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Quantum contributions to the magnetoconductivity of critically disordered superconducting TiN films. / Mironov, A. Yu; Postolova, S. V.; Baturina, T. I.
In: Journal of Physics Condensed Matter, Vol. 30, No. 48, 485601, 12.11.2018, p. 485601.Research output: Contribution to journal › Article › peer-review
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TY - JOUR
T1 - Quantum contributions to the magnetoconductivity of critically disordered superconducting TiN films
AU - Mironov, A. Yu
AU - Postolova, S. V.
AU - Baturina, T. I.
PY - 2018/11/12
Y1 - 2018/11/12
N2 - The onset of superconductivity in the presence of disorder is a fundamental problem of condensed matter physics. Here we investigate the magnetoconductance of disordered (8 > kFl > 1.8) superconducting TiN films above the critical temperature Tc. We show that the magnetoconductivity of moderately disordered films with kFl > 5 is in full agreement with the perturbative theory of quantum contributions to conductivity. We demonstrate that the magnetoconductivity of films with kFl ≲ 5 is also in agreement with the perturbative theory down to temperatures T ≈ 2Tc . The quantitative discrepancy between experiment and theory develops only below temperatures T - 2Tc for films with kFl ≈ 5. This discrepancy can be eliminated if we assume steeper temperature dependence of the Larkin's electron'electron attraction strength, Β(T/Tc). The obtained temperature dependence of electron phase breaking time τ (T/Tc) is in agreement with theoretical predictions for all samples.
AB - The onset of superconductivity in the presence of disorder is a fundamental problem of condensed matter physics. Here we investigate the magnetoconductance of disordered (8 > kFl > 1.8) superconducting TiN films above the critical temperature Tc. We show that the magnetoconductivity of moderately disordered films with kFl > 5 is in full agreement with the perturbative theory of quantum contributions to conductivity. We demonstrate that the magnetoconductivity of films with kFl ≲ 5 is also in agreement with the perturbative theory down to temperatures T ≈ 2Tc . The quantitative discrepancy between experiment and theory develops only below temperatures T - 2Tc for films with kFl ≈ 5. This discrepancy can be eliminated if we assume steeper temperature dependence of the Larkin's electron'electron attraction strength, Β(T/Tc). The obtained temperature dependence of electron phase breaking time τ (T/Tc) is in agreement with theoretical predictions for all samples.
KW - quantum corrections to conductivity
KW - superconductor-insulator transition
KW - two-dimensional superconductor
KW - INELASTIC-SCATTERING
KW - ALUMINUM FILMS
KW - DEPENDENCE
KW - FLUCTUATION
KW - TRANSITION
KW - TRANSPORT
KW - WEAK-LOCALIZATION
KW - TEMPERATURE
KW - RESISTANCE
KW - PARAMETER
UR - http://www.scopus.com/inward/record.url?scp=85056502987&partnerID=8YFLogxK
U2 - 10.1088/1361-648X/aae870
DO - 10.1088/1361-648X/aae870
M3 - Article
C2 - 30418946
AN - SCOPUS:85056502987
VL - 30
SP - 485601
JO - Journal of Physics Condensed Matter
JF - Journal of Physics Condensed Matter
SN - 0953-8984
IS - 48
M1 - 485601
ER -
ID: 17472868