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In [[superconductivity]], '''Homes's law''' is an empirical relation that states that a superconductor's
In [[superconductivity]], '''Homes's law''' is an empirical relation that states that a superconductor's
[[critical temperature]] (''T''<sub>c</sub>) is [[Proportionality (mathematics)|proportional]] to the strength of the superconducting state for temperatues well below ''T''<sub>c</sub> close to [[zero temperature]](that is, the fully formed [[superfluid density]], <math>\rho_{s0}</math>) multiplied by the [[electrical resistivity]] <math>\rho_{dc}</math> measured just above the critical temperature. The relation follows the form,
[[critical temperature]] (''T''<sub>c</sub>) is [[Proportionality (mathematics)|proportional]] to the strength of the superconducting state for temperatures well below ''T''<sub>c</sub> close to [[zero temperature]] (also referred to as the fully-formed [[superfluid density]], <math>\rho_{s0}</math>) multiplied by the [[electrical resistivity]] <math>\rho_{dc}</math> measured just above the critical temperature. In cuprate high-temperature superconductors the relation follows the form


<math> \rho_{dc}^\alpha\,\rho_{s0}^\alpha/8 \simeq 4.4\,T_c </math>.


<math> \rho_{dc}^\alpha\,\rho_{s0}^\alpha/8 \simeq 4.4\,T_c </math> ,
The superscript is to recognize that may novel superconductors are anisotropic, so that the resistivity

and the superfluid density are tensor quantities; the superscript <math>\alpha</math> denotes the

crystallographic direction along which these quantities are measured.
or alternatively


<math>\rho_{s0}^\alpha \simeq 4.1\,\sigma_{dc}^\alpha\, T_c</math>.


Many novel superconductors are anisotropic, so the resistivity and the superfluid density are
tensor quantities; the superscript <math>\alpha</math> denotes the crystallographic direction
along which these quantities are measured.
Note that this expression assumes that the conductivity and temperature have both been recast in units
of cm<sup>-1</sup> (or s<sup>-1</sup>), and that the superfluid density has units of cm<sup>-2</sup>
(or s<sup>-2</sup>); the constant is dimensionless. The expected form for a BCS dirty-limit superconductor
has slightly larger numerical constant of ~8.1.


The law is named for [[physics|physicist]] [[Christopher Homes]] and was first presented in the July 29, 2004 edition of [[Nature (journal)|Nature]],<ref>{{cite journal|author = C. C. Homes ''et al.''|title = A universal scaling relation in high-temperature superconductors| journal = Nature (London)| volume = 430| pages = 539-541| year = 2004| url = http://www.nature.com/nature/journal/v430/n6999/full/nature02673.html| doi = 10.1038/nature02673}}</ref> and was the subject of a News and Views article by Jan Zaanen in the same issue<ref>{{cite journal|author = J. Zaanen| title = Superconductivity: Why the temperature is high| journal = Nature (London)|volume = 430| pages = 512-513| year = 2004 | url = http://www.nature.com/nature/journal/v430/n6999/full/430512a.html | doi = 10.1038/430512a }}</ref> in which he speculated that the high transition temperatures observed in the
The law is named for [[physics|physicist]] [[Christopher Homes]] and was first presented in the July 29, 2004 edition of [[Nature (journal)|Nature]],<ref>{{cite journal|author = C. C. Homes ''et al.''|title = A universal scaling relation in high-temperature superconductors| journal = Nature (London)| volume = 430| pages = 539-541| year = 2004| url = http://www.nature.com/nature/journal/v430/n6999/full/nature02673.html| doi = 10.1038/nature02673}}</ref> and was the subject of a News and Views article by Jan Zaanen in the same issue<ref>{{cite journal|author = J. Zaanen| title = Superconductivity: Why the temperature is high| journal = Nature (London)|volume = 430| pages = 512-513| year = 2004 | url = http://www.nature.com/nature/journal/v430/n6999/full/430512a.html | doi = 10.1038/430512a }}</ref> in which he speculated that the high transition temperatures observed in the
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[[Physical Review B]] in 2005.<ref>{{cite journal|author = C. C. Homes, S. V. Dordevic, T. Valla and M. Strongin|title = Scaling of the superfluid density in high-temperature superconductors|journal = Phys. Rev. B|volume = 72|pages = 134517|year = 2005|url = http://link.aps.org/doi/10.1103/PhysRevB.72.134517|doi = 10.1103/PhysRevB.72.134517}}</ref>
[[Physical Review B]] in 2005.<ref>{{cite journal|author = C. C. Homes, S. V. Dordevic, T. Valla and M. Strongin|title = Scaling of the superfluid density in high-temperature superconductors|journal = Phys. Rev. B|volume = 72|pages = 134517|year = 2005|url = http://link.aps.org/doi/10.1103/PhysRevB.72.134517|doi = 10.1103/PhysRevB.72.134517}}</ref>


[[Francis Pratt]] and [[Stephen Blundell]] have argued that '''Homes's law''' is violated in the [[organic superconductor]]s. This work was first presented in [[Physical Review Letters]] in March 2005.

[[Francis Pratt]] and [[Stephen Blundell]] have shown that '''Homes's law''' is violated in the [[organic superconductor]]s. This work was first presented in [[Physical Review Letters]] in March 2005.


==See also==
==See also==
* [[Uemura's law]]
* [[Uemura relation]]
* [[Tanner's law]]
* [[Tanner's law]]



Revision as of 18:40, 17 January 2010

In superconductivity, Homes's law is an empirical relation that states that a superconductor's critical temperature (Tc) is proportional to the strength of the superconducting state for temperatures well below Tc close to zero temperature (also referred to as the fully-formed superfluid density, ) multiplied by the electrical resistivity measured just above the critical temperature. In cuprate high-temperature superconductors the relation follows the form


,


or alternatively


.


Many novel superconductors are anisotropic, so the resistivity and the superfluid density are tensor quantities; the superscript denotes the crystallographic direction along which these quantities are measured. Note that this expression assumes that the conductivity and temperature have both been recast in units of cm-1 (or s-1), and that the superfluid density has units of cm-2 (or s-2); the constant is dimensionless. The expected form for a BCS dirty-limit superconductor has slightly larger numerical constant of ~8.1.

The law is named for physicist Christopher Homes and was first presented in the July 29, 2004 edition of Nature,[1] and was the subject of a News and Views article by Jan Zaanen in the same issue[2] in which he speculated that the high transition temperatures observed in the cuprate superconductors are due to the fact that the metallic states in these materials are as viscous as permitted by the laws of quantum physics. A more detailed version of this scaling relation subsequently appeared in Physical Review B in 2005.[3]

Francis Pratt and Stephen Blundell have argued that Homes's law is violated in the organic superconductors. This work was first presented in Physical Review Letters in March 2005.

See also

References

  1. ^ C. C. Homes; et al. (2004). "A universal scaling relation in high-temperature superconductors". Nature (London). 430: 539–541. doi:10.1038/nature02673. {{cite journal}}: Explicit use of et al. in: |author= (help)
  2. ^ J. Zaanen (2004). "Superconductivity: Why the temperature is high". Nature (London). 430: 512–513. doi:10.1038/430512a.
  3. ^ C. C. Homes, S. V. Dordevic, T. Valla and M. Strongin (2005). "Scaling of the superfluid density in high-temperature superconductors". Phys. Rev. B. 72: 134517. doi:10.1103/PhysRevB.72.134517.{{cite journal}}: CS1 maint: multiple names: authors list (link)