| 127 | “Local structural disorder introduced by Cr in fcc high-/medium-entropy alloys consisting of 3d transition metal elements” (Featured Article) |
|---|---|
| 126 | “Magnetic structure of the noncentrosymmetric magnet Sr2MnSi2O7 through irreducible representation and magnetic space group analysis” |
| 125 | “Large nonlinear optical magnetoelectric response in a noncentrosymmetric magnetic Weyl semimetal” |
| 124 | “Diamond lattice in single-component molecular crystals comprising tetrabenzoporphyrin neutral radicals” |
| 123 | “Ferrimagnetic charge order in molecular conductors with diluted localized spins exhibiting enhanced giant magnetoresistance effect” |
| 122 | “Variation of Landau level splitting in the Fermi level controlled Dirac metals (Eu,Gd)MnBi2” |
| 121 | “Robustness of semimetallic transport properties of TaAs against off-stoichiometric disorder” |
| 120 | 「広域X線吸収微細構造法で見るミディアムエントロピー合金CrCoNiの局所構造」 |
| 119 | “Giant negative magnetoresistance in the layered semiconductor CeTe2-xSbx with variable magnetic polarom density” |
| 118 | “Field-tunable Weyl points and large anomalous Hall effect in the degenerate magnetic semiconductor EuMg2Bi2” |
| 117 | “Anomalous Nernst effect in the nonmagnetic nodal-line semimetal PbTaSe2” |
| 116 | “In-plane anisotropic charge dynamics in the layered polar Dirac semimetal BaMnSb2” |
| 115 | “Reversible Insulator-Metal Transition by Chemical Doping and Dedoping of a Mott Insulator” |
| 114 | “A large negative magnetoresistance effect in semiconducting crystals composed of an octahedrally ligated phthalocyanine complex with high-spin manganese(III)” |
| 113 | “Giant anisotropic magnetoresistance at low magnetic fields in a layered semiconductor” |
| 112 | “Optimizations of the Sintering Temperature to Reduce the Nd3RuO7 Phase and Investigations of their Effect on the Magnetic Properties in Nd2Ru2O7” |
| 111 | “Element dependence of local disorder in medium-entropy alloy CrCoNi” |
| 110 | “Variation of charge dynamics upon antiferromagnetic transitions in the Dirac semimetal EuMnBi2” |
| 109 | “Enhancing Thermopower and Nernst Signal of High-Mobility Dirac Carriers by Fermi Level Tuning in the Layered Magnet EuMnBi2” |
| 108 | “An electrically conducting molecular crystal composed of a magnetic iron (III) complex (S=1/2) with a large aromatic ligand, 1,2-naphthlalocyanine (C4th isomer): towards the development of molecular spintronics” |
| 107 | “Tunable spin-valley coupling in layered polar Dirac metals” |
| 106 | “181Ta nuclear quardrupole resonance study of the noncentrosymmetric superconductor PbTaSe2” |
| 105 | “Resonant X-ray Diffraction Study of Antiferromagnetic Transition in GdNiC2” |
| 104 | “Angular dependence of interlayer magnetoresistance for antiferromagnetic Dirac semimetal AMnBi2(A=Sr, Eu)” |
| 103 | “Bulk quantum Hall effect of spin-vally coupled Dirac fermions in the polar aniferromagnet BaMnSb2” |
| 102 | “Angle-dependent nontrivial phase in the Weyl semimetal NbAs with anisotropic Fermi surface” |
| 101 | “Intermolecular interactions of tetrabenzoporphyrin – and phthalocyanine – based charge – transfer complexes” |
| 100 |
“Large Enhancement of Thermoelectric Efficiency Due to a Pressure-Induced Lifshitz Transition in SnSe” |
|---|---|
| 99 |
“Defect-induced electronic structures on SnSe surfaces” |
| 98 |
“Nanoscale ice-type structural fluctuation in spinel titanates” |
| 97 |
“Quantitative evaluation of Dirac physics in PbTe” |
