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Phonon effects in high-energy photoemission spectra 高能光发射光谱中的声子效应
IF 1.8 4区 物理与天体物理 Q2 SPECTROSCOPY Pub Date : 2025-06-01 Epub Date: 2025-02-27 DOI: 10.1016/j.elspec.2025.147525
Takashi Fujikawa, Kaori Niki
In this paper some phonon effects on high-energy photoemission spectra for solids are discussed from a theoretical point of view. In case of photoemission from deep cores, recoil and Franck–Condon (FC) effects play some important roles: The former contributes to the peak shift following classical free atom recoil shift rule, however the latter has no influence on the shift within the harmonic phonon approximation. Both contribute to the temperature dependent peak broadening. In addition to these individual effects, the interference between recoil and FC should be considered, which contributes to the peak shift. In the harmonic approximation, the recoil shift is independent of the temperature. Beyond this approximation, we can expect that the recoil shift depends on the temperature in accordance with the observed results for some special systems. In addition to the core level photoemission, we discuss the high-energy photoemission from extended valence levels: Recoil effects and the turnover from ARPES to XPS limit are discussed.
本文从理论的角度讨论了固体高能光发射光谱中的声子效应。在深核光发射中,反冲和frank - condon (FC)效应起着重要的作用:前者有助于遵循经典自由原子反冲位移规则的峰移,而后者对谐波声子近似内的位移没有影响。两者都有助于温度依赖性峰展宽。除了这些单独的影响外,还应该考虑后坐力和FC之间的干扰,这有助于峰移。在谐波近似中,反冲位移与温度无关。在此近似值之外,根据对某些特殊系统的观测结果,我们可以预期反冲位移与温度有关。除了核心能级的光发射外,我们还讨论了扩展价能级的高能光发射,讨论了反冲效应和从ARPES到XPS极限的转换。
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引用次数: 0
Photoelectron diffraction of twisted bilayer graphene 扭曲双层石墨烯的光电子衍射
IF 1.8 4区 物理与天体物理 Q2 SPECTROSCOPY Pub Date : 2025-06-01 Epub Date: 2025-03-06 DOI: 10.1016/j.elspec.2025.147524
S. Tricot , H. Ikeda , H.C. Tchouekem , J.-C. Le Breton , S. Yasuda , P. Krüger , P. Le Fèvre , D. Sébilleau , T. Jaouen , P. Schieffer
Photoelectron diffraction (PED) is a powerful spectroscopic technique that combines elemental resolution with a high sensitivity to the local atomic arrangement at crystal surfaces, thus providing unique fingerprints of selected atomic sites in matter. Stimulated by the rapid innovation in the development of various analysis methods for probing the atomic and electronic structures of van der Waals (vdW) heterostructures of two-dimensional materials, we present a theoretical assessment of the capacity of PED for extracting structural properties such as stacking, twist angles and interlayer distances. We provide a complete description of PED for the benchmark vdW heterostructure bilayer graphene (BLG), by calculating and analyzing the PED of BLG in Bernal and AA-stacking as well as twisted BLG for a wide range of the twist angle.
光电子衍射(PED)是一种强大的光谱技术,它结合了元素分辨率和对晶体表面局部原子排列的高灵敏度,从而提供了物质中选定原子位置的独特指纹。在各种探测二维材料的范德华(vdW)异质结构的原子和电子结构的分析方法的快速创新发展的刺激下,我们提出了一个理论评估PED提取结构特性的能力,如堆叠,扭曲角和层间距离。通过计算和分析石墨烯在Bernal和aa堆叠以及大范围扭转角度下的PED,我们对基准vdW异质结构双层石墨烯(BLG)的PED进行了完整的描述。
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引用次数: 0
Fine structure of spectra for secondary electron excited by electron impact – Novel spectrum data analysis and application to nearly free electron metals 电子碰撞激发二次电子能谱的精细结构——新型能谱数据分析及其在近自由电子金属中的应用
IF 1.8 4区 物理与天体物理 Q2 SPECTROSCOPY Pub Date : 2025-06-01 Epub Date: 2025-04-12 DOI: 10.1016/j.elspec.2025.147539
Satoshi Hashimoto , Tsuguo Sakurada , Shigeo Tanuma , Keisuke Goto , Takaharu Nagatomi
In order to analyze the fine structure of the energy distribution of secondary electrons generated through the cascade process, we measured the electron spectra of NFE metals (Li, Mg, Al, Ca, Ga, In), their compounds (Al2O3 and GaAs) and Fe as transition metal with a CMA-type analyzer with absolute gain. We propose that the spectrum obtained by differentiating the energy spectrum in a logarithmic representation (defined as DLS) can be used to evaluate the excitation function that generates the fine structure of the secondary electron energy distribution. We found that the fine structure of the energy distribution of secondary electrons in NFE metals is mainly due to emission through a cascade process generated by the electrons from plasmon decay, which was obtained from analyses of the DLS, the excitation function, the energy distribution of secondary electrons N(E), and the EELS spectra. In addition, slow Auger electrons also generate secondary electrons through the cascade process. In Al2O3, a fine structure of secondary electrons was generated by electrons excited to unoccupied states by inter-band transitions and inner-shell excitation. In GaAs, both contributions from plasmon decay and electrons excited to unoccupied states by inter-band transitions and inner-shell excitation were observed. Based on these findings, it is concluded that the fine structure of the energy distribution of the secondary electrons emitted in the cascade process is due to the following electrons: 1) electrons from plasmon decay, 2) slow Auger electrons, and 3) electrons excited to unoccupied states by inter-band transitions or inner-shell excitation. These fine structures are superimposed on the structure of the individual excitation by primary electrons.
