dorsal/arxiv
View SchemaSuperfluid Density, Penetration Depth, Condensate Density
| Authors | Warren E. Pickett |
|---|---|
| Categories | |
| ArXiv ID | 2601.10578vv1 |
| URL | https://arxiv.org/abs/2601.10578 |
| License | http://creativecommons.org/licenses/by/4.0/ |
Abstract
Fascination with the concept of superconducting (SC) {\it superfluid density} $\rho_s$ has persisted since the beginning of superconductivity theory, with numerical values of an actual density rarely provided. Over time $\rho_s$, addressed mostly in cuprate and following high temperature superconductors, has become synonymous with the normalized (unitless) inverse square of the magnetic penetration depth $\lambda_L$ (the London expression, with superfluid density denoted $n_s$), with interest primarily on its temperature $T$ dependence that is expected to reflect the T-dependence of the SC gap amplitude and gap symmetry. In conventional superconductors, generalized expressions from the London penetration depth via Ginzburg-Landau theory, then to BCS theory provide updated pictures of the supercurrent density-vector potential relationship. The BCS value $\lambda_{band}$ is distinct from any particle density, instead involving particle availability at the Fermi surface and Fermi velocity as the determining factors, thus providing a basis for a more fundamental theory and understanding of what is being probed in penetration depth studies. The number density of superconducting electrons ${\cal N}_s(T$=0) -- the scalar SC {\it condensate density} -- is provided, first from a phenomenological estimate but then supported by BCS theory. A straightforward relation connecting ${\cal N}_s(0)$ to the density of dynamically transporting carriers in the normal state at $T_c$ is obtained. Numerical values of relevant material parameters including $\lambda_{band}$ and ${\cal N}_s$ are provided for a few conventional SCs.
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"abstract": "Fascination with the concept of superconducting (SC) {\\it superfluid density} $\\rho_s$ has persisted since the beginning of superconductivity theory, with numerical values of an actual density rarely provided. Over time $\\rho_s$, addressed mostly in cuprate and following high temperature superconductors, has become synonymous with the normalized (unitless) inverse square of the magnetic penetration depth $\\lambda_L$ (the London expression, with superfluid density denoted $n_s$), with interest primarily on its temperature $T$ dependence that is expected to reflect the T-dependence of the SC gap amplitude and gap symmetry. In conventional superconductors, generalized expressions from the London penetration depth via Ginzburg-Landau theory, then to BCS theory provide updated pictures of the supercurrent density-vector potential relationship. The BCS value $\\lambda_{band}$ is distinct from any particle density, instead involving particle availability at the Fermi surface and Fermi velocity as the determining factors, thus providing a basis for a more fundamental theory and understanding of what is being probed in penetration depth studies. The number density of superconducting electrons ${\\cal N}_s(T$=0) -- the scalar SC {\\it condensate density} -- is provided, first from a phenomenological estimate but then supported by BCS theory. A straightforward relation connecting ${\\cal N}_s(0)$ to the density of dynamically transporting carriers in the normal state at $T_c$ is obtained. Numerical values of relevant material parameters including $\\lambda_{band}$ and ${\\cal N}_s$ are provided for a few conventional SCs.",
"arxiv_id": "2601.10578",
"authors": [
"Warren E. Pickett"
],
"categories": [
"cond-mat.supr-con"
],
"license": "http://creativecommons.org/licenses/by/4.0/",
"title": "Superfluid Density, Penetration Depth, Condensate Density",
"url": "https://arxiv.org/abs/2601.10578",
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