significantly change the spin polarization of electrons. Under a certain magnetic field intensity (B=2 T), the light field significantly changes the spin polarization of electrons, the main effect is that the width of the spin polarization platform narrows and oscillatory peaks are accompanied on both sides of the platform. This effect is strengthened with the increase of the light field intensity. However, when the magnetic field is stronger (B=5 T), the opposite is true. These show that the spin polarization can be modulated by the light field. Finally, the tunneling time of spin-up and spin-down electrons is studied by the evolution of Gaussian wave packets in the structure. The results show that the tunneling time depends on a spin of electrons, and it can be seen that the tunneling time of the spin-down electron is shorter than that of the spin-up electron in the superlattice structure. These remarkable properties of spin polarized transport may be beneficial for the devising tunable spin filtering devices based on diluted magnetic semiconductor/semiconductor superlattice structure.
基于单电子有效质量近似理论和传递矩阵方法,研究了稀释磁性半导体/半导体超晶格中电子的自旋极化输运性质。详细讨论了光场和磁场对超晶格结构中自旋极化输运和隧穿时间的影响。结果表明,由于导带电子与掺杂Mn离子之间的sp-d电子相互作用,发生了巨大的塞曼分裂。结果表明,通过调节磁场和光场,可以控制自旋相关电子的显著自旋相关透射率和共振透射带的位置和宽度。考虑光场辐照,随着光场强度的增加,电子的共振带发生变形和展宽。在强磁场的情况下,不加光场时,低能区的透射系数(TC)几乎为零,但随着光强的增加,该区域的透射系数(TC)显著增加,即出现准束缚带。这些特征是由于电子在光照射下隧穿超晶格结构时与光场之间的能量交换。此外,光和磁场可以显著改变电子的自旋极化。在一定的磁场强度下(<i> </i>=2 T),光场显著改变了电子的自旋极化,主要影响是自旋极化平台的宽度变窄,平台两侧出现振荡峰。这种效应随着光场强度的增加而增强。然而,当磁场较强时(<i>B</i>= 5t),情况正好相反。这些结果表明,自旋极化可以被光场调制。最后,通过结构中高斯波包的演化,研究了自旋向上和自旋向下电子的隧穿时间。结果表明,隧穿时间取决于电子的自旋,并且可以看出,在超晶格结构中,自旋向下的电子的隧穿时间比自旋向上的电子短。自旋极化输运的这些显著性质可能有助于设计基于稀释磁性半导体/半导体超晶格结构的可调谐自旋滤波器件。
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引用次数: 0
Edge states and skin effect dependent electron transport properties of a non-Hermitian Su-Schrieffer-Heeger chain 非厄米Su-Schrieffer-Heeger链的边缘态和趋肤效应相关的电子输运性质
Pub Date : 2023-01-01 DOI: 10.7498/aps.72.20231286
None Yang Yan-Li, None Duan Zhi-Lei, None Xue Hai-Bin
In the non-reciprocal Su-Schrieffer-Heeger (SSH) chain, the hopping amplitude of an electron in the intra-cell depends on its hopping direction. Consequently, the non-Hermitian SSH chain has both non-trivial topological edge states and non-Hermitian skin effect. However, how to detect the non-trivial topological edge states and non-Hermitian skin effect have become an important topics in non-Hermitian physics. In this paper, we have studied the dependences of the non-trivial topological edge states and the non-Hermitian skin effect of non-Hermitian SSH chain on their electron transport properties in the vicinity of the zero energy. It is demonstrated that when the peak value of the electron transmission probability in the vicinity of the zero energy is much smaller than 1, the non-Hermitian SSH chain has a left-non-Hermitian skin effect; while that in the vicinity of the zero energy is much larger than 1, the non-Hermitian SSH chain has a right-non-Hermitian skin effect. In particular, the skin effect of non-Hermitian SSH chain can be further enhanced in the region of non-trivial topological edge states. Moreover, with increasing the electron tunneling coupling amplitudes between the non-Hermitian SSH chain and the left and right leads from the weak coupling regime to the strong coupling one, the number of the dips of reflection probability in the vicinity of the zero energy will change from two to zero. Therefore, these results theoretically provide an alternative scheme for detecting non-trivial topological edge states and non-Hermitian skin effect types of the non-Hermitian SSH chain.
在非互反的Su-Schrieffer-Heeger (SSH)链中,电子在细胞内的跳跃幅度取决于其跳跃方向。因此,非厄米SSH链具有非平凡拓扑边缘状态和非厄米集肤效应。然而,如何检测非平凡拓扑边缘状态和非厄米集肤效应已成为非厄米物理中的一个重要课题。本文研究了非厄米原子链的非平凡拓扑边缘态和非厄米原子链的非厄米集肤效应与它们在零能量附近的电子输运性质的关系。结果表明,当电子在零能量附近的透射概率峰值远小于1时,非厄米SSH链具有左非厄米集肤效应;而在零能级附近的能量远大于1,非厄米SSH链具有右非厄米集肤效应。特别是,在非平凡拓扑边缘状态区域,非厄米SSH链的趋肤效应可以进一步增强。此外,随着非厄米SSH链与左右导联之间的电子隧穿耦合幅值的增加,从弱耦合区到强耦合区,在零能量附近反射概率的下降数将从2变为0。因此,这些结果在理论上为检测非厄米SSH链的非平凡拓扑边缘状态和非厄米skin效应类型提供了一种替代方案。
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引用次数: 0
Recent progress on PbTe Majorana nanowires PbTe Majorana纳米线的研究进展
Pub Date : 2023-01-01 DOI: 10.7498/aps.72.20231603
None Yang Shuai, None Zhang Hao, None He Ke
Semiconductor-superconductor hybrid nanowire is one of the major platforms for realizing Majorana zero modes (MZMs) and topological quantum computing (TQC), and the III-V InAs and InSb-based nanowires are the most-studied materials in this approach. Despite years of efforts on material improvement and optimization, the too many defects and impurities in the nanowire samples remain the central problem hindering the research progress in the direction. In recent years, a new candidate Majorana nanowire system— IV-VI semiconductor PbTe-superconductor hybrid nanowire—have attracted much attention and witnessed rapid research progress. The unique advantages of PbTe-based nanowires, such as the large dielectric constant and the existence of a lattice-matched substrate, grant them great potential in overcoming the bottleneck problem of sample defects and impurities and becoming an ideal platform to study MZMs and TQC. In this paper, we briefly introduce the recent research progress on selective area growth and transport characterization of in-plane PbTe nanowires and PbTe-superconductor hybrid nanowires, and discuss the advantages and problems of the new candidate Majorana nanowire system, as well as the prospective of realizing TQC based on it.
