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Glassy properties of the Bose-glass phase of a one-dimensional disordered Bose fluid

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 نشر من قبل Nicolas Dupuis
 تاريخ النشر 2019
  مجال البحث فيزياء
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 تأليف Nicolas Dupuis




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We study a one-dimensional disordered Bose fluid using bosonization, the replica method and a nonperturbative functional renormalization-group approach. The Bose-glass phase is described by a fully attractive strong-disorder fixed point characterized by a singular disorder correlator whose functional dependence assumes a cuspy form that is related to the existence of metastable states. At nonzero momentum scale, quantum tunneling between these metastable states leads to a rounding of the nonanalyticity in a quantum boundary layer that encodes the existence of rare superfluid regions responsible for the $omega^2$ behavior of the (dissipative) conductivity in the low-frequency limit. These results can be understood within the droplet picture put forward for the description of glassy (classical) systems.



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We study a one-dimensional disordered Bose fluid using bosonization, the replica method and a nonperturbative functional renormalization-group approach. We find that the Bose-glass phase is described by a fully attractive strong-disorder fixed point characterized by a singular disorder correlator whose functional dependence assumes a cuspy form that is related to the existence of metastable states. At nonzero momentum scale $k$, quantum tunneling between the ground state and low-lying metastable states leads to a rounding of the cusp singularity into a quantum boundary layer (QBL). The width of the QBL depends on an effective Luttinger parameter $K_ksim k^theta$ that vanishes with an exponent $theta=z-1$ related to the dynamical critical exponent $z$. The QBL encodes the existence of rare superfluid regions, controls the low-energy dynamics and yields a (dissipative) conductivity vanishing as $omega^2$ in the low-frequency limit. These results reveal the glassy properties (pinning, shocks or static avalanches) of the Bose-glass phase and can be understood within the droplet picture put forward for the description of glassy (classical) systems.
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