1.
Pseudogap phase in the U(1) gauge theory with incoherent spinon pa..
[427]

2.
Topological term in the nonlinear sigma model of the SO(5) spin c..
[249]

3.
Second Renormalization of TensorNetwork States
[215]

4.
Electronic Structures and Magnetic Order of OrderedFeVacancy Ter..
[208]

5.
Proximity effect at superconducting SnBi2Se3 interface
[200]

6.
Anisotropic neutron spin resonance in superconducting BaFe(1.9)Ni(..
[191]

7.
Antiferromagnetic Heisenberg ladders in staggered magnetic field
[189]

8.
Plaquette order and deconfined quantum critical point in the spin..
[188]

9.
Evidence for a generic quantum transition in highT(c) cuprates
[181]

10.
Comment on "Fano resonance for Anderson impurity systems"  Luo et..
[179]

11.
Doping effects on the twodimensional spin dimer compound SrCu2(BO..
[175]

12.
Probing the Hofstadter butterfly with the quantum oscillation of m..
[174]

13.
Neutron Scattering Studies of spin excitations in holedoped Ba0.6..
[174]

14.
Ternary iron selenide K0.8Fe1.6Se2 is an antiferromagnetic semicon..
[174]

15.
NormalState Hourglass Dispersion of the Spin Excitations in FeSe(..
[171]

16.
Translation invariant tensor product states in a finite lattice sy..
[171]

17.
Exact solutions of a class of S=1 quantum Ising spin models
[170]

18.
A quantum transfer matrix method for onedimensional disordered el..
[168]

19.
Renormalization of tensornetwork states
[165]

20.
Universal lineartemperature dependence of static magnetic suscept..
[164]

21.
Partial Order and FiniteTemperature Phase Transitions in Potts Mo..
[162]

22.
Electronic and magnetic structures of the ternary iron selenides A..
[162]

23.
Strongcoupling superconductivity in the nickelbased oxypnictide ..
[159]

24.
Gapped spinliquid states in a onedimensional Hubbard model with ..
[159]

25.
Midgap states in antiferromagnetic Heisenberg chains with a stagge..
[155]

26.
Superfluid response in monolayer highTc cuprates
[150]

27.
VALIDITY OF THE SINGLEBAND MODEL
[149]

28.
Superconductivity mediated by the antiferromagnetic spin wave in c..
[149]

29.
Pnicogenbridged antiferromagnetic superexchange interactions in i..
[146]

30.
Arsenicbridged antiferromagnetic superexchange interactions in La..
[144]

31.
Comment on "Timedependent densitymatrix renormalization group: A..
[143]

32.
Topologically distinct classes of valencebond solid states with t..
[142]

33.
Fano resonance for Anderson impurity systems
[139]

34.
Continuous quantum phase transition between two topologically dist..
[139]

35.
Edge solitons of topological insulators and fractionalized quasipa..
[138]

36.
Critical behavior in the lowenergy spin fluctuations in highT(c)..
[138]

37.
Instability of the Fermi surface in the onedimensional Kondo latt..
[138]

38.
Coarsegraining renormalization by higherorder singular value dec..
[138]

39.
Intrinsic electron and hole bands in electrondoped cuprate superc..
[137]

40.
Pseudogap and Fermi arc in kappatype organic superconductors
[136]

41.
Magnetic frustration and ironvacancy ordering in iron chalcogenid..
[136]

42.
Rigorous solution of the spin1 quantum ising model with singleio..
[135]

43.
Infrared probe of the electronic structure and charge dynamics of ..
[135]

44.
Fractality of Hofstadter Butterfly in Specific Heat Oscillation
[135]

45.
The electron pairing of KxFe2ySe2
[133]

46.
Penetration depth study of LaOs4Sb12: Multiband swave superconduc..
[133]

47.
Twodimensional algorithm of the densitymatrix renormalization gr..
[132]

48.
FirstPrinciples Calculations of the Electronic Structure of Tetra..
[131]

49.
caxis superfluid response and pseudogap in highTc superconducto..
[131]

