We present a phase diagram as a function of disorder in three-dimensional NbN thin films as the system enters the critical disorder for destruction of the superconducting state. The superconducting state is investigated using a combination of magnetotransport and scanning tunneling spectroscopy measurements. Our studies reveal three disorder regimes. At low disorder (kF l similar to 10-4), the system follows the mean field Bardeen-Cooper-Schrieffer behavior, where the superconducting energy gap vanishes at the temperature at which electrical resistance appears. For stronger disorder (1 < k(F)l < 4), a ``pseudogap'' state emerges, where a gap in the electronic spectrum persists up to temperatures much higher than T-c, suggesting that Cooper pairs continue to exist in the system even after the zero resistance state is destroyed. Finally, at even stronger disorder (k(F)l < 1), the global superconducting ground state is destroyed even though superconducting correlations continue to survive, as evidenced from a pronounced magnetoresistance peak at low temperatures.
Phase diagram of the strongly disordered s-wave superconductor NbN close to the metal-insulator transition / Chand, Madhavi; Saraswat, Garima; Kamlapure, Anand; Mondal, Mintu; Kumar, Sanjeev; Jesudasan, John; Bagwe, Vivas; Benfatto, Lara; Tripathi, Vikram; Raychaudhuri, Pratap. - In: PHYSICAL REVIEW. B, CONDENSED MATTER AND MATERIALS PHYSICS. - ISSN 1098-0121. - 85:1(2012). [10.1103/PhysRevB.85.014508]
Phase diagram of the strongly disordered s-wave superconductor NbN close to the metal-insulator transition
Benfatto Lara;Raychaudhuri Pratap
2012
Abstract
We present a phase diagram as a function of disorder in three-dimensional NbN thin films as the system enters the critical disorder for destruction of the superconducting state. The superconducting state is investigated using a combination of magnetotransport and scanning tunneling spectroscopy measurements. Our studies reveal three disorder regimes. At low disorder (kF l similar to 10-4), the system follows the mean field Bardeen-Cooper-Schrieffer behavior, where the superconducting energy gap vanishes at the temperature at which electrical resistance appears. For stronger disorder (1 < k(F)l < 4), a ``pseudogap'' state emerges, where a gap in the electronic spectrum persists up to temperatures much higher than T-c, suggesting that Cooper pairs continue to exist in the system even after the zero resistance state is destroyed. Finally, at even stronger disorder (k(F)l < 1), the global superconducting ground state is destroyed even though superconducting correlations continue to survive, as evidenced from a pronounced magnetoresistance peak at low temperatures.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.