为了分析通过级联过程产生的次级电子能量分布的精细结构,我们使用具有绝对增益的cma型分析仪测量了NFE金属(Li, Mg, Al, Ca, Ga, In)及其化合物(Al2O3和GaAs)和Fe作为过渡金属的电子能谱。我们提出用对数表示(定义为DLS)微分能谱得到的谱可以用来评价产生次级电子能量分布精细结构的激发函数。通过对DLS、激发函数、二次电子能量分布N(E)和EELS谱的分析,我们发现NFE金属中二次电子能量分布的精细结构主要是由等离子体衰变产生的电子通过级联过程发射所致。此外,慢俄歇电子还通过级联过程产生二次电子。在Al2O3中,电子通过带间跃迁和内壳层激发激发到未占据态,产生了精细的二次电子结构。在砷化镓中,观察到等离子体衰变和电子被带间跃迁和内壳层激发激发到未占据态的贡献。基于这些发现,得出了级联过程中发射的次级电子能量分布的精细结构是由以下电子引起的:1)等离子体衰变产生的电子,2)慢俄歇电子,3)带间跃迁或内壳层激发激发到未占据态的电子。这些精细结构叠加在由初级电子激发的单个结构上。
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引用次数: 0
Electronic, magnetic and thermal behavior near the Invar compositions of Fe-Ni alloys 铁-镍合金因瓦尔成分附近的电子、磁性和热行为
IF 1.8 4区 物理与天体物理 Q2 SPECTROSCOPY Pub Date : 2025-06-01 Epub Date: 2025-04-19 DOI: 10.1016/j.elspec.2025.147540
Ananya Sahoo , Ayusa Aparupa Biswal , S.K. Parida , V.R.R. Medicherla , Soumya Shephalika Behera , M.N. Singh , A. Sagdeo , Sawani Datta , Abhishek Singh , Kalobaran Maiti
The structural, magnetic and electronic properties of Fe1xNix (x = 0.32, 0.36, 0.40, 0.50) alloys have been investigated using synchrotron based x-ray diffraction (XRD), superconducting quantum interference device (SQUID) magnetometer and the high resolution x-ray photoelectron spectroscopy (XPS) measurements. The XRD measurement was done down to 50 K temperature. The XRD studies suggest a single phase with fcc structure for x = 0.36, 0.40, and 0.50 alloys and a mixed phase for x = 0.32 alloy containing both bcc and fcc structures. The lattice parameter of the alloys exhibits a linear dependence on temperature giving rise to a temperature independent coefficient of thermal expansion (CTE). The lowest CTE is observed for x = 0.36 Invar alloy as expected while x = 0.50 alloy exhibits the highest CTE among the alloys studied. The CTE of the fcc component of mixed phase alloy is close to that of Invar alloy. The temperature dependence of magnetization of the alloys down to 2 K reveals an overall antiferromagnetic interactions within the ferromagnetic phase causing the magnetization decreasing with lowering temperature. The field cooled and zero field cooled data show larger differences for the Invar compositions; this is also manifested in the magnetic hysteresis data at 2 K and 300 K. The Fe 2p and Ni 2p core level spectra exhibit spin–orbit split features along with a satellite feature in the Ni 2p spectra. The spectral line shapes are almost similar for all the compositions studied. Interestingly, the spin–orbit splitting for Fe 3p spectra is larger than that observed for Ni 3p suggesting additional contributions due to the exchange interaction between the Fe 3p core hole with the Fe 3d moment. This suggests large magnetic moment contribution from Fe as expected. The core level and valence band spectra, and the magnetization data suggest significant role of disorder for the Invar compositions.
