Nature of a single doped hole in two-leg Hubbard and t-J ladders
被引:6
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作者:
Liu, Shenxiu
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Stanford Univ, Dept Phys, Stanford, CA 94305 USA
Stanford Inst Mat & Energy Sci, SLAC Natl Accelerator Lab, Menlo Pk, CA 94025 USA
Stanford Univ, Menlo Pk, CA 94025 USAStanford Univ, Dept Phys, Stanford, CA 94305 USA
Liu, Shenxiu
[1
,2
,3
]
Jiang, Hong-Chen
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机构:
Stanford Inst Mat & Energy Sci, SLAC Natl Accelerator Lab, Menlo Pk, CA 94025 USA
Stanford Univ, Menlo Pk, CA 94025 USAStanford Univ, Dept Phys, Stanford, CA 94305 USA
Jiang, Hong-Chen
[2
,3
]
Devereaux, Thomas P.
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Stanford Inst Mat & Energy Sci, SLAC Natl Accelerator Lab, Menlo Pk, CA 94025 USA
Stanford Univ, Menlo Pk, CA 94025 USA
Stanford Univ, Dept Phys, Geballe Lab Adv Mat, Stanford, CA 94305 USA
Stanford Univ, Dept Appl Phys, Stanford, CA 94305 USAStanford Univ, Dept Phys, Stanford, CA 94305 USA
Devereaux, Thomas P.
[2
,3
,4
,5
]
机构:
[1] Stanford Univ, Dept Phys, Stanford, CA 94305 USA
[2] Stanford Inst Mat & Energy Sci, SLAC Natl Accelerator Lab, Menlo Pk, CA 94025 USA
[3] Stanford Univ, Menlo Pk, CA 94025 USA
[4] Stanford Univ, Dept Phys, Geballe Lab Adv Mat, Stanford, CA 94305 USA
[5] Stanford Univ, Dept Appl Phys, Stanford, CA 94305 USA
In this paper, we have systematically studied the single-hole problem in two-leg Hubbard and t-J ladders by large-scale density-matrix renormalization-group calculations. We found that the doped holes in both models behave similarly, while the three-site correlated hopping term is not important in determining the ground-state properties. For more insights, we have also calculated the elementary excitations, i.e., the energy gaps to the excited states of the system. In the strong-rung limit, we found that the doped hole behaves as a Bloch quasiparticle in both systems where the spin and charge of the doped hole are tightly bound together. In the isotropic limit, while the hole still behaves like a quasiparticle in the long-wavelength limit, our results show that its spin and charge components are only loosely bound together inside the quasiparticle, whose internal structure can lead to a visible residual effect which dramatically changes the local structure of the ground-state wave function.
机构:
Lab. de Physique Theáorique, CNRS-UMRS5152, Universiteá Paul Sabatier, F-31062 Toulouse, FranceLab. de Physique Theáorique, CNRS-UMRS5152, Universiteá Paul Sabatier, F-31062 Toulouse, France
Poilblanc, Didier
Scalapino, D.J.
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Physics Department, University of California, Santa Barbara, CA 93106, United StatesLab. de Physique Theáorique, CNRS-UMRS5152, Universiteá Paul Sabatier, F-31062 Toulouse, France
Scalapino, D.J.
Capponi, Sylvain
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Lab. de Physique Theáorique, CNRS-UMRS5152, Universiteá Paul Sabatier, F-31062 Toulouse, France
Department of Physics, Stanford University, Stanford, CA 94305, United StatesLab. de Physique Theáorique, CNRS-UMRS5152, Universiteá Paul Sabatier, F-31062 Toulouse, France