半导体-超导混合纳米线是实现马约拉纳零模式(MZMs)和拓扑量子计算(TQC)的主要平台之一,其中III-V InAs和insb基纳米线是该方法中研究最多的材料。尽管经过多年的材料改进和优化,但纳米线样品中缺陷和杂质过多仍然是阻碍研究方向进展的核心问题。近年来,一种新的马约拉纳纳米线候选体系——ⅳ-ⅵ半导体pbte -超导杂化纳米线备受关注,研究进展迅速。pbte基纳米线具有较大的介电常数和晶格匹配衬底等独特优势,这使其在克服样品缺陷和杂质等瓶颈问题方面具有很大的潜力,成为研究MZMs和TQC的理想平台。本文简要介绍了平面内PbTe纳米线和PbTe-超导体混合纳米线的选择性面积生长和输运特性的最新研究进展,讨论了新型候选Majorana纳米线系统的优点和存在的问题,以及基于该系统实现TQC的前景。
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引用次数: 0
Calculation of nucleon scattering on <sup>40</sup>Ca based on dispersive optical model 基于色散光学模型的核子在&lt;sup&gt;40&lt;/sup&gt;Ca上的散射计算
Pub Date : 2023-01-01 DOI: 10.7498/aps.72.20231054
None Zhao Xiu-Niao, None Du Wen-Qing
Spherical nucleus 40Ca is important structural and alloy material nucleus. Based on important theoretical value and application prospect of nuclear data of calcium isotopes, nucleon-nucleus scattering data on 40Ca nucleus, the main isotopes of natural calcium, are calculated by using dispersive optical model (DOM). The dispersive optical model potential is defined by energy-dependent real potentials, imaginary potentials, and also by the corresponding dispersive contributions to the real potential which are calculated analytically from the corresponding imaginary potentials by using a dispersion relation that follow from the requirement of causality. By fit simultaneously scattering experimental data for neutron and proton, an isospin-dependent dispersive optical model potential containing a dispersive term is derived. This derived potential in this work considers the nonlocality in the real “Hartree-Fock” potential begin{document}$ V_{rm{HF}} $end{document} and introduces the shell gap in the definition of nuclear imaginary volume, surface and spin-orbit potentials near the Fermi energy. This dispersive optical model potential shows a good description of nucleon-nucleus scattering data on 40Ca nucleus up to 200 MeV including neutron total cross sections, neutron elastic scattering angular distributions, proton elastic scattering angular distributions, neutron analyzing powers and proton analyzing powers. In addition, the energy dependencies of calculated real volume integrals of dispersive optical model potential is shown, and a typical dispersive hump is seen around the Fermi energy. This dispersive hump behavior naturally obtained from dispersion relations, and allows the dispersion optical potential to get rid of energy dependent geometry, thus avoiding the use of a radius dependent on energy.
Spherical nucleus <sup>40</sup>Ca is important structural and alloy material nucleus. Based on important theoretical value and application prospect of nuclear data of calcium isotopes, nucleon-nucleus scattering data on <sup>40</sup>Ca nucleus, the main isotopes of natural calcium, are calculated by using dispersive optical model (DOM). The dispersive optical model potential is defined by energy-dependent real potentials, imaginary potentials, and also by the corresponding dispersive contributions to the real potential which are calculated analytically from the corresponding imaginary potentials by using a dispersion relation that follow from the requirement of causality. By fit simultaneously scattering experimental data for neutron and proton, an isospin-dependent dispersive optical model potential containing a dispersive term is derived. This derived potential in this work considers the nonlocality in the real “Hartree-Fock” potential <inline-formula><tex-math id="M5">begin{document}$ V_{rm{HF}} $end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="22-20231054_M5.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="22-20231054_M5.png"/></alternatives></inline-formula> and introduces the shell gap in the definition of nuclear imaginary volume, surface and spin-orbit potentials near the Fermi energy. This dispersive optical model potential shows a good description of nucleon-nucleus scattering data on <sup>40</sup>Ca nucleus up to 200 MeV including neutron total cross sections, neutron elastic scattering angular distributions, proton elastic scattering angular distributions, neutron analyzing powers and proton analyzing powers. In addition, the energy dependencies of calculated real volume integrals of dispersive optical model potential is shown, and a typical dispersive hump is seen around the Fermi energy. This dispersive hump behavior naturally obtained from dispersion relations, and allows the dispersion optical potential to get rid of energy dependent geometry, thus avoiding the use of a radius dependent on energy.
