Two-dimensional geometry of spin excitations in the high-transition-temperature superconductor YBa2Cu3O6+x
The fundamental building block of the copper oxide superconductors is a Cu 4 O 4 square plaquette. The plaquettes in most of these materials are slightly distorted to form a rectangular lattice, for which an influential theory predicts that high-transition-temperature (high- T c ) superconductivity...
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| Vydáno v: | Nature (London) Ročník 430; číslo 7000; s. 650 - 654 |
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| Hlavní autoři: | , , , , , , , , , |
| Médium: | Journal Article |
| Jazyk: | angličtina |
| Vydáno: |
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Nature Publishing Group UK
05.08.2004
Nature Publishing Group |
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| ISSN: | 0028-0836, 1476-4687, 1476-4687 |
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| Abstract | The fundamental building block of the copper oxide superconductors is a Cu
4
O
4
square plaquette. The plaquettes in most of these materials are slightly distorted to form a rectangular lattice, for which an influential theory predicts that high-transition-temperature (high-
T
c
) superconductivity is nucleated in ‘stripes’ aligned along one of the axes
1
,
2
,
3
. This theory received strong support from experiments that indicated a one-dimensional character for the magnetic excitations in the high-
T
c
material YBa
2
Cu
3
O
6.6
(ref.
4
). Here we report neutron scattering data on ‘untwinned’ YBa
2
Cu
3
O
6+
x
crystals, in which the orientation of the rectangular lattice is maintained throughout the entire volume. Contrary to the earlier claim
4
, we demonstrate that the geometry of the magnetic fluctuations is two-dimensional. Rigid stripe arrays therefore appear to be ruled out over a wide range of doping levels in YBa
2
Cu
3
O
6+
x
, but the data may be consistent with liquid-crystalline stripe order
5
. The debate about stripes has therefore been reopened. |
|---|---|
| AbstractList | The fundamental building block of the copper oxide superconductors is a Cu
4
O
4
square plaquette. The plaquettes in most of these materials are slightly distorted to form a rectangular lattice, for which an influential theory predicts that high-transition-temperature (high-
T
c
) superconductivity is nucleated in ‘stripes’ aligned along one of the axes
1
,
2
,
3
. This theory received strong support from experiments that indicated a one-dimensional character for the magnetic excitations in the high-
T
c
material YBa
2
Cu
3
O
6.6
(ref.
4
). Here we report neutron scattering data on ‘untwinned’ YBa
2
Cu
3
O
6+
x
crystals, in which the orientation of the rectangular lattice is maintained throughout the entire volume. Contrary to the earlier claim
4
, we demonstrate that the geometry of the magnetic fluctuations is two-dimensional. Rigid stripe arrays therefore appear to be ruled out over a wide range of doping levels in YBa
2
Cu
3
O
6+
x
, but the data may be consistent with liquid-crystalline stripe order
5
. The debate about stripes has therefore been reopened. The fundamental building block of the copper oxide superconductors is a Cu4O4 square plaquette. The plaquettes in most of these materials are slightly distorted to form a rectangular lattice, for which an influential theory predicts that high-transition-temperature (high-T(c)) superconductivity is nucleated in 'stripes' aligned along one of the axes. This theory received strong support from experiments that indicated a one-dimensional character for the magnetic excitations in the high-T(c) material YBa2Cu3O6.6 (ref. 4). Here we report neutron scattering data on 'untwinned' YBa2Cu3O6+x crystals, in which the orientation of the rectangular lattice is maintained throughout the entire volume. Contrary to the earlier claim, we demonstrate that the geometry of the magnetic fluctuations is two-dimensional. Rigid stripe arrays therefore appear to be ruled out over a wide range of doping levels in YBa2Cu3O6+x, but the data may be consistent with liquid-crystalline stripe order. The debate about stripes has therefore been reopened. The fundamental building block of the copper oxide superconductors is a Cu4O4 square plaquette. The plaquettes in most of these materials are slightly distorted to form a rectangular lattice, for which an influential theory predicts that high-transition-temperature (high-T(c)) superconductivity is nucleated in 'stripes' aligned along one of the axes. This theory received strong support from experiments that indicated a one-dimensional character for the magnetic excitations in the high-T(c) material YBa2Cu3O6.6 (ref. 4). Here we report neutron scattering data on 'untwinned' YBa2Cu3O6+x crystals, in which the orientation of the rectangular lattice is maintained throughout the entire volume. Contrary to the earlier claim, we demonstrate that the geometry of the magnetic fluctuations is two-dimensional. Rigid stripe arrays therefore appear to be ruled out over a wide range of doping levels in YBa2Cu3O6+x, but the data may be consistent with liquid-crystalline stripe order. The debate about stripes has therefore been reopened.The fundamental building block of the copper oxide superconductors is a Cu4O4 square plaquette. The plaquettes in most of these materials are slightly distorted to form a rectangular lattice, for which an influential theory predicts that high-transition-temperature (high-T(c)) superconductivity is nucleated in 'stripes' aligned along one of the axes. This theory received strong support from