TY - JOUR
T1 - dx2-y2 wave pairing fluctuations and pseudo spin gap in two-dimensional electron systems
AU - Onoda, Shigeki
AU - Imada, Masatoshi
N1 - Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.
PY - 1999/8
Y1 - 1999/8
N2 - Pseudogap phenomena of high-Tc cuprates are examined. In terms of AFM (antiferromagnetic) and dSC (dx2-y2-wave superconducting) auxiliary fields introduced to integrate out the fermions, the effective action for 2D electron systems with AFM and dSC fluctuations is considered. By the self-consistent renormalization (SCR), the NMR relaxation rate T1-1, the spin correlation length ξσ and the pairing correlation length ξd are calculated. From this calculation, a mechanism of the pseudogap formation emerges as the region of dominant d-wave short-range order (SRO) over AFM-SRO. When damping for the AFM fluctuation strongly depends on the dSC correlation length through the formation of precursor singlets around (π, 0) and (0, π) points in the momentum space, the pseudogap appears in a region of the normal state characterized by decreasing 1/T1T and increasing AFM correlation length with decrease in temperature. This reproduces a characteristic feature of the pseudogap phenomena in many underdoped cuprates. When the damping becomes insensitive to the dSC correlation length, the pseudogap region shrinks as in the overdoped cuprates.
AB - Pseudogap phenomena of high-Tc cuprates are examined. In terms of AFM (antiferromagnetic) and dSC (dx2-y2-wave superconducting) auxiliary fields introduced to integrate out the fermions, the effective action for 2D electron systems with AFM and dSC fluctuations is considered. By the self-consistent renormalization (SCR), the NMR relaxation rate T1-1, the spin correlation length ξσ and the pairing correlation length ξd are calculated. From this calculation, a mechanism of the pseudogap formation emerges as the region of dominant d-wave short-range order (SRO) over AFM-SRO. When damping for the AFM fluctuation strongly depends on the dSC correlation length through the formation of precursor singlets around (π, 0) and (0, π) points in the momentum space, the pseudogap appears in a region of the normal state characterized by decreasing 1/T1T and increasing AFM correlation length with decrease in temperature. This reproduces a characteristic feature of the pseudogap phenomena in many underdoped cuprates. When the damping becomes insensitive to the dSC correlation length, the pseudogap region shrinks as in the overdoped cuprates.
KW - Antiferromagnetism
KW - High-T superconductivity
KW - Pseudogap
KW - Self-consistent renormalization
KW - Van-Hove singularity
KW - d--wave superconductivity
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U2 - 10.1143/JPSJ.68.2762
DO - 10.1143/JPSJ.68.2762
M3 - Article
AN - SCOPUS:0033413234
SN - 0031-9015
VL - 68
SP - 2762
EP - 2772
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 8
ER -