TY - JOUR
T1 - Phase Glass is a Bose Metal
T2 - A New Conducting State in Two Dimensions
AU - Dalidovich, Denis
AU - Phillips, Philip
PY - 2002
Y1 - 2002
N2 - In the quantum rotor model with random exchange interactions having a nonzero mean, three phases, a (i) phase (Bose) glass, (ii) superfluid, and (iii) Mott insulator, meet at a bicritical point. We demonstrate that proximity to the bicritical point and the coupling between the energy landscape and the dissipative degrees of freedom of the phase glass lead to a metallic state at [Formula presented]. Consequently, the phase glass is unique in that it represents a concrete example of a metallic state that is mediated by disorder, even in 2D. We propose that the experimentally observed metallic phase which intervenes between the insulator and the superconductor in a wide range of thin films is in actuality a phase glass.
AB - In the quantum rotor model with random exchange interactions having a nonzero mean, three phases, a (i) phase (Bose) glass, (ii) superfluid, and (iii) Mott insulator, meet at a bicritical point. We demonstrate that proximity to the bicritical point and the coupling between the energy landscape and the dissipative degrees of freedom of the phase glass lead to a metallic state at [Formula presented]. Consequently, the phase glass is unique in that it represents a concrete example of a metallic state that is mediated by disorder, even in 2D. We propose that the experimentally observed metallic phase which intervenes between the insulator and the superconductor in a wide range of thin films is in actuality a phase glass.
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U2 - 10.1103/PhysRevLett.89.027001
DO - 10.1103/PhysRevLett.89.027001
M3 - Article
AN - SCOPUS:0037042999
SN - 0031-9007
VL - 89
JO - Physical review letters
JF - Physical review letters
IS - 2
ER -