{"title":"Calculation of nucleon scattering on &lt;sup&gt;40&lt;/sup&gt;Ca based on dispersive optical model","authors":"None Zhao Xiu-Niao, None Du Wen-Qing","doi":"10.7498/aps.72.20231054","DOIUrl":"https://doi.org/10.7498/aps.72.20231054","url":null,"abstract":"Spherical nucleus <sup>40</sup>Ca is important structural and alloy material nucleus. Based on important theoretical value and application prospect of nuclear data of calcium isotopes, nucleon-nucleus scattering data on <sup>40</sup>Ca nucleus, the main isotopes of natural calcium, are calculated by using dispersive optical model (DOM). The dispersive optical model potential is defined by energy-dependent real potentials, imaginary potentials, and also by the corresponding dispersive contributions to the real potential which are calculated analytically from the corresponding imaginary potentials by using a dispersion relation that follow from the requirement of causality. By fit simultaneously scattering experimental data for neutron and proton, an isospin-dependent dispersive optical model potential containing a dispersive term is derived. This derived potential in this work considers the nonlocality in the real “Hartree-Fock” potential <inline-formula><tex-math id=\"M5\">begin{document}$ V_{rm{HF}} $end{document}</tex-math><alternatives><graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"22-20231054_M5.jpg\"/><graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"22-20231054_M5.png\"/></alternatives></inline-formula> and introduces the shell gap in the definition of nuclear imaginary volume, surface and spin-orbit potentials near the Fermi energy. This dispersive optical model potential shows a good description of nucleon-nucleus scattering data on <sup>40</sup>Ca nucleus up to 200 MeV including neutron total cross sections, neutron elastic scattering angular distributions, proton elastic scattering angular distributions, neutron analyzing powers and proton analyzing powers. In addition, the energy dependencies of calculated real volume integrals of dispersive optical model potential is shown, and a typical dispersive hump is seen around the Fermi energy. This dispersive hump behavior naturally obtained from dispersion relations, and allows the dispersion optical potential to get rid of energy dependent geometry, thus avoiding the use of a radius dependent on energy.","PeriodicalId":10252,"journal":{"name":"Chinese Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135400405","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Experimental and theoretical study of parallel models for thermoelectric properties of double-layer thermoelectric thin films 双层热电薄膜热电特性平行模型的实验与理论研究
Pub Date : 2023-01-01 DOI: 10.7498/aps.72.20231259
None Yang Shi-Guan, None 孙志刚, None Lin Xin, None He Jun-Song, None Zhai Li-Jun, None Cheng Lin, None Lv Ming Hao, None Liu Hong-Xia, None Sun Zhi-Gang
Currently, the measurement and prediction of the electrical transport performance of thermoelectric double-layer membranes is often based on the theory of parallel modelling, however, the conditions for the use of parallel modelling lack theoretical and experimental support and validation. In this paper, the Seebeck coefficients of Cu/Si and Ag/Si bilayers under applied temperature difference are obtained by using finite element theory simulations with the help of COMSOL Multiphysics software and compared with the parallel model. The effects of whether the ends of the bilayer are plated with a metal Pt layer or not, and the insertion of a high-resistance/low-resistance/insulation interface between the bilayers on the Seebeck coefficient measurements of the bilayer are investigated. It is found that when there is no Pt at the hot and cold ends, the potentials on the Si and Cu sides at the high-resistance and electrically insulating interfaces are uniformly distributed along the direction of the temperature gradient, respectively, and the measured Seebeck coefficients are the same as the value of the material itself, respectively, and the thermal potentials on the Cu side at the low-resistance interfaces vary uniformly with the probe spacing L, while the Si side shows a non-uniform variation. With Pt, the thermal potentials on the Cu and Si sides are uniformly distributed along the direction of the temperature gradient, and the measured values on both Si and Cu sides are the same as the Cu Seebeck coefficients, regardless of the insulating/high-resistance/low-resistance interface. Si/Ag and Bi/Ag bilayers were experimentally investigated. In the absence of Pt, the absolute value of the Seebeck coefficient on the Si side of Si/Ag bilayers decreased with decreasing temperature, but the absolute value of the Seebeck coefficient on the Ag side increased with decreasing temperature. In the presence of Pt, the Seebeck coefficients are the same on both sides of the Bi/Ag bilayer membrane.
目前,热电双层膜电输运性能的测量和预测往往基于并行建模理论,然而,使用并行建模的条件缺乏理论和实验的支持和验证。本文利用COMSOL Multiphysics软件对Cu/Si和Ag/Si双层材料在外加温差下的塞贝克系数进行了有限元理论模拟,并与并行模型进行了比较。研究了双层膜两端是否镀金属Pt层、双层膜之间是否插入高阻/低阻/绝缘界面对双层膜塞贝克系数测量的影响。结果发现,当冷热端不存在Pt时,高阻和电绝缘界面处Si侧和Cu侧的电势分别沿温度梯度方向均匀分布,测得的塞贝克系数分别与材料本身的值相同,低阻界面处Cu侧的热势随探针间距L均匀变化。而Si侧则表现出不均匀的变化。Pt时,无论绝缘/高阻/低阻界面如何,Cu侧和Si侧的热势沿温度梯度方向均匀分布,且Si侧和Cu侧的测量值与Cu的Seebeck系数相同。实验研究了Si/Ag和Bi/Ag双分子层。在Pt不存在的情况下,Si/Ag双分子层Si侧的Seebeck系数绝对值随温度的降低而减小,而Ag侧的Seebeck系数绝对值随温度的降低而增大。Pt存在时,Bi/Ag双膜两侧的塞贝克系数相同。
