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Volumn 89, Issue 5, 2014, Pages

Diamond magnetometry of superconducting thin films

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EID: 84897662948     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.89.054509     Document Type: Article
Times cited : (51)

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    • To be precise,above a layer with a thickness d,the field does not decay exponentially,but rather falls off as 1/(z + λ eff) 2 as mentioned by A. APPLAB 0003-6951 10.1063/1.108334
    • To be precise,above a layer with a thickness d,the field does not decay exponentially,but rather falls off as 1/(z + λ eff) 2 as mentioned by A. M. Chang, H. D. Hallen, L. Harriott, H. F. Hess, H. L. Kao, J. Kwo, R. E. Miller, R. Wolfe, J. van der Ziel, and T. Y. Chang, Appl. Phys. Lett. 61, 1974 (1992). APPLAB 0003-6951 10.1063/1.108334
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    • Here, λ eff = λ coth [λ/2 d] is the effective penetration depth. However, close to the surface (0 < z < 1 μ m) which is the case discussed here, the exponential approximation is good enough.
    • Here, λ eff = λ coth [λ/2 d] is the effective penetration depth. However, close to the surface (0 < z < 1 μ m) which is the case discussed here, the exponential approximation is good enough.


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