experiments that indicated a one-dimensional character for the magnetic excitations in the high-T(c) material YBa2Cu3O6.6 (ref. 4). Here we report neutron scattering data on 'untwinned' YBa2Cu3O6+x crystals, in which the orientation of the rectangular lattice is maintained throughout the entire volume. Contrary to the earlier claim, we demonstrate that the geometry of the magnetic fluctuations is two-dimensional. Rigid stripe arrays therefore appear to be ruled out over a wide range of doping levels in YBa2Cu3O6+x, but the data may be consistent with liquid-crystalline stripe order. The debate about stripes has therefore been reopened. The fundamental building block of the copper oxide superconductors is a Cu4O4 square plaquette. The plaquettes in most of these materials are slightly distorted to form a rectangular lattice, for which an influential theory predicts that high-transition-temperature (high-Tc) superconductivity is nucleated in 'stripes' aligned along one of the axes. This theory received strong support from experiments that indicated a one-dimensional character for the magnetic excitations in the high-Tc material YBa2Cu3O6.6 (ref. 4). Here we report neutron scattering data on 'untwinned' YBa2Cu3O6+x crystals, in which the orientation of the rectangular lattice is maintained throughout the entire volume. Contrary to the earlier claim, we demonstrate that the geometry of the magnetic fluctuations is two-dimensional. Rigid stripe arrays therefore appear to be ruled out over a wide range of doping levels in YBa2Cu3O6+x, but the data may be consistent with liquid-crystalline stripe order. The debate about stripes has therefore been reopened. [PUBLICATION ABSTRACT] |
| Audience | Academic |
| Author | Chen, D. P. Keimer, B. Sidis, Y. Bernhard, C. Bourges, P. Hinkov, V. Lin, C. T. Ivanov, A. Kulakov, A. Pailhès, S. |
| Author_xml | – sequence: 1 givenname: V. surname: Hinkov fullname: Hinkov, V. organization: Max-Planck-Institut für Festkörperforschung – sequence: 2 givenname: S. surname: Pailhès fullname: Pailhès, S. organization: Laboratoire Léon Brillouin, CEA-CNRS, CE-Saclay – sequence: 3 givenname: P. surname: Bourges fullname: Bourges, P. organization: Laboratoire Léon Brillouin, CEA-CNRS, CE-Saclay – sequence: 4 givenname: Y. surname: Sidis fullname: Sidis, Y. organization: Laboratoire Léon Brillouin, CEA-CNRS, CE-Saclay – sequence: 5 givenname: A. surname: Ivanov fullname: Ivanov, A. organization: Institut Laue-Langevin, 156X – sequence: 6 givenname: A. surname: Kulakov fullname: Kulakov, A. organization: Max-Planck-Institut für Festkörperforschung – sequence: 7 givenname: C. T. surname: Lin fullname: Lin, C. T. organization: Max-Planck-Institut für Festkörperforschung – sequence: 8 givenname: D. P. surname: Chen fullname: Chen, D. P. organization: Max-Planck-Institut für Festkörperforschung – sequence: 9 givenname: C. surname: Bernhard fullname: Bernhard, C. organization: Max-Planck-Institut für Festkörperforschung – sequence: 10 givenname: B. surname: Keimer fullname: Keimer, B. email: b.keimer@fkf.mpg.de organization: Max-Planck-Institut für Festkörperforschung |
| BackLink | https://www.ncbi.nlm.nih.gov/pubmed/15295593$$D View this record in MEDLINE/PubMed https://cea.hal.science/cea-03011770$$DView record in HAL |
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| CODEN | NATUAS |
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| ContentType | Journal Article |
| Copyright | Macmillan Magazines Ltd. 2004 COPYRIGHT 2004 Nature Publishing Group Copyright Macmillan Journals Ltd. Aug 5, 2004 Distributed under a Creative Commons Attribution 4.0 International License |
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| References | MF Limonov (BFnature02774_CR24) 2000; 61 SA Kivelson (BFnature02774_CR6) 2003; 75 CD Batista (BFnature02774_CR13) 2001; 64 BFnature02774_CR20 CJ Halboth (BFnature02774_CR22) 2000; 85 V Oganesyan (BFnature02774_CR23) 2001; 64 OK Andersen (BFnature02774_CR18) 1995; 56 CT Lin (BFnature02774_CR26) 1992; 195 B Grévin (BFnature02774_CR19) 2000; 85 F Krüger (BFnature02774_CR14) 2003; 67 C Stock (BFnature02774_CR12) 2004; 69 J Brinckmann (BFnature02774_CR16) 2001; 65 HA Mook (BFnature02774_CR7) 1998; 395 P Bourges (BFnature02774_CR10) 2000; 288 DH Lu (BFnature02774_CR25) 2001; 86 K Yamada (BFnature02774_CR8) 1998; 57 VI Voronkova (BFnature02774_CR27) 1993; 218 M Arai (BFnature02774_CR9) 1999; 83 HA Mook (BFnature02774_CR4) 2000; 404 BFnature02774_CR11 SA Kivelson (BFnature02774_CR5) 1998; 393 BFnature02774_CR15 JM Tranquada (BFnature02774_CR3) 1995; 375 J Zaanen (BFnature02774_CR1) 1989; 40 F Onufrieva (BFnature02774_CR17) 2002; 65 M Popovici (BFnature02774_CR28) 1975; A 31 VJ Emery (BFnature02774_CR2) 1993; 209 H Yamase (BFnature02774_CR21) 2000; 69 |
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| Snippet | The fundamental building block of the copper oxide superconductors is a Cu
4
O
4
square plaquette. The plaquettes in most of these materials are slightly... The fundamental building block of the copper oxide superconductors is a Cu4O4 square plaquette. The plaquettes in most of these materials are slightly... |
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| SubjectTerms | Condensed Matter Crystals Geometry High temperature superconductors Humanities and Social Sciences letter multidisciplinary Physics Science Science (multidisciplinary) Strongly Correlated Electrons Superconductivity |
| Title | Two-dimensional geometry of spin excitations in the high-transition-temperature superconductor YBa2Cu3O6+x |
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