50.
Effects of the DzyaloshinskiiMoriya interaction on lowenergy mag..
[131]

51.
Effect of bilayer coupling on tunneling conductance of doublelaye..
[131]

52.
String order and hidden topological symmetry in the SO(2n+1) symme..
[130]

53.
Accurate determination of tensor network state of quantum lattice ..
[130]

54.
Zigzag spin chains with antiferromagneticferromagnetic interactio..
[129]

55.
Exciton excitations in a onedimensional band insulator with Hubba..
[129]

56.
Angulardependent magnetoresistance oscillations in Na0.48CoO2 sin..
[128]

57.
Scaling of superconducting energy gap with critical temperature in..
[128]

58.
Electronic structures of ternary iron arsenides AFe(2)As(2) (A = B..
[127]

59.
Thermodynamic properties of tetrameric bondalternating spin chain..
[127]

60.
Metamagnetic transition in Na0.85CoO2 single crystals
[127]

61.
Twoband model of Raman scattering on electrondoped highT(c) sup..
[126]

62.
Lowfrequency spins and the ground state in highT(c) cuprates
[126]

63.
Effect of impurity resonance states on the NMR spectra of highTc..
[126]

64.
Evidence of swave pairing symmetry in the layered superconductor ..
[125]

65.
A GINZBURGLANDAU APPROACH FOR THE BA2YCU3O78 SUPERCONDUCTOR
[125]

66.
SuperfluidMottinsulator transition in a onedimensional optical ..
[124]

67.
Universal scaling behavior of the caxis resistivity of hightempe..
[124]

68.
Effects of the CuO chains on the anisotropic penetration depth of..
[124]

69.
Absence of the zero bias peak in vortex tunneling spectra of high..
[123]

70.
Efficient simulation of infinite tree tensor network states on the..
[123]

71.
Surface structures of ternary iron arsenides AFe(2)As(2) (A = Ba, ..
[122]

72.
Lowenergy physical properties of highTc superconducting Cu oxid..
[122]

73.
Geometrical structure effect on localization length of carbon nano..
[121]

74.
Electronic specific heat and lowenergy quasiparticle excitations ..
[120]

75.
Optical study of the metalinsulator transition in CuIr2S4 crystal..
[119]

76.
Scaling analysis of normalstate properties of hightemperature su..
[117]

77.
Lowtemperature magnetic and transport properties of layered SrxCo..
[117]

78.
Density matrix renormalization group study of a quantum impurity m..
[116]

79.
Universal caxis conductivity of highTc oxides in the supercondu..
[116]

80.
Microscopic hamiltonian for Zn or Nisubstituted hightemperature..
[116]

81.
Probing superconducting phase fluctuations from the current noise ..
[114]

82.
Thermodynamics of the bilinearbiquadratic spinone Heisenberg cha..
[114]

83.
Optimizing HartreeFock orbitals by the densitymatrix renormaliza..
[112]

84.
Penetration depth measurements in MgB2: Evidence for unconventiona..
[112]

85.
Atomic and electronic structures of FeSe monolayer and bilayer thi..
[112]

86.
Superfluid response in electrondoped cuprate superconductors
[110]

87.
Tunable Coulomb Blockade and Giant Coulomb Blockade Magnetoresista..
[110]

88.
Maximized string order parameters in the valence bond solid states..
[109]

89.
Inplane substitution effect on the magnetic properties of the two..
[109]

90.
Thermodynamics of quantum Heisenberg spin chains
[107]

91.
Effects of doping on thermally excited quasiparticles in the high..
[106]

92.
Class of exactly solvable SO(n) symmetric spin chains with matrix ..
[105]

93.
Low temperature superfluid response of highTc superconductors
[105]

94.
Topological characterization of quantum phase transitions in a spi..
[104]

95.
Relationship between the superconducting energy gap and the critic..
[95]

96.
Quantum torus chain
[88]

97.
Partial longrange order in antiferromagnetic Potts models
[86]

98.
Charge dynamics of the antiferromagnetically ordered Mott insulato..
[79]

99.
Gapless SpinLiquid Ground State in the S=1/2 Kagome Antiferromagn..
[75]

100.
Optimized contraction scheme for tensornetwork states
[69]