利用同步加速器x射线衍射(XRD)、超导量子干涉仪(SQUID)磁强计和高分辨率x射线光电子能谱(XPS)测量研究了Fe1-xNix(x=0.32,0.36,0.40,0.50)合金的结构、磁性和电子性能。XRD测量在低至50 K的温度下进行。XRD研究表明,对于x=0.36、0.40和0.50的合金,存在具有fcc结构的单相,而对于x=0.32的合金,则存在含有bcc和fcc结构两者的混合相。合金的晶格参数与温度呈线性关系,从而产生与温度无关的热膨胀系数(CTE)。正如预期的那样,x=0.36因瓦合金的CTE最低,而x=0.50合金在所研究的合金中表现出最高的CTE。混合相合金fcc组分的CTE接近殷钢合金。低至2 K的合金磁化强度的温度依赖性揭示了铁磁相中的整体反铁磁相互作用,导致磁化强度随温度降低而降低。场冷和零场冷数据显示殷钢成分差异较大;这也表现在2 K和300 K下的磁滞数据中。Fe 2p和Ni 2p核能级谱在Ni 2p谱中表现出自旋轨道分裂特征和卫星特征。所研究的所有成分的谱线形状几乎相似。有趣的是,Fe 3p光谱的自旋轨道分裂比Ni 3p光谱观察到的更大,这表明由于Fe 3p核心空穴与Fe 3d矩之间的交换相互作用,有额外的贡献。这表明铁的磁矩贡献很大,正如预期的那样。核心能级和价带谱以及磁化数据表明,无序对殷钢成分起着重要作用。
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引用次数: 0
The effect of edge configurations diversity on the energy gap in MXene zigzag nanoribbons based on Ti3C2O2 and Sc3C2F2 边缘构型多样性对基于Ti3C2O2和Sc3C2F2的MXene之字形纳米带能隙的影响
IF 1.8 4区 物理与天体物理 Q2 SPECTROSCOPY Pub Date : 2025-03-01 Epub Date: 2025-02-26 DOI: 10.1016/j.elspec.2025.147526
M.S. Akhoundi Khezrabad , O. Soltani , A. Shokri
In this study, we report the band structure and energy gap of different edges of Ti3C2O2 and Sc3C2F2 zigzag nanoribbons using tight-binding approximation. Our results show that in most widths of zigzag nanoribbons, the energy gap in different edge configurations has different values even though they have the same width. In Ti3C2O2 nanoribbons, the presence of central atoms at the edge of the zigzag nanoribbon increases the band-gap and in Sc3C2F2 nanoribbon, depending on the width of the nanoribbon, the presence of central atoms or surface atoms on the edge of the nanoribbon can increase the band-gap. The maximum difference reaches 0.3 eV in Sc3C2F2 nanoribbon and 0.17 eV in Ti3C2O2 nanoribbon. The band gap depending on the edge atoms can be important for the design and use of MXene nanoribbons in electronic and optoelectronic devices.
在这项研究中,我们报道了Ti3C2O2和Sc3C2F2之字形纳米带不同边缘的能带结构和能隙。结果表明,在大多数宽度的锯齿形纳米带中,即使宽度相同,不同边缘构型的能隙值也不同。在Ti3C2O2纳米带中,锯齿形纳米带边缘中心原子的存在增加了带隙;在Sc3C2F2纳米带中,根据纳米带宽度的不同,纳米带边缘中心原子或表面原子的存在都会增加带隙。Sc3C2F2纳米带的最大差异为0.3 eV, Ti3C2O2纳米带的最大差异为0.17 eV。依赖于边缘原子的带隙对于MXene纳米带在电子和光电子器件中的设计和使用是重要的。
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引用次数: 0
Time evolution of ion states formed during the cascade decay of vacancies produced by the electron capture decay of the 125I radionuclide 125I放射性核素电子俘获衰变产生的空位级联衰变过程中离子态的时间演化
IF 1.8 4区 物理与天体物理 Q2 SPECTROSCOPY Pub Date : 2025-03-01 Epub Date: 2025-01-25 DOI: 10.1016/j.elspec.2025.147522
A.P. Chaynikov , A.G. Kochur , A.I. Dudenko
Cascade relaxation of inner-shell vacancies in tellurium atom produced by the electron capture decay of the 125I radionuclide is studied using Monte Carlo simulations. Final cascade ions yields and mean final ion charges upon the decay of single-inner-vacancy states TeX–15p5 (X = 1 s to 5 s) were calculated. The time evolution of the cascade ion states is simulated, and the mean final ion charge is found to be stabilized within τcasc = 10–12 s after the electron capture decay of the 125I nucleus. This time interval must be compared to the time τneutr needed for ions neutralization when 125I is used as an Auger emitter in radiotherapy. Depending on the relation between τcasc and τneutr, either ‘isolated-atom’ or ‘condensed-phase’ approximation should be used in theoretical descriptions of local energy deposition.
