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Figure 1
Schematic representation of the quasiparticle density of states for the normal-conducting material (nn, horizontal broken line) and for the superconducting material (ns, full line) close to the Fermi energy EF. The broken curve represents a Lorentzian broadening function.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 12| Part 2| February 2005| Pages 251-253
doi:10.1107/S0909049504028936
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