ass5: Draft essay 18
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@ -124,8 +124,23 @@ This leads to our final maximum
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For larger $T_c$ values, larger binding of Cooper pairs would be needed to overcome the thermal energy.
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For larger $T_c$ values, larger binding of Cooper pairs would be needed to overcome the thermal energy.
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This means our assumption of weak coupling breaks down, making most of the derivation invalid without further arguments.
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This means our assumption of weak coupling breaks down, making most of the derivation invalid without further arguments.
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\section{Energy gap $\Delta$ et al.}
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\clearpage
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\section{Penetration depth $\lambda$ and measuring it}
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There are many species of superconductors.
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Conventional superconductors we can describe using BCS theory or some extension of it.
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Others we do not yet have a theory for.
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Some are type-I, others type-II.
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What they do have in common, is that they can be characterized by some key quantities.
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Starting with the coherence length $\xi$ and the penetration depth $ \lambda$, we also have their critical temperatures $T_c$ and can relate them to the energy band gap around the Fermi surface in BCS theory.
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In this essay, we will take a look at what the penetration depth can tell us about the superconducting energy gap, and will go into measuring the penetration depth.
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In the weak coupling limit of BCS theory, the coherence length can be related to the gap parameter\cite[chapter 9]{waldram} as
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\[
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\xi_{BCS} = \frac{\hbar v_F}{\pi\Delta},
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\]
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for $v_F$ the Fermi velocity.
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Furthermore, it has the physical interpretation of the size of the separation in a Cooper pair\cite[p. 62]{annett}.
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\bibliographystyle{vancouver}
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\bibliographystyle{vancouver}
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\bibliography{references.bib}
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\bibliography{references.bib}
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