Resistivity in the Spin-Gap State of the t-J Model

Journal of the Physical Society of Japan

Volumn 67, Issue 8, 1998, Pages 2606-2609

  Onoda, Masaru ^a   Ichinose, Ikuo ^a   Matsui, Tetsuo ^b  

^a UNIVERSITY OF TOKYO   (Japan)

^b KINKI UNIVERSITY   (Japan)

Author keywords

Electric transport; Gauge field theory; High Tc superconductivity; Spin gap state; t J model

Indexed keywords

EID: 0032355395     PISSN: 00319015     EISSN: None     Source Type: Journal    
DOI: 10.1143/JPSJ.67.2606     Document Type: Article

References (27)

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7. I. Ichinose and T. Matsui: Nucl. Phys. B 394 (1993) 281; Phys. Rev. B 51 (1995) 11860; I. Ichinose, T. Matsui and K. Sakakibara: J. Phys. Soc. Jpn. 67 (1998) 543; N. Nagaosa: Phys. Rev. Lett. 71 (1993) 4210, also studied a CD transition of certain dissipative gauge theory of fermions.
8. I. Ichinose and T. Matsui: Nucl. Phys. B 394 (1993) 281; Phys. Rev. B 51 (1995) 11860; I. Ichinose, T. Matsui and K. Sakakibara: J. Phys. Soc. Jpn. 67 (1998) 543; N. Nagaosa: Phys. Rev. Lett. 71 (1993) 4210, also studied a CD transition of certain dissipative gauge theory of fermions.
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16. As early suggestions, see e.g., N. Nagaosa: J. Phys. Chem. Solids 53 (1992) 1493.
17. Although we do explicit calculations in two dimensions, we keep in mind that weak but finite three dimensionality is necessary to stabilize the spin gap.
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20. xi.
21. CSS since they are short-ranged.
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24. B. Thus this is a natural choice for the typical momentum scale of holons.
25. N. Nagaosa and P. A. Lee: Phys. Rev. B 45 (1992) 966, argued that the phase transition at T* becomes crossover due to the gauge-field fluctuations. Their argument has been criticized in the paper of Ichinose, Matsui and Sakakibara of ref. 3.
26. See also P. A. Lee and N. Nagaosa: Phys. Rev. Lett. 79 (1997) 3755.
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