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1.
Nature ; 406(6799): 965-8, 2000 Aug 31.
Artículo en Inglés | MEDLINE | ID: mdl-10984044

RESUMEN

One of the most striking properties of the high-transition-temperature (high-Tc) superconductors is that they are all derived from insulating antiferromagnetic parent compounds. The intimate relationship between magnetism and superconductivity in these copper oxide materials has intrigued researchers from the outset, because it does not exist in conventional superconductors. Evidence for this link comes from neutron-scattering experiments that show the unambiguous presence of short-range antiferromagnetic correlations (excitations) in the high-Tc superconductors. Even so, the role of such excitations in the pairing mechanism for superconductivity is still a subject of controversy. For YBa2Cu3O(6+x), where x controls the hole-doping level, the most prominent feature in the magnetic excitation spectrum is a sharp resonance (refs 6-11). Here we show that for underdoped YBa2Cu3O6.6, where x and Tc are below their optimal values, modest magnetic fields suppress the resonance significantly, much more so for fields approximately perpendicular to the CuO2 planes than for parallel fields. Our results indicate that the resonance measures pairing and phase coherence, suggesting that magnetism plays an important role in high-Tc superconductivity. The persistence of a field effect above Tc favours mechanisms in which the superconducting electron pairs are pre-formed in the normal state of underdoped copper oxide superconductors, awaiting transition to the superconducting state.

2.
Phys Rev Lett ; 66(6): 821-824, 1991 Feb 11.
Artículo en Inglés | MEDLINE | ID: mdl-10043909
3.
Phys Rev Lett ; 62(6): 657-660, 1989 Feb 06.
Artículo en Inglés | MEDLINE | ID: mdl-10040295
5.
Phys Rev Lett ; 77(8): 1604-1607, 1996 Aug 19.
Artículo en Inglés | MEDLINE | ID: mdl-10063120
7.
Phys Rev Lett ; 71(6): 919-922, 1993 Aug 09.
Artículo en Inglés | MEDLINE | ID: mdl-10055401
8.
Phys Rev Lett ; 67(13): 1791-1794, 1991 Sep 23.
Artículo en Inglés | MEDLINE | ID: mdl-10044248
9.
Phys Rev Lett ; 67(25): 3622-3625, 1991 Dec 16.
Artículo en Inglés | MEDLINE | ID: mdl-10044782
10.
Phys Rev Lett ; 68(7): 1061-1064, 1992 Feb 17.
Artículo en Inglés | MEDLINE | ID: mdl-10046068
11.
Phys Rev Lett ; 62(17): 2052-2055, 1989 Apr 24.
Artículo en Inglés | MEDLINE | ID: mdl-10039844
13.
Phys Rev Lett ; 72(5): 701-704, 1994 Jan 31.
Artículo en Inglés | MEDLINE | ID: mdl-10056501
14.
16.
Phys Rev B Condens Matter ; 42(16): 10220-10225, 1990 Dec 01.
Artículo en Inglés | MEDLINE | ID: mdl-9995280
17.
Phys Rev B Condens Matter ; 54(10): R6905-R6908, 1996 Sep 01.
Artículo en Inglés | MEDLINE | ID: mdl-9984410
19.
Science ; 278(5342): 1432-5, 1997 Nov 21.
Artículo en Inglés | MEDLINE | ID: mdl-9367949

RESUMEN

Polarized and unpolarized neutron scattering was used to measure the wave vector- and frequency-dependent magnetic fluctuations in the normal state (from the superconducting transition temperature, Tc = 35 kelvin, up to 350 kelvin) of single crystals of La1.86Sr0.14CuO4. The peaks that dominate the fluctuations have amplitudes that decrease as T-2 and widths that increase in proportion to the thermal energy, kBT (where kB is Boltzmann's constant), and energy transfer added in quadrature. The nearly singular fluctuations are consistent with a nearby quantum critical point.

20.
Science ; 284(5418): 1344-7, 1999 May 21.
Artículo en Inglés | MEDLINE | ID: mdl-10334986

RESUMEN

Inelastic neutron scattering was used to study the wave vector- and frequency-dependent magnetic fluctuations in single crystals of superconducting YBa2Cu3O6+x. The spectra contain several important features, including a gap in the superconducting state, a pseudogap in the normal state, and the much-discussed resonance peak. The appearance of the pseudogap determined from transport and nuclear resonance coincides with formation of the resonance in the magnetic excitations. The exchange energy associated with the resonance has the temperature and doping dependences as well as the magnitude to describe approximately the electronic specific heat near the superconducting transition temperature (Tc).

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