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NISHIGUCHI KazutakaGraduate School of System Informatics / Department of System InformaticsAssociate Professor
Research activity information
■ Paper- Lead, American Chemical Society (ACS), Mar. 2025, The Journal of Physical Chemistry Letters, 2823 - 2830[Refereed]Scientific journal
- Physical Society of Japan, Feb. 2025, Journal of the Physical Society of Japan, 94(2) (2)[Refereed]Scientific journal
- Layered perovskite Y2Ti2O5S2 is a promising semiconductor photocatalyst with an electronic structure suitable for overall water splitting under visible light. However, similar to other photocatalysts, structural defects during synthesis should be controlled. Transmission electron microscopy (TEM) revealed extremely large planar defects composed of S-Mg-S layers in Y2Ti2O5S2 synthesized using the flux method. We determined the planar defect structure and electronic structure using first-principles calculations based on the density functional theory. The evaluation of the formation energy suggests that S-and Mg-poor conditions may prevent defect formation. Furthermore, we discuss the impurity levels caused by the planar defects and their effects on the electronic state and catalytic performance.Lead, AMER CHEMICAL SOC, Apr. 2023, JOURNAL OF PHYSICAL CHEMISTRY C, 127(16) (16), 7887 - 7893, English[Refereed]Scientific journal
- Lead, Physical Society of Japan, Jun. 2022, Journal of the Physical Society of Japan, 91(6) (6)[Refereed]Scientific journal
- American Chemical Society (ACS), Oct. 2021, The Journal of Physical Chemistry C, 125(40) (40), 21840 - 21850[Refereed]Scientific journal
- Physical Society of Japan, Sep. 2021, Journal of the Physical Society of Japan, 90(9) (9), 094707 - 094707, English[Refereed]Scientific journal
- Apr. 2021, J. Phys. Soc. Jpn. 90, 054705 (2021)[Refereed]
- We study possible superconductivity in a carrier-doped iridium oxideLead, Physical Society of Japan, Apr. 2019, J. Phys. Soc. Jpn. 88 (2019), 094701, 88(9) (9), 094701 - 094701, English
insulator Sr$_{2}$IrO$_{4}$ based on an effective $t_{2g}$ three-orbital
Hubbard model on the square lattice with a large spin-orbit coupling (SOC).
Numerically solving the linearized Eliashberg equation for the superconducting
(SC) gap function with the random phase approximation, we systematically
examine both singlet and triplet SC gap functions with possible pairing
symmetries and the parameter dependence of the superconductivity. For the
realistic SOC $\lambda$ and Hund's coupling $J/U$ relevant to
Sr$_{2}$IrO$_{4}$, namely, for a large $\lambda$ and small $J/U$ region, we
find that the intra-band antiferromagnetic (AF) pseudospin $\bm{j}_{\text{eff } }
= -\bm{l}+\bm{s}$ fluctuations favor a $d_{x^{2}-y^{2 } }$-wave pseudospin
$j_{\text{eff } }=1/2$ singlet pairing in the electron-doping. We also find that
the $d_{x^{2}-y^{2 } }$-wave pairing is more stabilized with increasing the SOC
and decreasing the Hund's coupling. Furthermore, we show for a small $\lambda$
and large $J/U$ region that an $s_{\pm}$-wave singlet pairing is favored in the
hole-doped region. The origin of the $s_{\pm}$-wave pairing is due to the
inter-band pair scattering arising from the intra-orbital AF spin $\bm s$
fluctuations. Although the possibility of a pseudospin triplet pairing is
considered, we find it always unfavorable for all parameters studied here. The
experimental consequences for other strongly correlated materials with a large
SOC are also discussed.[Refereed]Scientific journal - This study theoretically investigated the magnetic properties and electronicNov. 2018, Carbon 143 (2019) 828-836
structure of a graphene-based nano-spin-valve-like structure. Magnetic nickel
layers on both sides of the graphene were considered. A spin-polarized
generalized-gradient approximation determined the electronic states. In an
energetically stable stacking arrangement of graphene and two nickel layers,
the anti-parallel spin configuration of the underlayer and overlayer magnetic
moments had the lowest energy, which is in agreement with previous experimental
studies. The spin density mapping and obtained band-structure results show that