{"title":"Experimental and theoretical study of parallel models for thermoelectric properties of double-layer thermoelectric thin films","authors":"None Yang Shi-Guan, None 孙志刚, None Lin Xin, None He Jun-Song, None Zhai Li-Jun, None Cheng Lin, None Lv Ming Hao, None Liu Hong-Xia, None Sun Zhi-Gang","doi":"10.7498/aps.72.20231259","DOIUrl":"https://doi.org/10.7498/aps.72.20231259","url":null,"abstract":"Currently, the measurement and prediction of the electrical transport performance of thermoelectric double-layer membranes is often based on the theory of parallel modelling, however, the conditions for the use of parallel modelling lack theoretical and experimental support and validation. In this paper, the Seebeck coefficients of Cu/Si and Ag/Si bilayers under applied temperature difference are obtained by using finite element theory simulations with the help of COMSOL Multiphysics software and compared with the parallel model. The effects of whether the ends of the bilayer are plated with a metal Pt layer or not, and the insertion of a high-resistance/low-resistance/insulation interface between the bilayers on the Seebeck coefficient measurements of the bilayer are investigated. It is found that when there is no Pt at the hot and cold ends, the potentials on the Si and Cu sides at the high-resistance and electrically insulating interfaces are uniformly distributed along the direction of the temperature gradient, respectively, and the measured Seebeck coefficients are the same as the value of the material itself, respectively, and the thermal potentials on the Cu side at the low-resistance interfaces vary uniformly with the probe spacing L, while the Si side shows a non-uniform variation. With Pt, the thermal potentials on the Cu and Si sides are uniformly distributed along the direction of the temperature gradient, and the measured values on both Si and Cu sides are the same as the Cu Seebeck coefficients, regardless of the insulating/high-resistance/low-resistance interface. Si/Ag and Bi/Ag bilayers were experimentally investigated. In the absence of Pt, the absolute value of the Seebeck coefficient on the Si side of Si/Ag bilayers decreased with decreasing temperature, but the absolute value of the Seebeck coefficient on the Ag side increased with decreasing temperature. In the presence of Pt, the Seebeck coefficients are the same on both sides of the Bi/Ag bilayer membrane.","PeriodicalId":10252,"journal":{"name":"Chinese Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135400648","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Dual-mode up/down-conversion optical thermometry of Pr<sup>3+</sup>-regulated Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub>:Er<sup>3+</sup> phosphors Pr&lt;sup&gt;3+&lt;/sup&gt;调节Li&lt;sub&gt;0.9&lt;/sub&gt;K&lt;sub&gt;0.1&lt;/sub&gt;NbO&lt;sub&gt;3&lt;/sub&gt; Er&lt;sup&gt;3+&lt;/sup&gt;荧光粉
Pub Date : 2023-01-01 DOI: 10.7498/aps.72.20231170
None Jia Chao-Yang, None Yang Xue, None Wang Zhi-Gang, None Chai Rui-Peng, None Pang Qing, None Zhang Xiang-Yu, None Gao Dang-Li
Photothermal sensing is crucial for the development of smart wearable devices. However, designing and synthesizing luminescent materials with suitable multi-wavelength emission and constructing multiple sets of probes in a single material system is a huge challenge for constructing sensitive temperature sensors with a wide temperature range. In this paper, Pr3+, Er3+ single-doped and double-doped Li0.9K0.1NbO3 phosphors were successfully prepared by high temperature solid phase method, and their structure, morphology, excitation wavelength and temperature-dependent fluorescence properties were characterized by XRD, SEM, fluorescence spectrometer and self-made heating device. Firstly, the photoluminescence of the synthesized series of samples was investigated. The results show that compared with the single-doped Li0.9K0.1NbO3: Er3+sample, the up/down-conversion spectra of Pr3+, Er3+ co-doped phosphors under 808/380 nm excitation show that the green fluorescence emission of Er3+ is enhanced. In addition, under 980 nm excitation, Pr3+ can effectively regulate the fluorescence energy level population pathway, so that the electrons are more effectively arranged in the 2H11/2 and 4S3/2 energy levels during the excitation process. The red emission is weakened and the green emission is enhanced, which improves the signal resolution of the fluorescent material and has a significant impact on the optical temperature measurement. Secondly, the up-conversion fluorescence property of Er3+ under 808/980 nm laser excitation in Li0.9K0.1NbO3:Er3+and Li0.9K0.1NbO3:Pr3+,Er3+phosphors were investigated. The results show that the red and green fluorescence emissions of Er3+ are two-photon processes. Finally, the up/down-conversion dual-mode temperature sensing properties of Er3+ in Li0.9K0.1NbO3:Er3+ and Li0.9K0.1NbO3:Pr3+,Er3+ phosphors were investigated. It was found that both materials have good optical temperature measurement performance. Pr3+ doping optimizes the dual-mode optical temperature measurement performance of Li0.9K0.1NbO3:Er3+ phosphors derived from the thermal coupling energy level of Er3+ions. In addition, the up/down-conversion fluorescence mechanism of Li0.9K0.1NbO3:Er3+ and Li0.9K0.1NbO3:Er3+,Pr3+ phosphors is proposed, and the enhanced green fluorescence by Pr3+ co-doping is attributed to the energy transfer from Pr3+ to Er3+ ions, leading
光热传感对于智能可穿戴设备的发展至关重要。然而,设计和合成具有合适的多波长发射的发光材料,并在单一材料体系中构建多组探头,对于构建宽温度范围的敏感温度传感器是一个巨大的挑战。摘要Pr< sup> 3 + & lt; / sup> Er< sup> 3 + & lt; / sup>单掺杂和双掺杂Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub>采用高温固相法成功制备了荧光粉,并利用XRD、SEM、荧光光谱仪和自制加热装置对其结构、形貌、激发波长和温度依赖性荧光性质进行了表征。首先,研究了合成的系列样品的光致发光性能。结果表明:与单掺杂的Li<sub>0.9</sub>K<sub>0.1</sub> nbo>3</sub> 3+</sup>样品相比,Pr<sup>3+</sup>共掺杂荧光粉在808/380 nm激发下,Er<sup>3+<是增强。此外,在980 nm激发下,Pr<sup>3+</sup>能有效调节荧光能级居子通路,使电子更有效地排列在<sup>2</sup>H<sub>11/2</sub>和& lt; sup> 4 & lt; / sup> S< sub> 3/2< / sub>激发过程中的能级。红光发射减弱,绿光发射增强,提高了荧光材料的信号分辨率,对光学测温有重要影响。其次,Er<sup>3+</sup>在808/980 nm激光激发下,对Li<sub>0.9</sub>K<sub>0.1</sub> nbo>3+</ sub> Er< 3+</ sub>K<sub>0.1</sub> nbo>3+</ sub> Pr<sup>3+</sup> Er<sup>3+</sup> Er<sup>3+</sup>进行了研究。结果表明,Er<sup>3+</sup>都是双光子过程。最后,对Er<sup>3+</sup>在Li< sub> 0.9 & lt; / sub> K< sub> 0.1 & lt; / sub> NbO< sub> 3 & lt; / sub>: Er< sup> 3 + & lt; / sup>和Li< sub> 0.9 & lt; / sub> K< sub> 0.1 & lt; / sub> NbO< sub> 3 & lt; / sub>: Pr< sup> 3 + & lt; / sup> Er< sup> 3 + & lt; / sup>对荧光粉进行了研究。结果表明,两种材料均具有良好的光学测温性能。Pr< sup> 3 + & lt; / sup>掺杂优化了Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub> Er<sup>3+</sup>来源于Er<sup>3+</sup>离子热耦合能级的荧光粉。此外,Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub> Er<sup>3+</sup>和Li< sub> 0.9 & lt; / sub> K< sub> 0.1 & lt; / sub> NbO< sub> 3 & lt; / sub>: Er< sup> 3 + & lt; / sup> Pr< sup> 3 + & lt; / sup>采用Pr<sup>3+</sup>共掺杂归因于Pr<sup>3+</sup>Er< sup> 3 + & lt; / sup>,导致Er<sup>3+</sup>离子。这种新型双模光学测温材料为探索其他测温材料提供了物质基础和光学测温技术。