| 96 |
“Microwave nonreciprocity of magnon excitations in the noncentrosymmetric antiferromagnet Ba2MnGe2O7” |
| 95 |
“An electrically conducting crystal composed of an octahedrally ligated porphyrin complex with high-spin iron(Ⅲ)” |
| 94 |
“Enhanced magnetoresistance in the binary semimetal NbAs2 due to improved crystal quality” |
| 93 |
“Electrochemical synthesis of phthalocyanine-molecular mixed crystals in dilute solution” |
| 92 |
“PVD thin film growth of M(Pc)(CN)2 axially substituted metal-phtalocyanines” |
| 91 |
“A new strategy for inducing dipole moments in charge-transfer complexes: introduction of asymmetry into axially ligated iron phthalocyanines” |
| 90 |
「金属フタロシアニン系伝導体における分子設計と巨大磁気抵抗効果」 |
| 89 |
“Axially Ligated Phthalocyanine Conductors with Magnetic Moments” |
| 88 |
“Synthesis and Characterization of Iodide-coordinated Dinuclear Molecular Single Crystal Cr2(μ-I)2I4(C8N2H4)4” |
| 87 |
“Interplay between charge-density wave and antiferromagnetic order in GdNiC2” |
| 86 |
“A giant negative magnetoresistance effect in an iron tetrabenzoporphyrin complex” |
| 85 |
“Phthalocyanine-Based Single-Component Molecular Conductor [MnIII(Pc)(CN)]2O” |
| 84 |
“High Magnetic Field Study on Giant Negative Magnetoresistance in the Molecular Conductor TPP[Cr(Pc)(CN)2]2” |
| 83 |
“Multiple charge density wave transitions in the antiferromagnets RNiC2(R=Gd,Tb)” |
| 82 |
“Observation of all-in type tetrahedral displacements in nonmagnetic pyrochlore niobates” |
| 81 |
“Effect of Localized Spin Concentration on Giant Magnetoresistance in Molecular Conductor TPP[FexCo1-x(Pc)(CN)2]2” |
| 80 |
“Giant ferromagnetic p–d interaction in a phthalocyanine molecule” |
| 79 |
“One-dimensional phthalocyanine-based conductor with S=3/2 isotopic magnetic centers” |
| 78 |
“Metal-Insulator Transition and Thermoelectric Properties in Hexagonal Barium Titanates” |
| 77 |
“Bistable Multifunctionality and Switchable Strong Ferromagnetic-to-Antiferromagnetic Coupling in a One-Dimensional Rhodium(I)-Semiquinonato Complex” |
| 76 |
“Magnetoelectric Effect in FeSb2O4 Single Crystals” |
| 75 |
“Ligand and Charge Dependence for Absorption Edge in XANES spectra of TPP[Fe(Pc)L2]2 systems” |
| 74 |
“Metamagnetic Transition and Its Related Magnetocapacitance Effect in Phthalocyanine-Molecular Conductor Exhibiting Giant Magnetoresistance” |
| 73 |
“Magnetic torque experiments on TPP[Fe(Pc)L2]2 (L=Br and Cl):Antiferromagnetic short range ordering of d electrons, Antiferromagnetic ordering of p electrons, and anisotropy energy” |
| 72 |
“Thermoelectric Effect in Hexagonal Tungsten Oxides” |
| 71 |
“XANES analysis of phthalocyanine molecular conductor” |
| 70 |
“Magnetic field switching of the charge-density-wave state in the lanthanide intermetallic SmNiC2” |
| 69 |
“Successive transition in Rare-earth intermetallic compound GdNiC2” |
| 68 |
“X-ray Absorption Spectra in Pyrochlore Niobates” |
| 67 |
“Hydrothermal Synthesis of Hexagonal Vanadium Oxide” |
| 66 |
“Charge order competition leading to nonlinearity in organic thyristor family” |
| 65 |
“Interplay between charge-density waves and superconductivity in the organic conductor b’’-(BEDT-TTF)2AuBr2” |
| 64 |
“Giant magnetoresistance response by the p-d interaction in an axially ligated phthalocyanine conductor with two-dimensional p-p stacking structure” |
| 63 |
“Magneto-electric effect in charge-ordered LuFe2O4” |
| 62 |
