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| 1 | +@Article{Chen_PhysRevB_2009_v80_p165121, |
| 2 | + author = {Mohan Chen and Wei Fang and G.-Z. Sun and G.-C. Guo and Lixin He}, |
| 3 | + title = {{Method to construct transferable minimal basis sets forab |
| 4 | + initiocalculations}}, |
| 5 | + journal = {Phys. Rev. B}, |
| 6 | + year = 2009, |
| 7 | + volume = 80, |
| 8 | + number = 16, |
| 9 | + pages = 165121, |
| 10 | + doi = {10.1103/PhysRevB.80.165121}, |
| 11 | + abstract = {We propose a scheme to construct transferable minimal basis of |
| 12 | + localized orbitals for ab initio calculations. We first extract a set |
| 13 | + of highly localized Wannier-type orbitals from the reference systems. |
| 14 | + For each orbital, we decompose it to a pseudoatomic orbital, augmented |
| 15 | + by small local functions centered at its nearest-neighbor atoms. When |
| 16 | + applied for a real system, the center of each local function moves |
| 17 | + with its associated atoms, without changing its shape and amplitude. |
| 18 | + We have done intensive tests of this scheme for |
| 19 | + III{\textbackslash}char21{\{}{\}}V and group IV semiconductors and |
| 20 | + find the modified orbitals have very good transferability while still |
| 21 | + keep the basis size minimal. This work discusses why Wannier and |
| 22 | + Wannier-type functions are not transferable as one may expect.}, |
| 23 | +} |
| 24 | + |
| 25 | +@Article{Li_PhysRevB_2023_v107_p35433, |
| 26 | + author = {Pengfei Li and Rong Shi and Peize Lin and Xinguo Ren}, |
| 27 | + title = {{First-principles calculations of plasmon excitations in graphene, |
| 28 | + silicene, and germanene}}, |
| 29 | + journal = {Phys. Rev. B}, |
| 30 | + year = 2023, |
| 31 | + volume = 107, |
| 32 | + number = 3, |
| 33 | + pages = 35433, |
| 34 | + doi = {10.1103/PhysRevB.107.035433}, |
| 35 | + abstract = {Plasmon excitations in graphene, silicene and germanene are studied |
| 36 | + using linear-response time-dependent density functional theory within |
| 37 | + the random phase approximation (RPA). Here, we examine both the |
| 38 | + plasmon dispersion behavior and lifetime of extrinsic and intrinsic |
| 39 | + plasmons for these three materials. For extrinsic plasmons, we found |
| 40 | + that their properties are closely related to Landau damping. In the |
| 41 | + region without single-particle excitation (SPE), the plasmon |
| 42 | + dispersion shows a {\ensuremath{\sqrt{}}} q behavior and the lifetime |
| 43 | + is in{fi}nite at the RPA level, while in the single-particle |
| 44 | + excitation region, the plasmon dispersion shows a quasilinear behavior |
| 45 | + and the lifetime is {fi}nite. Moreover, for intrinsic plasmons, unlike |
| 46 | + graphene, the plasmon dispersion behavior of silicene and germanene |
| 47 | + exhibits a two-peak structure, which can be attributed to the complex |
| 48 | + and hybridized band structure of these two materials.}, |
| 49 | +} |
| 50 | + |
| 51 | +@Article{Sun_PhysRevB_2023_v108_p75158, |
| 52 | + author = {Liang Sun and Yuanbo Li and Mohan Chen}, |
| 53 | + title = {{Truncated nonlocal kinetic energy density functionals for simple |
| 54 | + metals and silicon}}, |
| 55 | + journal = {Phys. Rev. B}, |
| 56 | + year = 2023, |
| 57 | + volume = 108, |
| 58 | + number = 7, |
| 59 | + pages = 75158, |
| 60 | + doi = {10.1103/PhysRevB.108.075158}, |
| 61 | + abstract = {Adopting an accurate kinetic energy density functional (KEDF) to |
| 62 | + characterize the noninteracting kinetic energy within the framework of |
| 63 | + orbital-free density functional theory (OFDFT) is challenging. We |
| 64 | + propose a new form of the non-local KEDF with a real-space truncation |
| 65 | + cutoff that satisfies the uniform electron gas limit and design KEDFs |
| 66 | + for simple metals and silicon. The new KEDFs are obtained by |
| 67 | + minimizing a residual function, which contains the differences in the |
| 68 | + total energy and charge density of several representative systems with |