when the upper and lower Ni(111) slabs have an anti-parallel (parallel)
magnetic-moment configuration, the carbon atoms of sublattices A and B will
have an antiferromagnetic (ferromagnetic) spin configuration. A band gap at the
Dirac cone was open when the alignment had an anti-parallel configuration and
closed when the alignment had a parallel configuration. Therefore, the in-plane
conductance of the graphene layer depends on the magnetic alignment of the two
nickel slabs when the Fermi level is adjusted at the Dirac point. Both the
magnetic properties and electronic structures of the Ni/graphene/Ni
nanostructure cause the system to be a new prospective spintronic device
showing controllable in-plane magnetoresistance.[Refereed]Scientific journal - We present a theoretical study of non-bonding edge modes at the mono-hydrogenated armchair edge (A1 edge) of a graphene ribbon by modifying its bulk electronic structure. Structural deformation of graphene bulk is known to lead Dirac cones to change their location in the Brillouin zone. We adopt the Ryu–Hatsugai criterion on the edge states to identify a non-trivial topological phase in a parametrized Hamiltonian space for graphene ribbons. For the armchair ribbon, the Dirac-cone shift happens along the 1st Brillouin zone and a non-trivial winding number appears except for a special case where the shifted Dirac points are mapped always to the Γ point irrespective of the deformation. We also discuss the electronic band structure of the ribbon by performing DFT-LDA calculation to show the indication of edge state occurrence. By utilizing the tight-binding model to examine a large-size limit of the deformed ribbon structure, an explicit function form of the edge state at A1 is derived. Our results from the Ryu–Hatsugai criterion and the band structure calculations show a physical proof of the existence of the edge states at the armchair graphene ribbon edge when the bulk graphene structure is properly deformed. Observation of this phenomenon is expected to be induced by coherent phonons in a µm graphene sample having a long armchair edge.Jul. 2018, J. Phys. Soc. Jpn. 87, 084706 (2018)[Refereed]
- In order to theoretically identify the factors governing superconductivity inLead, Jun. 2018, Phys. Rev. B 98, 174508 (2018)
multi-layer cuprates, a three-layer Hubbard model is studied with the
two-particle self-consistent (TPSC) approach so as to incorporate electron
correlations. The linearized Eliashberg equation is then solved for the gap
function in a matrix form to resolve the role of outer CuO$_2$ planes (OPs) and
inner plane (IP). We show that OPs dominate IP in the $d_{x^{2}-y^{2 } }$-wave
superconductivity, while IP dominates in the antiferromagnetism. This comes
from an electron correlation effect in that the correlation makes the doping
rates different between OPs and IP (i.e., a self-doping effect), which occurs
in intermediate and strong correlation regimes. Namely, the antiferromagnetic
fluctuations in IP are stronger due to a stronger electron correlation, which
simultaneously reduces the quasiparticle density of states in IP with a
suppressed $d_{x^{2}-y^{2 } }$-wave superconductivity. Intriguingly, while the
off-diagonal (inter-layer) elements in the gap function matrix are tiny, {\it
inter-layer pair scattering} processes are in fact at work in enhancing the
superconducting transition temperature $T_{\text{c } }$ through the inter-layer
Green's functions. This actually causes the trilayer system to have higher
$T_{\text{c } }$ than the single-layer in a weak- and intermediate-coupling
regimes. This picture holds for a range of the on-site Hubbard repulsion $U$
that contains those estimated for the cuprates. The present result is
qualitatively consistent with nuclear magnetic resonance experiments in
multi-layer cuprates superconductors.[Refereed]Scientific journal - To explore material dependence of cuprate superconductors, we evaluateMay 2018, J. Phys. Soc. Jpn. 87, 114701 (2018)
effective Coulomb interactions for Hg1201 and Tl1201, where Tl1201 having a
nearly half value of T_c of Hg1201 even at the optimal oxygen concentration.