“Nonequilibrium charge ordering in q-(BEDT-TTF)2MM’(SCN)4 (M=Rb, Cs; M’=Co, Zn)” |
| 61 |
“Magnetic torque measurements of TPP[Fe(Pc)Br2]2” |
| 60 |
“Synchrotron X-ray study of charge density waves in ο-TaS3” |
| 59 |
“Variable magnetotransport properties in the TPP[Fe(Pc)L2]2 system (TPP = tetraphenylphosphonium, Pc=phthalocyaninato, L=CN, Cl and Br)” |
| 58 |
“Emergence of a diffusive metal state with no magnetic order near the Mott transition in frustrated pyrochlore-type molybdates” |
| 57 |
“Magnetic torque and ac and dc magnetic susceptibility measurements on PTMA0.5[Fe(Pc)(CN)2]CH3CN : Origin of spontaneous magnetization in [Fe(Pc)(CN)2] molecular conductors” |
| 56 |
“Nonlinear Transport Phenomena in Highly One-dimensional MIII(Pc)(CN)2 Chains with p-d Interaction (M = Co and Fe and Pc =Phthalocyaninato)” |
| 55 |
“Stoichiometric study of the dielectric and magnetic properties in charge frustrated system LuFe2O4” |
| 54 |
“Commensurate-incommensurate transition of charge density waves in o-TaS3” |
| 53 |
“Anomalous Nernst effects in pyrochlore molybdates with spin chirality ” |
| 52 |
“Non-thermal evidence for current-induced melting of charge order in q-(BEDT-TTF)2CsZn(SCN)4” |
| 51 |
“Field-induced discommensuration in charge density waves in o-TaS3” |
| 50 |
“Magnetic torque and heat capacity measurements on TPP[Fe(Pc)(CN)2]2” |
| 49 |
「金属フタロシアニン錯体」 |
| 48 |
“Scaling of anomalous Hall resistivity in Nd2(Mo1-xNbx)2O7 with spin chirality” |
| 47 |
“Nature of transition between a ferromagnetic metal and a spin-glass insulator in pyrochlore molybdates” |
| 46 |
「磁場によって電気抵抗が激減する分子性物質」 |
| 45 |
“Giant negative magnetoresistance reflecting molecular symmetry in dicyano (phthalocyaninate)iron compounds” (Editor’s Choice) |
| 44 |
“Mott-Anderson transition controlled by magnetic field in pyrochlore molybdate” |
| 43 |
“Variation of the charge dynamics in bandwidth and filling controlled metal-insulator transitions of pyrochlore-type molybdates” |
| 42 |
“Charge disproportionation in highly one-dimensional molecular conductor TPP[Co(Pc)(CN)2]2” |
| 41 |
“Electrical inhomogeneity at the Mott transition in the band with controlled k-(BEDT-TTF)2Cu[N(CN)2]Br” |
| 40 |
“Magneto-optical effect induced by the spin chirality in the itinerant ferromagnet Nd2Mo2O7” |
| 39 |
“Electronic correlation in the infrared optical properties of the quasi two dimensional k-type BEDT-TTF dimer system” |
| 38 |
“Novel electroluminescence properties of thin films using soluble metallophthalocyanine salts” |
| 37 |
“Charge dynamics near the electron-correlation induced metal-insulator transition in pyrochlore-type molybdates” |
| 36 |
“Anisotripic giant magnetoresistance originating from the p-d interaction in a molecule” |
| 35 |
“Infrared optical conductivity and the electronic phase diagram in the organic superconductor k-(BEDT-TTF)2X” |
| 34 |
“Molecular unit based on metal phthalocyanine; designed for molecular electronics” |
| 33 |
実験化学講座（丸善）第5版 第７巻「電気物性、磁気物性」、 |
| 32 |
“Fabrication of thin films using a soluble metal phthalocyanine salt and their photocoductive properties” |
| 31 |
“A light-emitting diode fabricated from horse–heart cytochrome c” |
| 30 |
“Charge-density-wave state within Pd(dmit)2 layer in two-dimensional molecular conductor (IEDT)[Pd(dmit)2]” |
| 29 |
“Structure and physical properties of low-dimensional molecular conductors, [PXX][FeIII(Pc)(CN)2] and [PXX][CoIII(Pc)(CN)2] (PXX = peri-xanthenoxanthene, Pc = phthalocyaninato)” |
