2014
DOI: 10.1007/s10948-014-2549-5
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Pairing Symmetry, Spin Gap, and More in HTSC Cuprates

Abstract: This work is based on the double correlated linear aggregations of holes in checkerboard geometry. It is proved that the pairing function symmetry is -2 2 x y d , as been observed experimentally. It is also shown that there is a "superconductive spin gap" for the observation of the magnetic incommensurate modulation peaks, in agreement with experiment. In addition, the unperturbed Hamiltonian and its related propagator are reanalyzed and modified.

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Cited by 2 publications
(2 citation statements)
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“…The first suggestion that comes to mind is Eq. (18a) has actually been used, for the approximation of k  at low energies throughout my former works [2,12,14]. However, here we suggest that when the wavevector k is to be specifically expressed, Eq.…”
Section: F Qk mentioning
confidence: 90%
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“…The first suggestion that comes to mind is Eq. (18a) has actually been used, for the approximation of k  at low energies throughout my former works [2,12,14]. However, here we suggest that when the wavevector k is to be specifically expressed, Eq.…”
Section: F Qk mentioning
confidence: 90%
“…At the Fermi level |k| = k = k F and when one of them tends to zero, the other one tends to √ 2k F . Equation (18a) has actually been used for the approximation of εk at low energies throughout my former works [2,12,14]. However, here, we suggest that when the wave vectork is to be specifically expressed, (17) should be replaced by (18b) and not only as a low-energy approximation.…”
Section: The Low-energy Inward Dispersionmentioning
confidence: 90%