| 69 | + respect to the Kohn-Sham DFT results. By systematically testing |
| 70 | + different cutoffs of the new KEDFs, we find that the cutoff plays a |
| 71 | + crucial role in determining the properties of metallic Al and |
| 72 | + semiconductor Si systems. We conclude that the new KEDF with a |
| 73 | + sufficiently long cutoff performs even better than some representative |
| 74 | + non-local KEDFs in some aspects, which sheds new light on optimizing |
| 75 | + the KEDFs in OFDFT to achieve better accuracy.}, |
| 76 | +} |
| 77 | + |
| 78 | +@Article{Bakhsh_BeilsteinJNanotechnol_2024_v15_p310, |
| 79 | + author = {Sunila Bakhsh and Muhammad Khalid and Sameen Aslam and Muhammad Sohail |
| 80 | + and Muhammad Aamir Iqbal and Mujtaba Ikram and Kareem Morsy}, |
| 81 | + title = {{Investigating structural and electronic properties of neutral zinc |
| 82 | + clusters: a G0W0 and G0W0{\CYRG}0(1) benchmark}}, |
| 83 | + journal = {Beilstein J. Nanotechnol.}, |
| 84 | + year = 2024, |
| 85 | + volume = 15, |
| 86 | + pages = {310--316}, |
| 87 | + doi = {10.3762/bjnano.15.28}, |
| 88 | + abstract = {The structural and electronic properties of zinc clusters (Znn) for a |
| 89 | + size range of n = 2-15 are studied using density functional theory. |
| 90 | + The particle swarm optimization algorithm is employed to search the |
| 91 | + structure and to determine the ground-state structure of the neutral |
| 92 | + Zn clusters. The structural motifs are optimized using the density |
| 93 | + functional theory approach to ensure that the structures are fully |
| 94 | + relaxed. Results are compared with the literature to validate the |
| 95 | + accuracy of the prediction method. The binding energy per cluster is |
| 96 | + obtained and compared with the reported literature to study the |
| 97 | + stability of these structures. We further assess the electronic |
| 98 | + properties, including the ionization potential, using the all-electron |
| 99 | + FHI-aims code employing G0W0 calculations, and the G0W0{\CYRG}0(1) |
| 100 | + correction for a few smaller clusters, which provides a better |
| 101 | + estimation of the ionization potential compared to other methods.}, |
| 102 | +} |
| 103 | + |
| 104 | +@Article{Zhang_AdvMaterDeerfieldBeachFla_2024_pe2411137, |
| 105 | + author = {Xiaoqian Zhang and Qiangsheng Lu and Zhen-Xiong Shen and Wei Niu and |
| 106 | + Xiangrui Liu and Jiahua Lu and Wenting Lin and Lulu Han and Yakui Weng |
| 107 | + and Tianhao Shao and Pengfei Yan and Quan Ren and Huayao Li and Tay- |
| 108 | + Rong Chang and David J. Singh and Lixin He and Liang He and Chang Liu |
| 109 | + and Guang Bian and Lin Miao and Yongbing Xu}, |
| 110 | + title = {{Substantially Enhanced Spin Polarization in Epitaxial CrTe2 Quantum |
| 111 | + Films}}, |
| 112 | + journal = {Adv. Mater. (Deerfield Beach Fla,)}, |
| 113 | + year = 2024, |
| 114 | + pages = {e2411137}, |
| 115 | + doi = {10.1002/adma.202411137}, |
| 116 | + abstract = {2D van der Waals (vdW) magnets, which extend to the monolayer (ML) |
| 117 | + limit, are rapidly gaining prominence in logic applications for low- |
| 118 | + power electronics. To improve the performance of spintronic devices, |
| 119 | + such as vdW magnetic tunnel junctions, a large effective spin |
| 120 | + polarization of valence electrons is highly desired. Despite its |
| 121 | + considerable significance, direct probe of spin polarization in these |
| 122 | + 2D magnets has not been extensively explored. Here, using 2D vdW |
| 123 | + ferromagnet of CrTe2 as a prototype, the spin degrees of freedom in |
| 124 | + the thin films are directly probed using Mott polarimetry. The |
| 125 | + electronic band of 50 ML CrTe2 thin film, spanning the Brillouin zone, |
| 126 | + exhibits pronounced spin-splitting with polarization peaking at |
| 127 | + 7.9{\%} along the out-of-plane direction. Surprisingly, atomic-layer- |
| 128 | + dependent spin-resolved measurements show a significantly enhanced |