Although structures are similar for these superconductors, there is an apparent
difference in the occupied levels below EF. The characteristic difference in
the band structure is correlated with oxygen contents in the buffer layer. By
using constrained Random Phase Approximation, effective screened Coulomb
interactions are estimated for HgBa_2CuO_4 and TlBa_2CuO_5. The results shows
that the value of screened on-site Coulomb interaction in Hg1201 is nearly
twice bigger than that in Tl1201. In addition, The eigenvalues of the
linearized Eliashberg equation of single-band Hubbard model within FLEX can
show apparent difference in T_c. When we assume that the twice big screened
on-site Coulomb for Hg, the material dependent T_c might be explained.[Refereed]Scientific journal - Lead, 東京 : アドバンスソフト出版事業部, Jan. 2018, アドバンスシミュレーション = Advance simulation / アドバンスソフト株式会社編集委員会 編, 25, 43 - 54, Japanese強相関電子系へのAdvance/PHASEの適用—Application of Advance/PHASE to Strongly Correlated Electron Systems—特集 アドバンスソフトにおける研究開発 ; アドバンスソフトにおける外部機関との連携[Refereed][Invited]
- A self-doping effect between outer and inner CuO2 planes (OPs and IPs) in multilayer cuprate superconductors is studied. When one considers a three-layer tight-binding model of the Hg-based three-layer cuprate derived from first-principles calculations, the electron concentration becomes larger in the OPs than in the IP. This is inconsistent with the experimental finding that more hole carriers tend to be introduced into the OPs than into the IP. We investigate a three-layer Hubbard model with the two-particle self-consistent approach for multilayer systems to incorporate electron correlations. We observe that the double occupancy (antiferromagnetic instability) in the IP decreases (increases) more than that in the OPs, and also reveal that more electrons tend to be introduced into the IP than into the OPs to obtain an energy gain from the on-site Hubbard interaction. These results are consistent with the experimental findings, and this electron distribution between the OPs and IP can be interpreted as a self-doping effect arising from strong electron correlations.Lead, PHYSICAL SOC JAPAN, Aug. 2017, JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN, 86(8) (8), English[Refereed]Scientific journal
- To better understand electronic and magnetic properties of superconducting (SC) states in 5d transition metal oxides, we derive an analytical formula of the dynamical correlation function for multi-orbital systems with the spin-orbit coupling (SOC), which is accessible to the experimental responses. Starting with a multi-orbital BCS Hamiltonian including the SC gap function, we introduce the dynamical correlation function in the non-interacting case. Based on the diagrammatic techniques, we derive the dynamical correlation function for the interacting case within the random phase approximation. With the help of a numerical calculation, we also show the temperature dependence of the magnetic susceptibility for two different SC states in the presence of the SOC.Lead, Institute of Physics Publishing, Apr. 2017, Journal of Physics: Conference Series, 807(5) (5), English[Refereed]International conference proceedings
- An enhancement mechanism of two-particle exchange interactions in single- and multi-layer cuprate superconductorsTo explore material dependence of layered cuprate superconductors, we examineApr. 2017
effective two-particle interactions for Hg1201 and Tl1201, where Tl1201 having
a nearly half value of Tc of Hg1201 even at the optimal oxygen concentration.
Although the 3dx_2-y_2 band, the Fermi surface, and its Wannier-orbitals are
similar for these superconductors, there is an apparent difference in the
unoccupied levels above EF. Based on a multi-reference
density-functional-theory formulation, effective two-particle exchange
interactions are estimated to derive enhancement in intra-layer exchange
interactions for HgBa2CuO4, while it is weakened in TlBaLaCuO5 and furthermore
it is weak in TlBa2CuO5. The characteristic difference in the band structure is