利用蒙特卡罗模拟研究了125I放射性核素的电子俘获衰变对碲原子内壳空位的级联弛豫。计算了单内空位态tec - 15p5 (X = 1 s ~ 5 s)衰变时的最终级联离子产额和平均最终离子电荷。模拟了级联离子态的时间演化,发现在125I原子核的电子俘获衰变后,离子的平均最终电荷稳定在τcasc = 10-12 s内。这个时间间隔必须与使用125I作为放射治疗中的俄歇辐射源时离子中和所需的时间τ中性相比较。根据τcasc和τ中性之间的关系,局部能量沉积的理论描述可以采用“孤立原子”近似或“凝聚相”近似。
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引用次数: 0
Photoionization and electronic structure of chemical warfare agents 化学战剂的光电离和电子结构
IF 1.8 4区 物理与天体物理 Q2 SPECTROSCOPY Pub Date : 2025-03-01 Epub Date: 2025-02-14 DOI: 10.1016/j.elspec.2025.147523
Igor Novak
The vertical, valence ionization energies for several chemical warfare agents (CWA): nerve agents, choking agents and blister agents have been calculated (as free molecules) using high-level ab initio coupled-cluster method: IP-EOM-CCSD. The calculated vertical, valence ionization energies were used to simulate UV photoelectron spectra. We also calculated 1st adiabatic ionization energies for these CWA. Our results, especially 1st ionization energies (vertical and adiabatic) may be useful when applying photoionization techniques as part of hyphenated methods for detection and identification of CWA. The variations of vertical ionization energies were rationalized by the analysis of the electronic structure of CWA. The influence of electronic structures on toxicological properties is also discussed on the basis of calculated Hirshfeld type charges.
几种化学战剂(CWA):神经毒剂,窒息剂和水泡剂的垂直价电离能已经计算(作为自由分子)使用高级从头算耦合簇方法:IP-EOM-CCSD。用计算得到的垂直价电子电离能来模拟紫外光电子能谱。我们还计算了这些CWA的第一绝热电离能。我们的研究结果,特别是第一电离能(垂直和绝热),在应用光电离技术作为连接方法的一部分来检测和鉴定CWA时可能是有用的。通过对水煤浆电子结构的分析,对垂直电离能的变化规律进行了解释。在计算赫希菲尔德型电荷的基础上,讨论了电子结构对毒理学性质的影响。
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引用次数: 0
Anisotropic dispersion of excitonic bands of the single-crystal pentacene (001) surface as measured by low-energy angle-resolved high-resolution electron energy-loss spectroscopy 单晶并五苯(001)表面激子带各向异性色散的低能角分辨高分辨率电子能量损失谱测量
IF 1.8 4区 物理与天体物理 Q2 SPECTROSCOPY Pub Date : 2025-03-01 Epub Date: 2025-01-31 DOI: 10.1016/j.elspec.2025.147514
Yasuo Nakayama , François C. Bocquet , Ryohei Tsuruta , Serguei Soubatch , F. Stefan Tautz
Low-energy high-resolution electron energy-loss spectroscopy (HREELS) is a useful technique for the characterization of various excitation processes at solid surfaces. However, no successful work has been reported on molecular single-crystal samples yet. In the present study, low-energy angle-resolved HREELS measurements were conducted on single-crystal pentacene, an organic semiconductor. The results confirmed the excitonic bands exhibiting energy–momentum dispersion and anisotropy of these depending on the surface crystallographic directions, corroborating the occurrence of exciton delocalization, contrary to the ordinary notion of the Frenkel exciton for weakly interacting van der Waals molecular solids. The present results demonstrate that low-energy angle-resolved HREELS is applicable to the precise examination of the excitonic characteristics of solid-state surfaces, even for molecular semiconductor single crystals.
