Nature of the Cooper-pair insulator beyond the transition · revision history

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Title
Nature of the Cooper-pair insulator beyond the transition
Plain
On the insulating side, some films such as amorphous indium oxide and titanium nitride show a giant resistance peak in a magnetic field and signs that electrons are still bound in pairs. How paired electrons form an insulator, and what sets its conduction, is open.
Precise
In amorphous InOx, TiN and nanopatterned Bi films on the insulating side of the field-tuned transition, $\rho \sim \operatorname{exp}(T_{0}/T)$ with $T_{0}$ peaking at a field $B_{\mathrm{peak}}$, the magnetoresistance peak spans several orders of magnitude, and patterned films show $h/2e$ periodic magnetoresistance (Stewart et al. 2007). Explain the pair-localization mechanism and $T_{0}(B)$, and determine whether abrupt current jumps in the $I-V$ curves reflect electron overheating (Altshuler, Kravtsov, Lerner and Aleiner 2009) or a distinct phase (proposed superinsulator).
Settled by
Electron-temperature measurement during nonlinear transport plus local probes of pair density in the insulator, compared with a theory of localized preformed pairs.
Kind
phenomenon
Answer type
mechanism
References
(empty)
Literature status
contested
Status note
(empty)
Posed since
(empty)