Wilson ratio: Difference between revisions
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The '''Wilson ratio''' of a metal is the dimensionless ratio of the zero-[[temperature]] [[magnetic susceptibility]] and the coefficient of the linear temperature term in the electronic [[specific heat]]. The relative—value of the Wilson ratio, compared to the Wilson ratio for the non-interacting Fermi-gas, can provide insight into the types of interactions present. |
The '''Wilson ratio''' of a metal is the dimensionless ratio of the zero-[[temperature]] [[magnetic susceptibility]] and the coefficient of the linear temperature term in the electronic [[specific heat]]. The relative—value of the Wilson ratio, compared to the Wilson ratio for the non-interacting Fermi-gas, can provide insight into the types of interactions present. |
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== Applications == |
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To give a specific example, it can be used to characterise [[strongly correlated]] [[Fermi liquids]].<ref>http://condensedconcepts.blogspot.in/2011/04/long-live-fermi-liquid-theory.html</ref> |
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=== Fermi liquid theory === |
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The Wilson ratio can be used to characterize [[Strongly correlated material|strongly correlated]] [[Fermi liquid]]s.<ref>Condensed Concepts (Blogspot) [http://condensedconcepts.blogspot.in/2011/04/long-live-fermi-liquid-theory.html ''Long live Fermi liquid theory] Retrieved March 2015</ref> The [[Fermi liquid theory]] explains the behaviour of metals at very low temperatures. Two important features of a metal which obey this theory are: |
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⚫ | Both of these quantities, however, are proportional to the electronic density of states at Fermi energy. Their ratio is a dimensionless quantity called the Wilson (or the Sommerfeld - Wilson) Ratio,<ref>Condensed Concepts (Blogspot) [http://condensedconcepts.blogspot.in/2012/12/wilsons-ratio-for-strongly-correlated.html Wilson's ratio for strongly correlated electrons] Retrieved March 2015</ref> defined as: |
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The [[Fermi Liquid Theory]] is a theory explaining the behaviour of metals at very low temperatures. Two important features of a metal which obeys this theory are: |
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<ref>http://condensedconcepts.blogspot.in/2012/12/wilsons-ratio-for-strongly-correlated.html</ref> |
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⚫ | In the case of real Fermi-liquid metals, the ratio can differ significantly from 1. The difference arises due to electron - electron interactions within the system. These tend to change the effective electronic mass, which affects both [[specific heat]] and magnetic susceptibility. Whether or not this increase in both is given by the same multiplicative factor is shown by the Wilson ratio. In some cases, electron - electron interactions give rise to an additional increase in susceptibility. |
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However, the Wilson ratio for real Fermi-liquid metals can differ substantially from 1. (In this regard,even cases like R<sub>w</sub> = 2 are already substantially different from unity). |
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<ref>Fundamentals of the Physics of Solids - Volume 2 by Jenö Sólyom</ref> |
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==See also== |
==See also== |
Revision as of 21:34, 16 March 2015
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The Wilson ratio of a metal is the dimensionless ratio of the zero-temperature magnetic susceptibility and the coefficient of the linear temperature term in the electronic specific heat. The relative—value of the Wilson ratio, compared to the Wilson ratio for the non-interacting Fermi-gas, can provide insight into the types of interactions present.
Applications
Fermi liquid theory
The Wilson ratio can be used to characterize strongly correlated Fermi liquids.[1] The Fermi liquid theory explains the behaviour of metals at very low temperatures. Two important features of a metal which obey this theory are:
- At temperatures much below the Fermi temperature the specific heat is proportional to the temperature
- The magnetic susceptibility is independent of temperature
Both of these quantities, however, are proportional to the electronic density of states at Fermi energy. Their ratio is a dimensionless quantity called the Wilson (or the Sommerfeld - Wilson) Ratio,[2] defined as:
Rw = 4π2kB2Tχp/3μ0(geμB)2Celec
After substituting the values of χp (Pauli susceptibility) and Celec (electronic contribution to specific heat), obtained using Sommerfeld theory, the value obtained for Rw in the case of a free electron gas is 1.
In the case of real Fermi-liquid metals, the ratio can differ significantly from 1. The difference arises due to electron - electron interactions within the system. These tend to change the effective electronic mass, which affects both specific heat and magnetic susceptibility. Whether or not this increase in both is given by the same multiplicative factor is shown by the Wilson ratio. In some cases, electron - electron interactions give rise to an additional increase in susceptibility.
The converse is also true, i.e. a deviation of experimental value of Rw from 1 indicates strong electronic correlations.[3]
See also
References
- ^ Condensed Concepts (Blogspot) Long live Fermi liquid theory Retrieved March 2015
- ^ Condensed Concepts (Blogspot) Wilson's ratio for strongly correlated electrons Retrieved March 2015
- ^ Fundamentals of the Physics of Solids - Volume 2 by Jenö Sólyom