低能高分辨率电子能量损失谱(HREELS)是表征固体表面各种激发过程的有用技术。然而,在分子单晶样品上还没有成功的工作报道。在本研究中,对单晶并五苯(一种有机半导体)进行了低能角分辨HREELS测量。结果证实了激子带表现出能量-动量色散和各向异性,这些色散和各向异性取决于表面晶体学方向,证实了激子离域的存在,这与弱相互作用范德华分子固体中Frenkel激子的通常概念相反。目前的结果表明,低能角分辨HREELS适用于固体表面激子特性的精确检测,甚至适用于分子半导体单晶。
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引用次数: 0
Density functional theory calculations of the electronic structure and dielectric properties of metal oxide systems Al2O3, MgO, Cu2O, TiO2, WO3 金属氧化物体系Al2O3, MgO, Cu2O, TiO2, WO3的电子结构和介电性能的密度泛函理论计算
IF 1.8 4区 物理与天体物理 Q2 SPECTROSCOPY Pub Date : 2025-01-01 Epub Date: 2024-12-21 DOI: 10.1016/j.elspec.2024.147512
Raul E. Gutierrez , Ivana Matanovic , Maciej P. Polak , Dane Morgan , Edl Schamiloglu
Density Functional Theory is utilized to study the electronic structure and dielectric properties of various metal oxide systems (Al2O3, MgO, Cu2O, TiO2, WO3) in comparison to their base metals (Al, Mg, Cu, Ti, and W). The properties studied include the density of states, energy band gap, Fermi energy, work function, ionization potential, and the frequency- and momentum-dependent energy loss function. This work provides high-quality first principles-calculated properties that can be further utilized in computational simulations which aim to model complicated electron inelastic scattering interactions in metal oxides and their corresponding metals. In general, properties of this nature might be of interest, but not limited, to those involved in the multipactor effect, magnetic confinement fusion, photovoltaics, charged particle accelerators, x-ray photoelectron spectroscopy, Auger electron spectroscopy, and photomultipliers.
密度泛函理论用于研究各种金属氧化物体系(Al2O3, MgO, Cu2O, TiO2, WO3)与其母金属(Al, Mg, Cu, Ti, W)的电子结构和介电性质,研究的性质包括态密度,能带隙,费米能,功函数,电离势以及频率和动量相关的能量损失函数。这项工作提供了高质量的第一性原理计算性质,可以进一步用于旨在模拟金属氧化物及其相应金属中复杂的电子非弹性散射相互作用的计算模拟。一般来说,这种性质可能会引起人们的兴趣,但不限于那些涉及多因子效应、磁约束聚变、光伏、带电粒子加速器、x射线光电子能谱、俄歇电子能谱和光电倍增管的性质。
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引用次数: 0
Embedding of cluster models of oxides: Implications for XPS predictions 氧化物簇模型的嵌入:对XPS预测的影响
IF 1.8 4区 物理与天体物理 Q2 SPECTROSCOPY Pub Date : 2025-01-01 Epub Date: 2024-12-15 DOI: 10.1016/j.elspec.2024.147511
Paul S. Bagus , Connie J. Nelin
The importance of embedding cluster models of NiO that are used to predict and analyze the Ni 2p XPS spectra in this compound is studied. The XPS obtained with an isolated NiO6 cluster are compared with those obtained with the cluster embedded in a point charge field designed to reproduce the Madelung potential of the crystal. It is found that there is a remarkable and possibly unexpected similarity between the theoretical XPS spectra with and without point charge embedding. It is believed that this can be expected to be a general conclusion relevant for the XPS of other ionic compounds.
研究了在该化合物中嵌入NiO簇模型用于预测和分析ni2p XPS光谱的重要性。将分离NiO6团簇得到的XPS与嵌入点电荷场得到的XPS进行了比较,以重现晶体的马德隆电位。发现在有和没有嵌入点电荷的情况下,理论XPS光谱有显著的、可能是意想不到的相似性。相信这一结论对其他离子化合物的XPS分析具有普遍意义。
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引用次数: 0
期刊
Journal of Electron Spectroscopy and Related Phenomena
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