{"title":"Dual-mode up/down-conversion optical thermometry of Pr&lt;sup&gt;3+&lt;/sup&gt;-regulated Li&lt;sub&gt;0.9&lt;/sub&gt;K&lt;sub&gt;0.1&lt;/sub&gt;NbO&lt;sub&gt;3&lt;/sub&gt;:Er&lt;sup&gt;3+&lt;/sup&gt; phosphors","authors":"None Jia Chao-Yang, None Yang Xue, None Wang Zhi-Gang, None Chai Rui-Peng, None Pang Qing, None Zhang Xiang-Yu, None Gao Dang-Li","doi":"10.7498/aps.72.20231170","DOIUrl":"https://doi.org/10.7498/aps.72.20231170","url":null,"abstract":"Photothermal sensing is crucial for the development of smart wearable devices. However, designing and synthesizing luminescent materials with suitable multi-wavelength emission and constructing multiple sets of probes in a single material system is a huge challenge for constructing sensitive temperature sensors with a wide temperature range. In this paper, Pr<sup>3+</sup>, Er<sup>3+</sup> single-doped and double-doped Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub> phosphors were successfully prepared by high temperature solid phase method, and their structure, morphology, excitation wavelength and temperature-dependent fluorescence properties were characterized by XRD, SEM, fluorescence spectrometer and self-made heating device. Firstly, the photoluminescence of the synthesized series of samples was investigated. The results show that compared with the single-doped Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub>: Er<sup>3+</sup>sample, the up/down-conversion spectra of Pr<sup>3+</sup>, Er<sup>3+</sup> co-doped phosphors under 808/380 nm excitation show that the green fluorescence emission of Er<sup>3+</sup> is enhanced. In addition, under 980 nm excitation, Pr<sup>3+</sup> can effectively regulate the fluorescence energy level population pathway, so that the electrons are more effectively arranged in the <sup>2</sup>H<sub>11/2</sub> and <sup>4</sup>S<sub>3/2</sub> energy levels during the excitation process. The red emission is weakened and the green emission is enhanced, which improves the signal resolution of the fluorescent material and has a significant impact on the optical temperature measurement. Secondly, the up-conversion fluorescence property of Er<sup>3+</sup> under 808/980 nm laser excitation in Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub>:Er<sup>3+</sup>and Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub>:Pr<sup>3+</sup>,Er<sup>3+</sup>phosphors were investigated. The results show that the red and green fluorescence emissions of Er<sup>3+</sup> are two-photon processes. Finally, the up/down-conversion dual-mode temperature sensing properties of Er<sup>3+</sup> in Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub>:Er<sup>3+</sup> and Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub>:Pr<sup>3+</sup>,Er<sup>3+</sup> phosphors were investigated. It was found that both materials have good optical temperature measurement performance. Pr<sup>3+</sup> doping optimizes the dual-mode optical temperature measurement performance of Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub>:Er<sup>3+</sup> phosphors derived from the thermal coupling energy level of Er<sup>3+</sup>ions. In addition, the up/down-conversion fluorescence mechanism of Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub>:Er<sup>3+</sup> and Li<sub>0.9</sub>K<sub>0.1</sub>NbO<sub>3</sub>:Er<sup>3+</sup>,Pr<sup>3+</sup> phosphors is proposed, and the enhanced green fluorescence by Pr<sup>3+</sup> co-doping is attributed to the energy transfer from Pr<sup>3+</sup> to Er<sup>3+</sup> ions, leading ","PeriodicalId":10252,"journal":{"name":"Chinese Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135400893","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
All-optical reservoir computing system based on polarization dynamics 基于偏振动力学的全光储层计算系统
Pub Date : 2023-01-01 DOI: 10.7498/aps.72.20230727
None Yi You-Jian, None Ding Fu-Cai, None Zhu Ping, None Zhang Dong-Jun, None Liang Xiao, None Sun Mei-Zhi, None Guo Ai-Lin, None Yang Qing-Wei, None Kang Hai-Tao, None Yao Xiu-yu, None Li Zhao-Liang, None Xie Xing-Long, None Zhu Jian-Qiang
The laser probe is one of the main techniques for capturing ultrafast dynamic processes and has extensive applications in fields such as plasma physics, photochemistry, and biomedical science. In this work, a time-wavelength encoded optical probe generation scheme is proposed, which uses cascaded frequency doubling crystals with different phase-matching angles and independent delay lines to achieve time-wavelength encoding. This method offers single-shot high-spatiotemporal resolution, high frame rate, and a wide range of adjustable time windows. The temporal resolution of the optical probe depends on the pulse width of the second harmonic, which can be adjusted by changing the phase-matching angle of the frequency-doubling crystal. The time window of the optical probe is only related to the change in the delay line, which can be adjusted by changing the length of the delay line. Therefore, the time resolution and time window of the optical probe are independent of each other. An optical probe generation system is constructed with 247 fs temporal resolution, 4 μm spatial resolution, 4.05 THz maximal frame rate, and an adjustable time window from sub-picosecond to 3 ns. The three-dimensional spatiotemporal evolution process of plasma filaments is captured within a single shot by using the optical probe. The experimental results show that the ionization front of the plasma propagates forward at a velocity of begin{document}$ {left(2.963pm 0.024right)times 10}^{8};{rm{m}}/{rm{s}} $end{document}, which is consistent with the theoretical prediction. This demonstrates the feasibility of using the probe for capturing ultrafast events. In the part of discussion, we analyze that the key parameters of the optical probe can reach a maximum frame rate of 35.7 THz, a maximum time resolution of 28 fs, and a time window range that can be adjusted from hundreds of femtoseconds to tens of nanoseconds. Finally, the optimal design parameters of the optical probe are given for different application scenarios. The optical probe generation scheme has good scalability and versatility, and can be combined with any wavelength decoding device, diffraction imaging, holographic imaging, tomography scanning, and other technologies. The high spatiotemporal resolution of the optical probe and the independent adjustability of its parameters provide a feasible solution for single-shot high spatiotemporal resolution captures of ultrafast dynamic processes on a multiple time scale.