correlated with oxygen contents in the buffer layer. We also comment on the
similar feature in triple-layered compounds. Our spin-fluctuation enhancement
mechanism in an electron-correlation regime is consistent with the experimental
fact.Scientific journal - Lead, 2017, アドバンスシミュレーション, Vol. 25. (2017)[Refereed][Invited]
- To reveal a possible electronic instability toward various symmetry broken ordered states of Sr2IrO4, we investigate generalized susceptibilities of a three-orbital Hubbard model with spin–orbit coupling in the random phase approximation (RPA). By calculating the magnetic susceptibilities, we find that the in-plane antiferromagnetic instability of an effective total angular momentum Jeff = 1/2 is the strongest for a realistic set of parameters for Sr2IrO4. This is in good agreement with the strong coupling theoretical study and the experimental observation. We also discuss the possibility of superconductivity in doped Sr2IrO4.Lead, Sep. 2013, JPS Conf. Proc. 3, 015037 (2014)[Refereed]
- In order to explore why the multilayered cuprates have such high T c values, we have examined various interlayer processes. Since the interlayer one-electron hopping has little effect on the band structure, we turn to the interlayer pair hopping. The superconductivity in a double-layer Hubbard model with and without the interlayer pair hopping, as studied by solving the Eliashberg equation with the fluctuation exchange approximation, reveals that the interlayer pair hopping acts to increase the pairing interaction and the self-energy simultaneously, but that the former effect supersedes the latter and enhances the superconductivity, along with how the sign of the interlayer off-site pair hopping determines the relative configuration of d waves between the adjacent layers. Study of the triple-layer case with the interlayer pair hopping further reveals that the superconductivity is further enhanced but tends to be saturated toward the triple-layer case. © 2013 American Physical Society.Jul. 2013, Physical Review B - Condensed Matter and Materials Physics, 88(1) (1), English[Refereed]Scientific journal
- Lead, Mar. 2013, The University of TokyoTheory of high Tc superconductivity in multi-layered cuprates[Refereed]Doctoral thesis
- 近畿化学協会コンピュータ化学部会(第120回例会)公開講演会, Oct. 2024人工光合成による水素生成:ペロブスカイト半導体光触媒の第一原理解析[Invited]Public discourse
- The 18th Annual Meeting of Japan Society for Molecular Science, Sep. 2024First-principles analysis of photocatalytic activities in perovskite oxynitride ATaO2N (A = Ba, Sr, Ca)Poster presentation
- The 18th Annual Meeting of Japan Society for Molecular Science, Sep. 2024Machine learning-based prediction of crystal phases in perovskite compoundsPoster presentation
- The 3rd Research Workshop of ”Program for Promoting Research on the Supercomputer Fugaku", Mar. 2024Material design of high-performance perovskite semiconductor photocatalysts for hydrogen evolution through artificial photosynthesisPoster presentation
- 2024 APS March Meeting, Mar. 2024, EnglishFerromagnetic fluctuations in thermoelectric Heusler alloy Fe2VAl: A weak-coupling approachOral presentation
- 日本物理学会講演概要集(CD-ROM), 2024Ferromagnetic fluctuations in Heusler thermoelectric material Fe2VAl: A weak-coupling approach
- 第2回「富岳」成果創出加速プログラム 研究交流会, Mar. 2023First-principles analysis of planar defect in layered perovskite Y2Ti2O5S2Poster presentation
- PCoMS Symposium & Annual meeting of Supercomputing Consortium for Computational Materials Science 2022, Feb. 2023First-principles analysis of defects in layered perovskite photocatalyst Y2Ti2O5S2Oral presentation
- 分子科学討論会講演プログラム&要旨(Web), 2023First-Principles Analysis of Doped Layered Perovskite Semiconductor Photocatalyst Y2Ti2O5S2
- 分子科学討論会講演プログラム&要旨(Web), 2023First-principles analysis of doped perovskite semiconductor photocatalysts: toward promoting photocatalytic performance
- 日本物理学会講演概要集(CD-ROM), 2023Theoretical study of spin fluctuations in Heusler compound Fe2VAl
- 分子科学討論会講演プログラム&要旨(Web), 2022Theoretical Study of Planar Defect in Layered Perovskite Photocatalyst Y2Ti2O5S2
