Low-energy spectra in t-J-type models at low doping levels
Based on a variational approach, we propose that there are two kinds of low-energy states in the t-J-type models at low doping. In a quasiparticle state an unpaired spin bound to a hole with a well-defined momentum can be excited with spin waves. The resulting state shows a suppression of antiferrom...
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Published in | Physical review letters Vol. 91; no. 5; p. 057001 |
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Main Authors | , , , |
Format | Journal Article |
Language | English |
Published |
United States
01.08.2003
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Abstract | Based on a variational approach, we propose that there are two kinds of low-energy states in the t-J-type models at low doping. In a quasiparticle state an unpaired spin bound to a hole with a well-defined momentum can be excited with spin waves. The resulting state shows a suppression of antiferromagnetic order around the hole with the profile of a spin bag. These spin-bag states with spin and charge or hole separated form a continuum of low-energy excitations. Very different properties predicted by these two kinds of states explain a number of anomalous results observed in the exact diagonalization studies on small clusters up to 32 sites. |
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AbstractList | Based on a variational approach, we propose that there are two kinds of low-energy states in the t-J-type models at low doping. In a quasiparticle state an unpaired spin bound to a hole with a well-defined momentum can be excited with spin waves. The resulting state shows a suppression of antiferromagnetic order around the hole with the profile of a spin bag. These spin-bag states with spin and charge or hole separated form a continuum of low-energy excitations. Very different properties predicted by these two kinds of states explain a number of anomalous results observed in the exact diagonalization studies on small clusters up to 32 sites. |
Author | Lee, Wei-Cheng Lee, T K Leung, P W Ho, Chang-Ming |
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BackLink | https://www.ncbi.nlm.nih.gov/pubmed/12906623$$D View this record in MEDLINE/PubMed |
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CitedBy_id | crossref_primary_10_1103_PhysRevB_73_104502 crossref_primary_10_1143_JPSJ_74_3340 crossref_primary_10_1103_PhysRevB_99_205128 crossref_primary_10_1103_PhysRevLett_95_057001 crossref_primary_10_1016_j_jpcs_2008_06_015 crossref_primary_10_1103_PhysRevB_73_052501 crossref_primary_10_1016_j_jpcs_2005_10_049 crossref_primary_10_1103_PhysRevB_96_115114 crossref_primary_10_1088_1367_2630_15_4_043045 crossref_primary_10_1103_RevModPhys_78_17 crossref_primary_10_1140_epjb_e2007_00028_4 crossref_primary_10_1103_PhysRevB_71_134522 crossref_primary_10_1103_PhysRevLett_100_117004 |
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