The laser probe is one of the main techniques for capturing ultrafast dynamic processes and has extensive applications in fields such as plasma physics, photochemistry, and biomedical science. In this work, a time-wavelength encoded optical probe generation scheme is proposed, which uses cascaded frequency doubling crystals with different phase-matching angles and independent delay lines to achieve time-wavelength encoding. This method offers single-shot high-spatiotemporal resolution, high frame rate, and a wide range of adjustable time windows. The temporal resolution of the optical probe depends on the pulse width of the second harmonic, which can be adjusted by changing the phase-matching angle of the frequency-doubling crystal. The time window of the optical probe is only related to the change in the delay line, which can be adjusted by changing the length of the delay line. Therefore, the time resolution and time window of the optical probe are independent of each other. An optical probe generation system is constructed with 247 fs temporal resolution, 4 μm spatial resolution, 4.05 THz maximal frame rate, and an adjustable time window from sub-picosecond to 3 ns. The three-dimensional spatiotemporal evolution process of plasma filaments is captured within a single shot by using the optical probe. The experimental results show that the ionization front of the plasma propagates forward at a velocity of <inline-formula><tex-math id="M2">begin{document}$ {left(2.963pm 0.024right)times 10}^{8};{rm{m}}/{rm{s}} $end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="22-20230727_M2.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="22-20230727_M2.png"/></alternatives></inline-formula>, which is consistent with the theoretical prediction. This demonstrates the feasibility of using the probe for capturing ultrafast events. In the part of discussion, we analyze that the key parameters of the optical probe can reach a maximum frame rate of 35.7 THz, a maximum time resolution of 28 fs, and a time window range that can be adjusted from hundreds of femtoseconds to tens of nanoseconds. Finally, the optimal design parameters of the optical probe are given for different application scenarios. The optical probe generation scheme has good scalability and versatility, and can be combined with any wavelength decoding device, diffraction imaging, holographic imaging, tomography scanning, and other technologies. The high spatiotemporal resolution of the optical probe and the independent adjustability of its parameters provide a feasible solution for single-shot high spatiotemporal resolution captures of ultrafast dynamic processes on a multiple time scale.
{"title":"All-optical reservoir computing system based on polarization dynamics","authors":"None Yi You-Jian, None Ding Fu-Cai, None Zhu Ping, None Zhang Dong-Jun, None Liang Xiao, None Sun Mei-Zhi, None Guo Ai-Lin, None Yang Qing-Wei, None Kang Hai-Tao, None Yao Xiu-yu, None Li Zhao-Liang, None Xie Xing-Long, None Zhu Jian-Qiang","doi":"10.7498/aps.72.20230727","DOIUrl":"https://doi.org/10.7498/aps.72.20230727","url":null,"abstract":"The laser probe is one of the main techniques for capturing ultrafast dynamic processes and has extensive applications in fields such as plasma physics, photochemistry, and biomedical science. In this work, a time-wavelength encoded optical probe generation scheme is proposed, which uses cascaded frequency doubling crystals with different phase-matching angles and independent delay lines to achieve time-wavelength encoding. This method offers single-shot high-spatiotemporal resolution, high frame rate, and a wide range of adjustable time windows. The temporal resolution of the optical probe depends on the pulse width of the second harmonic, which can be adjusted by changing the phase-matching angle of the frequency-doubling crystal. The time window of the optical probe is only related to the change in the delay line, which can be adjusted by changing the length of the delay line. Therefore, the time resolution and time window of the optical probe are independent of each other. An optical probe generation system is constructed with 247 fs temporal resolution, 4 μm spatial resolution, 4.05 THz maximal frame rate, and an adjustable time window from sub-picosecond to 3 ns. The three-dimensional spatiotemporal evolution process of plasma filaments is captured within a single shot by using the optical probe. The experimental results show that the ionization front of the plasma propagates forward at a velocity of <inline-formula><tex-math id=\"M2\">begin{document}$ {left(2.963pm 0.024right)times 10}^{8};{rm{m}}/{rm{s}} $end{document}</tex-math><alternatives><graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"22-20230727_M2.jpg\"/><graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"22-20230727_M2.png\"/></alternatives></inline-formula>, which is consistent with the theoretical prediction. This demonstrates the feasibility of using the probe for capturing ultrafast events. In the part of discussion, we analyze that the key parameters of the optical probe can reach a maximum frame rate of 35.7 THz, a maximum time resolution of 28 fs, and a time window range that can be adjusted from hundreds of femtoseconds to tens of nanoseconds. Finally, the optimal design parameters of the optical probe are given for different application scenarios. The optical probe generation scheme has good scalability and versatility, and can be combined with any wavelength decoding device, diffraction imaging, holographic imaging, tomography scanning, and other technologies. The high spatiotemporal resolution of the optical probe and the independent adjustability of its parameters provide a feasible solution for single-shot high spatiotemporal resolution captures of ultrafast dynamic processes on a multiple time scale.","PeriodicalId":10252,"journal":{"name":"Chinese Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135402171","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Dynamic migration of <100> interstitial dislocation loops under pure W and W containing helium impurity (010) surfaces studied by molecular dynamics simulation 动态偏移&lt;100&gt;通过分子动力学模拟研究了纯W和含氦杂质W(010)表面的间隙位错环
Pub Date : 2023-01-01 DOI: 10.7498/aps.72.20230651
None Qin Meng-fei, None Wang Ying-Min, None Zhang Hong-Yu, None Sun Ji-Zhong
In the fusion irradiation environment, dislocation loop defects occur under the plasma-facing tungsten surfaces, which affect its mechanical properties and hydrogen/helium retention. This paper presents a study that dynamic behaviors of a loop with a radius of 1 nm under the W surface are simulated by using molecular dynamics simulation at the atomic level. It finds that the dislocation loop direction, bulk temperature, depth, and helium atoms have great influence on the motion of the dislocation. This study shows that the dislocation loop ( is the Burgers vector, is the surface normal direction) tends to move towards the surface and the dislocation loop tends to stay in the material. In the course of its migration, the habit plane of dislocation loop may change and the internal stress reduces gradually. The probability of a dislocation loops escaping from the surface is over 90% when the temperature is higher than 800 K and their initial depth is less than 5 nm. The dislocation loop can escape from the surface when the temperature is 800 K and the initial depth is less than 2 nm. It is found that dislocation loops decompose into dislocations at elevated temperatures. Helium atoms impedes the migration of dislocation loop and increases its retention time. The existence of dislocation loops results in the uneven distribution of helium atoms under the W surface, and will potentially affect the surface morphology of tungsten.
