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Impurity effects of hydrogen and deuterium in vanadium nanoconstrictions
by
Islam, M S
, Ueno, Y
, Kawae, T
, Takata, H
, Hashizume, K
, Inagaki, Y
in
Critical temperature
/ Deuterium
/ Energy gap
/ Impurities
/ Impurity effects
/ Low temperature
/ MCBJ
/ over-the-gap structure
/ Physics
/ sub-gap structure
/ Temperature dependence
/ Transition temperature
/ Vanadium
2018
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Impurity effects of hydrogen and deuterium in vanadium nanoconstrictions
by
Islam, M S
, Ueno, Y
, Kawae, T
, Takata, H
, Hashizume, K
, Inagaki, Y
in
Critical temperature
/ Deuterium
/ Energy gap
/ Impurities
/ Impurity effects
/ Low temperature
/ MCBJ
/ over-the-gap structure
/ Physics
/ sub-gap structure
/ Temperature dependence
/ Transition temperature
/ Vanadium
2018
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Do you wish to request the book?
Impurity effects of hydrogen and deuterium in vanadium nanoconstrictions
by
Islam, M S
, Ueno, Y
, Kawae, T
, Takata, H
, Hashizume, K
, Inagaki, Y
in
Critical temperature
/ Deuterium
/ Energy gap
/ Impurities
/ Impurity effects
/ Low temperature
/ MCBJ
/ over-the-gap structure
/ Physics
/ sub-gap structure
/ Temperature dependence
/ Transition temperature
/ Vanadium
2018
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Impurity effects of hydrogen and deuterium in vanadium nanoconstrictions
Journal Article
Impurity effects of hydrogen and deuterium in vanadium nanoconstrictions
2018
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Overview
To study non-magnetic and magnetic impurity effects at the superconductor-normal metal interfaces, we have measured the differential conductance dI/dV for Josephson contacts made by vanadium (V) nanoconstrictions with a different amount of hydrogen (H) and deuterium (D) impurities, which are prepared by a mechanically controllable break junction (MCBJ) technique at low temperature. Below the superconducting transition temperature TC, we have found distinct peaks within and outside the gap, known as the sub-gap structure and an over-the-gap structure respectively, due to 5% concentration of atomic H and D on V nanocontact. Moreover, the temperature dependence of dI/dV spectra represents that both structures are survived until the critical temperature TC, which is consistent with the prediction of BCS energy gap. On the other hand, a very high concentrating phase (30atom%) behaves as a normal metal.
Publisher
IOP Publishing
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