TY - JOUR
T1 - Coherence gap edge and pseudo-gap in cuprates and other non-BCS superconductors
AU - Deutscher, Guy
N1 - Publisher Copyright:
© 2023
PY - 2023/11/15
Y1 - 2023/11/15
N2 - The energy gap Δ, proportional to the critical temperature, is the unique energy scale that characterizes the superconducting state in BCS theory. It is the single particle excitation energy Δp seen by tunneling experiments as well as the coherence gap edge Δc, up to which electron-hole reflections take place at clean superconducting/normal (S/N) interfaces, seen by point contacts. Both scales go to zero at the critical temperature Tc. These BCS predictions are well verified in conventional superconducting metals and alloys. But we show that they are violated in a variety of new superconductors such as the High Tc cuprates, granular Aluminum and other quasi two-dimensional compounds such as intercalated nitrides. In this new class of superconductors Δp is not anymore proportional to the critical temperature, while Δc is. Δp persists above Tc, Δc does not. Spectroscopic maps show that at energies larger than Δc the superconducting state becomes inhomogeneous, breaking up into nano-scale regions having different values of Δp. Coherence is lost, which explains why non-local electron-hole reflections are quenched.
AB - The energy gap Δ, proportional to the critical temperature, is the unique energy scale that characterizes the superconducting state in BCS theory. It is the single particle excitation energy Δp seen by tunneling experiments as well as the coherence gap edge Δc, up to which electron-hole reflections take place at clean superconducting/normal (S/N) interfaces, seen by point contacts. Both scales go to zero at the critical temperature Tc. These BCS predictions are well verified in conventional superconducting metals and alloys. But we show that they are violated in a variety of new superconductors such as the High Tc cuprates, granular Aluminum and other quasi two-dimensional compounds such as intercalated nitrides. In this new class of superconductors Δp is not anymore proportional to the critical temperature, while Δc is. Δp persists above Tc, Δc does not. Spectroscopic maps show that at energies larger than Δc the superconducting state becomes inhomogeneous, breaking up into nano-scale regions having different values of Δp. Coherence is lost, which explains why non-local electron-hole reflections are quenched.
KW - Energy gap
KW - Point contact
KW - Pseudo-gap
KW - Superfluid coherence
KW - Tunneling
UR - http://www.scopus.com/inward/record.url?scp=85172918637&partnerID=8YFLogxK
U2 - 10.1016/j.physc.2023.1354323
DO - 10.1016/j.physc.2023.1354323
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AN - SCOPUS:85172918637
SN - 0921-4534
VL - 614
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
M1 - 1354323
ER -