在聚变辐照环境下,面向等离子体的钨表面会出现位错环缺陷,影响其力学性能和氢/氦潴留。本文研究了<img border=0 >W<img border=0 src="20230651_O_editing.files/image103.png">用分子动力学方法在原子水平上对表面进行了模拟。发现位错环的方向、体温、深度和氦原子对位错的运动有较大影响。本研究显示<img border=0 src="20230651_O_editing.files/image104.png">错位循环(<img border=0 src="20230651_O_editing.files/image105.png">为汉堡矢量,<img border=0 src="20230651_O_editing.files/image106.png">(为表面法线方向)趋向于向表面移动<img边界=0 >位错环倾向于留在材料中。在其迁移过程中,位错环的习惯面可能发生改变,内应力逐渐减小。<img border=0 src="20230651_O_editing.files/image104.png">当温度高于800 K且初始深度小于5 nm时,位错环从表面逸出的比例超过90%。img border=0 >当温度为800 K,初始深度小于2 nm时,位错环可以从表面逸出。发现<img border=0 src="20230651_O_editing.files/image108.png">错位循环分解为<img border=0 src="20230651_O_editing.files/image109.png">高温下的位错。氦原子阻碍了位错环的迁移,延长了位错环的保留时间。位错环的存在导致钨表面下氦原子分布不均匀,对钨的表面形貌有潜在影响。
{"title":"Dynamic migration of &lt;100&gt; interstitial dislocation loops under pure W and W containing helium impurity (010) surfaces studied by molecular dynamics simulation","authors":"None Qin Meng-fei, None Wang Ying-Min, None Zhang Hong-Yu, None Sun Ji-Zhong","doi":"10.7498/aps.72.20230651","DOIUrl":"https://doi.org/10.7498/aps.72.20230651","url":null,"abstract":"In the fusion irradiation environment, dislocation loop defects occur under the plasma-facing tungsten surfaces, which affect its mechanical properties and hydrogen/helium retention. This paper presents a study that dynamic behaviors of a <img border=0 > loop with a radius of 1 nm under the W<img border=0 src=\"20230651_O_editing.files/image103.png\"> surface are simulated by using molecular dynamics simulation at the atomic level. It finds that the dislocation loop direction, bulk temperature, depth, and helium atoms have great influence on the motion of the dislocation. This study shows that the <img border=0 src=\"20230651_O_editing.files/image104.png\"> dislocation loop (<img border=0 src=\"20230651_O_editing.files/image105.png\"> is the Burgers vector, <img border=0 src=\"20230651_O_editing.files/image106.png\"> is the surface normal direction) tends to move towards the surface and the <img border=0 > dislocation loop tends to stay in the material. In the course of its migration, the habit plane of dislocation loop may change and the internal stress reduces gradually. The probability of a <img border=0 src=\"20230651_O_editing.files/image104.png\"> dislocation loops escaping from the surface is over 90% when the temperature is higher than 800 K and their initial depth is less than 5 nm. The <img border=0 > dislocation loop can escape from the surface when the temperature is 800 K and the initial depth is less than 2 nm. It is found that <img border=0 src=\"20230651_O_editing.files/image108.png\"> dislocation loops decompose into <img border=0 src=\"20230651_O_editing.files/image109.png\"> dislocations at elevated temperatures. Helium atoms impedes the migration of dislocation loop and increases its retention time. The existence of dislocation loops results in the uneven distribution of helium atoms under the W surface, and will potentially affect the surface morphology of tungsten.","PeriodicalId":10252,"journal":{"name":"Chinese Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135550504","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
The asymmetric transmission realized by cascading an acousto-optic device and a whispering gallery mode microcavity 通过声光器件与低语通道模微腔级联实现非对称传输
Pub Date : 2023-01-01 DOI: 10.7498/aps.73.20230653
None Lv Yu-Xi, None Wang Chen, None Duan Tian-Qi, None Zhao Tong, None Chang Peng-Fa, None Wang An-Bang
In this paper, An asymmetric transmission scheme is proposed by cascading an acousto-optic device and a coupled whispering gallery mode (WGM) microsphere cavity, and it is demonstrated by theory and experiment. With the acousto-optic interaction in a fiber, the vector modes of the fundamental core mode could be converted to the different vector modes of a cladding (linear polarization -LP) mode, and because of the optical path difference between the cladding vector modes, the polarization of the cladding mode will be changed. The cladding mode could be converted back to the core fundamental mode by coupling with a WGM microcavity. By calculating the overlapping of the mode fields in the tapered fiber and the microcavity at the resonance wavelength, the coupling coefficients between different LP modes and WGM will be solved. And, the transmittivity and conversion coefficient of the two fiber modes, under the condition that when the polarization of the incident light does not coincide with the polarization orientation of the WGM, can be got. The transmission spectrum of the coupled WGM microcavity is calculated by using MATLAB program under eight states, including the states at different incident directions, different incident polarization of input and whether the acoustic wave is on or off. The results show that the conversion coefficient from the cladding modes to the core mode is completely different from that of the contrary process when the acoustic wave is working. And the forward and backward incident lights have completely different transmission characteristics, thus achieved the asymmetric transmission. The transmittances of forward incidence and reverse incidence at different polarizations are also studied, both of them change periodically over the polarization angle, and their phase difference is equal to the polarization change caused by acousto-optic interaction in the fiber. In the