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Published on: December 4, 2017
Mott-Glass Phase of a One-Dimensional Quantum Fluid with Long-Range Interactions
Romain Daviet1, Nicolas Dupuis1
1Sorbonne Université, CNRS, Laboratoire de Physique Théorique de la Matière Condensée, LPTMC, F-75005 Paris, France.
Disorder suppresses Wigner crystallization in quantum particles with repulsive potentials between -3/2 and 0. Above this range, particles form a Wigner crystal, but below it, they transition to a Mott glass state.
Area of Science:
- Condensed matter physics
- Quantum mechanics
- Many-body systems
Background:
- Quantum particles with long-range potentials exhibit complex ground-state phases.
- The transition from Coulombic to linear confinement potentials is crucial for understanding these phases.
- Disorder's role in these quantum systems is a key area of investigation.
Purpose of the Study:
- Investigate ground-state properties of quantum particles with tunable long-range potentials.
- Determine the impact of disorder on the Wigner crystal phase.
- Characterize the emergent phases, such as the Mott glass.
Main Methods:
- Bosonization techniques to map fermionic systems to bosonic ones.
- Nonperturbative functional renormalization group (FRG) for analyzing interacting quantum systems.
- Analysis of ground-state properties including compressibility and conductivity.
Main Results:
- In the absence of disorder, a Wigner crystal forms for potentials with σ ≤ 0.
- Disorder suppresses Wigner crystallization for -3/2 < σ ≤ 0, leading to a Mott glass.
- For σ < -3/2, the Wigner crystal state persists even with disorder.
Conclusions:
- Disorder plays a critical role in determining the ground state of quantum particles with long-range interactions.
- The study identifies a transition from Wigner crystal to Mott glass phases driven by disorder.
- The findings provide insights into quantum phase transitions in disordered systems.
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