The density of Andreev levels in a normal metal (N) in contact with two superconductors (S) is known to exhibit an induced minigap related to the inverse dwell time. We predict a small secondary gap just below the superconducting gap edge—a feature that has been overlooked so far in numerous microscopic studies of the density of states in S?N?S structures. In a generic structure with N being a chaotic cavity, the secondary gap is the widest at zero phase bias. It closes at some finite phase bias, forming the shape of a “smile”. Asymmetric couplings give even richer gap structures near the phase difference ?. All the features found should be amendable to experimental detection in high-resolution low-temperature tunneling spectroscopy.QN/Quan...
Contains fulltext : 221474.pdf (publisher's version ) (Closed access
We argue that the spatial distribution of resonant impurity states in underdoped high-Tc superconduc...
Using scanning tunneling spectroscopy at $T = 4.2\,$K, we perform simultaneously the topographic ima...
The density of Andreev levels in a normal metal (N) in contact with two superconductors (S) is known...
The density of Andreev levels in a normal metal (N) in contact with two superconductors (S) is known...
The superconducting proximity effect leads to strong modifications of the local density of states in...
The energy levels of a quasicontinuous spectrum in mesoscopic systems fluctuate in positions and the...
We describe the proximity effect in a short disordered metallic junction between three superconducti...
We develop a theory of normal metal–superconductor and superconductor tunneling in “bosonic” superco...
The nature and behavior of electronic states in high temperature superconductors are the center of m...
The gap function $\Delta(\omega)$ carries essential information on both, the pairing glue as well as...
Using high-speed scanning tunneling spectroscopy (STS), we perform a full mapping of the quasipartic...
We have studied the gap instability in a superconductor under tunneling injection at high voltages b...
International audienceThe mysterious pseudo-gap (PG) phase of cuprate superconductors has been the s...
Quantum cavities or dots have markedly different properties depending on whether their classical cou...
Contains fulltext : 221474.pdf (publisher's version ) (Closed access
We argue that the spatial distribution of resonant impurity states in underdoped high-Tc superconduc...
Using scanning tunneling spectroscopy at $T = 4.2\,$K, we perform simultaneously the topographic ima...
The density of Andreev levels in a normal metal (N) in contact with two superconductors (S) is known...
The density of Andreev levels in a normal metal (N) in contact with two superconductors (S) is known...
The superconducting proximity effect leads to strong modifications of the local density of states in...
The energy levels of a quasicontinuous spectrum in mesoscopic systems fluctuate in positions and the...
We describe the proximity effect in a short disordered metallic junction between three superconducti...
We develop a theory of normal metal–superconductor and superconductor tunneling in “bosonic” superco...
The nature and behavior of electronic states in high temperature superconductors are the center of m...
The gap function $\Delta(\omega)$ carries essential information on both, the pairing glue as well as...
Using high-speed scanning tunneling spectroscopy (STS), we perform a full mapping of the quasipartic...
We have studied the gap instability in a superconductor under tunneling injection at high voltages b...
International audienceThe mysterious pseudo-gap (PG) phase of cuprate superconductors has been the s...
Quantum cavities or dots have markedly different properties depending on whether their classical cou...
Contains fulltext : 221474.pdf (publisher's version ) (Closed access
We argue that the spatial distribution of resonant impurity states in underdoped high-Tc superconduc...
Using scanning tunneling spectroscopy at $T = 4.2\,$K, we perform simultaneously the topographic ima...