| 129 | + spin polarization in a 3 ML CrTe2 film, achieving 23.4{\%} |
| 130 | + polarization even in the absence of an external magnetic field. The |
| 131 | + demonstrated correlation between spin polarization and film thickness |
| 132 | + highlights the pivotal influence of perpendicular magnetic anisotropy, |
| 133 | + interlayer interactions, and itinerant behavior on these properties, |
| 134 | + as corroborated by theoretical analysis. This groundbreaking |
| 135 | + experimental verification of intrinsic effective spin polarization in |
| 136 | + CrTe2 ultrathin films marks a significant advance in establishing 2D |
| 137 | + ferromagnetic atomic layers as a promising platform for innovative |
| 138 | + vdW-based spintronic devices.}, |
| 139 | +} |
| 140 | + |
| 141 | +@Article{Zhang_npjComputMater_2024_v10_p293, |
| 142 | + author = {Duo Zhang and Xinzijian Liu and Xiangyu Zhang and Chengqian Zhang and |
| 143 | + Chun Cai and Hangrui Bi and Yiming Du and Xuejian Qin and Anyang Peng |
| 144 | + and Jiameng Huang and Bowen Li and Yifan Shan and Jinzhe Zeng and |
| 145 | + Yuzhi Zhang and Siyuan Liu and Yifan Li and Junhan Chang and Xinyan |
| 146 | + Wang and Shuo Zhou and Jianchuan Liu and Xiaoshan Luo and Zhenyu Wang |
| 147 | + and Wanrun Jiang and Jing Wu and Yudi Yang and Jiyuan Yang and Manyi |
| 148 | + Yang and Fu-Qiang Gong and Linshuang Zhang and Mengchao Shi and Fu-Zhi |
| 149 | + Dai and Darrin M. York and Shi Liu and Tong Zhu and Zhicheng Zhong and |
| 150 | + Jian Lv and Jun Cheng and Weile Jia and Mohan Chen and Guolin Ke and |
| 151 | + Weinan E and Linfeng Zhang and Han Wang}, |
| 152 | + title = {{DPA-2: a large atomic model as a multi-task learner}}, |
| 153 | + journal = {npj Comput. Mater}, |
| 154 | + year = 2024, |
| 155 | + volume = 10, |
| 156 | + number = 1, |
| 157 | + pages = 293, |
| 158 | + doi = {10.1038/s41524-024-01493-2}, |
| 159 | +} |
| 160 | + |
| 161 | +@Article{Sun_NanoLett_2024_v24_p16283, |
| 162 | + author = {Dongdong Sun and Xudong Zhu and Shaochuan Chen and Haotian Fang and |
| 163 | + Guixu Zhu and Gongpeng Lan and Lixin He and Yuanyuan Shi}, |
| 164 | + title = {{Uniformity, Linearity, and Symmetry Enhancement in TiOx/MoS2-xOx Based |
| 165 | + Analog RRAM via S-Vacancy Confined Nanofilament}}, |
| 166 | + journal = {Nano Lett.}, |
| 167 | + year = 2024, |
| 168 | + volume = 24, |
| 169 | + number = 51, |
| 170 | + pages = {16283--16292}, |
| 171 | + doi = {10.1021/acs.nanolett.4c04434}, |
| 172 | + abstract = {Due to the stochastic formation of conductive filaments (CFs), analog |
| 173 | + resistive random-access memory (RRAM) struggles to simultaneously |
| 174 | + achieve low variability, high linearity, and symmetry in conductance |
| 175 | + tuning, thus complicating on-chip training and limiting versatility of |
| 176 | + RRAM based computing-in-memory (CIM) chips. In this study, we present |
| 177 | + a simple and effective approach using monolayer (ML) MoS2 as |
| 178 | + interlayer to control the CFs formation in TiOx switching layer. The |
| 179 | + limited S-vacancies (Sv) in MoS2-xOx interlayer can further confine |
| 180 | + the position, size, and quantity of CFs, resulting in a highly uniform |
| 181 | + and symmetrical switching behavior. The set and reset voltages (Vset |
| 182 | + and Vreset) in TiOx/MoS2-xOx based RRAM are symmetric, with cycle-to- |
| 183 | + cycle variations of 1.28{\%} and 1.7{\%}, respectively. Moreover, high |
| 184 | + conductance tuning linearity and 64-level switching capabilities are |
| 185 | + achieved, which facilitate high accuracy (93.02{\%}) on-chip training. |
| 186 | + This method mitigates the device nonidealities of analog RRAM through |
| 187 | + Sv confined CFs, accelerating the development of RRAM based CIM chips.}, |
| 188 | +} |
| 189 | + |
1 | 190 | @Article{Zhang_PhysRevB_2024_v110_p224419, |
2 | 191 | author = {Tinghai Zhang and Yantao Cao and Bo Zhang and Hanjie Guo and Liang |
3 | 192 | Qiao and Fashen Li and Zhiwei Li}, |
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