- 日本物理学会講演概要集(CD-ROM), 2022Theoretical study of spin fluctuations in Heusler compound Fe2VAl
- 1st Japan-France Virtual Workshop on Thermoelectrics, Sep. 2021, EnglishPossibility of n-type doping in CaAl2Si2-type Zintl phase compound CaZn2X2 (X = As, P)Poster presentation
- 日本物理学会講演概要集(CD-ROM), 2021Theoretical study of n-type doping and its formation energy for thermoelectric material 122-Zintl phase compound with the first-principles calculations
- 日本物理学会講演概要集(CD-ROM), 2020Effects of electron correlations on ferromagnetic fluctuations in heavily over-doped cuprates
- 日本物理学会講演概要集(CD-ROM), 2020Theoretical study of impurity doping and its formation energy for thermoelectric material 122-Zintl phase compound with the first-principles calculations
- 1 & 2DM Conference, EnglishMagnetic Field Dependence of Opening and Closing Dirac Cone in Ni/Graphene/Ni nano-spin-valve-like structureOral presentation
- 応用物理学会春季学術講演会講演予稿集(CD-ROM), 2019Nd2CuO4における3d/4f局在電子軌道の第一原理有効ハミルトニアンの理論的評価
- 応用物理学会秋季学術講演会講演予稿集(CD-ROM), 2019Nd2CuO4における3d/4f局在電子軌道の超交換相互作用の理論的評価
- 日本物理学会講演概要集(CD-ROM), 2018電子相関の層分化から生じる多層系銅酸化物の高温超伝導
- 日本物理学会講演概要集(CD-ROM), 2018銅酸化物におけるバッファ層構造の違いに起因する遮蔽効果の物質依存性
- 日本物理学会講演概要集(CD-ROM), 2018コヒーレントフォノン導入によるディラック点の移動とアームチェア・エッジ状態の理論
- APS March Meeting 2017, Mar. 2017, EnglishAn effective 2-band ���� model of sulfur hydride H3S for high-��c superconductivity[Invited]Oral presentation
- 日本物理学会講演概要集(CD-ROM), 2017強相関電子系の量子時間発展演算子表現におけるアルゴリズム開発
- 日本物理学会講演概要集(CD-ROM), 2017Photon Pass processで記述した第一原理的電子正孔系量子ダイナミクス解析法
- 日本物理学会講演概要集(CD-ROM), 2017多層系銅酸化物超伝導体における反強磁性不安定性とフィリングの層依存性の多軌道二体自己無撞着法による解析
- 日本物理学会講演概要集(CD-ROM), 2017銅酸化物超伝導体における二電子交換相互作用増加効果の物質依存性と超伝導性解析
- 日本物理学会講演概要集(CD-ROM), 2017ルテニウム酸化物Sr2RuO4における超伝導の一軸性圧力効果の弱結合理論による研究
- The International Conference on STRONGLY CORRELATED ELECTRON SYSTEMS, May 2016, EnglishKnight shift of Sr2IrO4 in Pseudospin Singlet Superconductivity Induced by Large Spin-Orbit CouplingPoster presentation
- 日本物理学会講演概要集(CD-ROM), 2016イリジウム酸化物の超伝導状態におけるナイトシフトの乱雑位相近似による理論的解析
- APS March Meeting 2014, Mar. 2014, EnglishPossible Superconductivity Induced by Strong Spin-Orbit Coupling in Carrier Doped Iridium Oxides InsulatorsOral presentation
- The International Conference on STRONGLY CORRELATED ELECTRON SYSTEMS, Aug. 2013, EnglishTheoretical study for the superconductivity in Sr2IrO4Poster presentation
- APS March Meeting 2012, Feb. 2012, EnglishEffect of inter-layer single-electron hopping and pair-hopping on superconductivity in multi-layered cupratesPoster presentation
- Materials & Mechanisms of Superconductivity Conference (M2S), 2012, EnglishEffect of inter-layer pair hopping and single electron-hopping on superconductivity in multi-layered high-Tc cupratesPoster presentation
- GCOE International Symposium on Physical Sciences Frontier, 2012, EnglishEffect of inter-layer Pair hopping and One-electron hopping on Superconductivity in Multi-layered high-Tc CupratesPoster presentation
- XVI Training Course in the Physics of Strong Correlated Systems, 2011, EnglishTheoretical Study of Superconductivity in Multi-layered CupratesOral presentation
■ Research Themes
- Japan Society for the Promotion of Science, Grants-in-Aid for Scientific Research, Grant-in-Aid for Scientific Research (C), Kobe University, Apr. 2021 - Mar. 2024Theoretical study and material design of high performance thermoelectric materials arising from ferromagnetic spin fluctuations強磁性揺らぎによる熱電性能の増強のメカニズムを理解するために、代表物質であるホイスラー化合物Fe$_2$VAlに対して密度汎関数理論に基づく第一原理計算を行い、基本的な電子状態構造(状態密度やバンド構造)を得た。特に、フェルミレベル付近を構成する軌道成分としては、Feのd軌道やVのd軌道だけでなく、Alのs/p軌道も強く混成していることが見出された。更に、ドーパントの効果を調べるために、ドープされたFe$_2$VAl(Fe$_2$V$_{0.9}$Cr$_{0.1}$Al$_{0.9}$Si$_{0.1}$やFe$_{2.2}$V$_{0.8}$Al$_{1-y}$Si$_y$)の電子状態についてスーパーセルを用いて数値解析を行った。スーパーセル計算では、CrのV置換ドープやVのFe置換ドープの場合には、キャリアドープとともにスピン分極し磁気モーメントが誘起され、SiのAl置換ドープの場合には、単純にキャリアがドープされることを見出した。また、強相関ソルバーによる強磁性揺らぎを考慮するために、最局在ワニエ関数を用いてFe$_2$VAlの第一原理有効模型を構築した。そこでは、フェルミレベル付近の軌道成分を取り込んだ低エネルギー模型として、Feのd軌道、Vのd軌道、そしてAlのs/p軌道を考慮した19(=5*2+5+1+3)軌道模型を見出した。これらの軌道成分は上述の通り強くエンタングルしており、これら全てを考慮することでフェルミレベル付近のバンド構造を再現することが出来た。