experiment, a two-stage tapered fiber is used to realize the working of acousto-optic interaction and the coupling of whispering gallery mode at the same time. By controlling the working states of the system, the same 8 states as in the calculation had been studied experimentally. In the results, due to the polarization-selection effect of the WGM, the light energy incident from the opposite directions will show different transmission characteristics. While the forward transmittance reaches the maximum value (about 0.505), the reverse transmittance reaches about the minimum value (0.010), and the transmission isolation reaches about 17 dB. The transmittance in two directions was measured at different incident polarization angles, the transmission isolation was analyzed, and the polarization change of cladding mode in the fiber was verified to be about 80°. The measured results coincide with the calculations of the developed theory well. At last, the shortcomings and optimization methods of the scheme are discussed. The asymmetric transmission scheme in this
本文提出了声光器件与耦合低语通道(WGM)微球腔级联的非对称传输方案,并进行了理论和实验验证。在光纤中,随着声光相互作用,基芯模式的矢量模式可以转换为包层(线性偏振-LP)模式的不同矢量模式,并且由于包层矢量模式之间的光程差异,将改变包层模式的偏振。通过与WGM微腔的耦合,可以将包层模式转换回核心基模。通过计算锥形光纤与微腔在共振波长处的模场重叠,求解不同LP模式与WGM之间的耦合系数。在入射光的偏振方向与WGM的偏振方向不重合的情况下,可以得到两种光纤模式的透光率和转换系数。利用MATLAB程序计算了耦合WGM微腔在不同入射方向下的状态、输入的不同入射偏振态以及声波开、关等8种状态下的透射谱。结果表明,声波工作时包层模式到核心模式的转换系数与相反过程的转换系数完全不同。而前后入射光具有完全不同的传输特性,从而实现了不对称传输。研究了不同偏振方向下正向入射和反向入射的透射率随偏振角的周期性变化,其相位差等于光纤中声光相互作用引起的偏振变化。在实验中,采用两级锥形光纤同时实现声光相互作用的工作和窃窃廊模式的耦合。通过控制系统的工作状态,实验研究了与计算相同的8种状态。结果表明,由于WGM的偏振选择效应,从相反方向入射的光能会表现出不同的透射特性。正向透过率达到最大值(约0.505),反向透过率达到最小值(约0.010),传输隔离达到约17db。在不同的入射偏振角下测量了两个方向的透射率,分析了传输隔离,验证了光纤包层模式的偏振变化约为80°。实测结果与理论计算结果吻合较好。最后讨论了该方案存在的不足和优化方法。本文提出的非对称传输方案继承了声光器件响应快、调谐好等优点,具有全光纤结构,在光开关和光隔离器等方面具有重要的应用潜力。
{"title":"The asymmetric transmission realized by cascading an acousto-optic device and a whispering gallery mode microcavity","authors":"None Lv Yu-Xi, None Wang Chen, None Duan Tian-Qi, None Zhao Tong, None Chang Peng-Fa, None Wang An-Bang","doi":"10.7498/aps.73.20230653","DOIUrl":"https://doi.org/10.7498/aps.73.20230653","url":null,"abstract":"In this paper, An asymmetric transmission scheme is proposed by cascading an acousto-optic device and a coupled whispering gallery mode (WGM) microsphere cavity, and it is demonstrated by theory and experiment. With the acousto-optic interaction in a fiber, the vector modes of the fundamental core mode could be converted to the different vector modes of a cladding (linear polarization -LP) mode, and because of the optical path difference between the cladding vector modes, the polarization of the cladding mode will be changed. The cladding mode could be converted back to the core fundamental mode by coupling with a WGM microcavity. By calculating the overlapping of the mode fields in the tapered fiber and the microcavity at the resonance wavelength, the coupling coefficients between different LP modes and WGM will be solved. And, the transmittivity and conversion coefficient of the two fiber modes, under the condition that when the polarization of the incident light does not coincide with the polarization orientation of the WGM, can be got. The transmission spectrum of the coupled WGM microcavity is calculated by using MATLAB program under eight states, including the states at different incident directions, different incident polarization of input and whether the acoustic wave is on or off. The results show that the conversion coefficient from the cladding modes to the core mode is completely different from that of the contrary process when the acoustic wave is working. And the forward and backward incident lights have completely different transmission characteristics, thus achieved the asymmetric transmission. The transmittances of forward incidence and reverse incidence at different polarizations are also studied, both of them change periodically over the polarization angle, and their phase difference is equal to the polarization change caused by acousto-optic interaction in the fiber. In the experiment, a two-stage tapered fiber is used to realize the working of acousto-optic interaction and the coupling of whispering gallery mode at the same time. By controlling the working states of the system, the same 8 states as in the calculation had been studied experimentally. In the results, due to the polarization-selection effect of the WGM, the light energy incident from the opposite directions will show different transmission characteristics. While the forward transmittance reaches the maximum value (about 0.505), the reverse transmittance reaches about the minimum value (0.010), and the transmission isolation reaches about 17 dB. The transmittance in two directions was measured at different incident polarization angles, the transmission isolation was analyzed, and the polarization change of cladding mode in the fiber was verified to be about 80°. The measured results coincide with the calculations of the developed theory well. At last, the shortcomings and optimization methods of the scheme are discussed. The asymmetric transmission scheme in this","PeriodicalId":10252,"journal":{"name":"Chinese Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2023-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"136202189","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
期刊
Chinese Physics
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