| 28 |
“Contribution of degenerate molecular orbitals to molecular orbital angular momentum in molecular magnet Fe(Pc)(CN)2” |
| 27 |
“Infrared reflectance spectra of a-ET2KHg(SCN)4 under high magnetic field” |
| 26 |
“One-dimensional p-d electron system in TPP[Fe(Pc)(CN)2]2, [PXX][Fe(Pc)(CN)2], and (PTMA)x[Fe(Pc)(CN)2]Y(CH3CN) : Electron spin resonance and negative magnetoresistance” |
| 25 |
“Magnetic and optical properties of one-dimensional p-d system with axially substituted iron(III) phthalocyanine” |
| 24 |
“Magnetic properties of d-p conducting system, TPP[FeIIIxCoIII1-x(Pc)(CN)2]2” |
| 23 |
“Torque study of TPP[Fe(Pc)(CN)2]2 (TPP = tetraphenylphosphonium and Pc = phthalocyanine)” |
| 22 |
“Magnetoresistance study on TPP[M(Pc)(CN)2]2 [M=Fe, Co, Fe0.30Co0.70] salts” |
| 21 |
“One-dimensional p-d system with axially substituted iron(III) phthalocyanine” |
| 20 |
“Angle-dependent magnetoresistance oscillations in the quasi-two-dimensional organic conductor a-(BEDT-TTF)2NH4Hg(SCN)4 : Origin of the difference in ground state between a-(BEDT-TTF)2NH4Hg(SCN)4 and a-(BEDT-TTF)2KHg(SCN)4” |
| 19 |
“Structure and electrical and magnetic properties of (PTMA)x[M(Pc)(CN)2]・y(solvent) (PTMA= phenyltrimethylammonium and [M(Pc)(CN)2]= dicyano(phthalocyaninato)MIII with M= Co and Fe). Partial oxidation by partial solvent occupation of the cation site” |
| 18 |
“Giant negative magnetoresistance of one-dimensional conductor TPP[Fe(Pc)(CN)2]2” |
| 17 |
“Phase diagrams of (DMe-DCNQI)Li1-xCux system” |
| 16 |
“A one-dimensional macrocyclic p-ligand conductor carrying a magnetic center. Structure and electrical, optical and magnetic properties of TPP[Fe(Pc)(CN)2]2 {TPP=tetraphenylphosphonium and [Fe(Pc)(CN)2] = dicyano(phthalocyaninato)iron(III)}” |
| 15 |
“Giant negative magnetoresistance in one-dimensional p-d system : TPP[Fe(Pc)(CN)2]2 (TPP=tetraphenylphosphonium, Pc=phthalocyanine)” |
| 14 |
“Giant negative magnetoresistance in quasi-one-dimensional conductor TPP[Fe(Pc)(CN)2]2 : interplay between 3d-local moments and one-dimensional conduction electrons” |
| 13 |
“Upper critical field of the molecular superconductor b’– Et2Me2P[Pd(dmit)2]2” |
| 12 |
“Reply to “Comment on “Contribution of small closed orbits to magnetoresistance in quasi-two-dimensional conductors””” |
| 11 |
“Hybrid-dimensional system in M(dmit)2 salts” |
| 10 |
“AMRO study of Fermi surface nesting of (BEDT-TTF)2MHg(SCN)4 , M=K and NH4” |
| 9 |
“Physical properties of (TMET-STF)2BF4” |
| 8 |
“Contribution of small closed orbits to magnetoresistance in quasi-two-dimensional conductors” |
| 7 |
“A new molecular superconductor b’-Et2Me2P[Pd(dmit)2]2 (dmit =2-thioxo-1,3-dithiole-4,5-dithiolate)” |
| 6 |
“Electronic states of low-dimensional organic conductors (DMeDCNQI)2Cu and a-(BEDT-TTF)2KHg(SCN)4 under pressure” |
| 5 |
“The pressure approach to the origin of the anomalous state in the quasi-two-dimensional organic conductor a-(BEDT-TTF)2KHg(SCN)4 “ |
| 4 |
“Angle dependent magnetoresistance oscillations of a-(BEDT-TTF)2KHg(SCN)4 under high pressure” |
| 3 |
“Pressure effects to the anomalous state of quasi two-dimensional conductor a-(BEDT-TTF)2KHg(SCN)4” |
| 2 |
“The origin of anomalous angular dependent magnetoresistance oscillation effect in a-(BEDT-TTF)2KHg(SCN)4” |
| 1 |
“Study of the angular dependent magnetoresistance oscillations in a-(BEDT-TTF)2MHg(SCN)4 [M : K, NH4]” |