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Supertransport by Superclimbing Dislocations in ^{4}He: When All Dimensions Matter
Anatoly B Kuklov1, Lode Pollet2,3,4, Nikolay V Prokof'ev5
1Department of Physics and Astronomy, College of Staten Island and the Graduate Center of CUNY, Staten Island, New York 10314, USA.
Superfluidity in solid helium-4 is uniquely suppressed by pressure and has an unusual temperature dependence. Thermal fluctuations of dislocations explain these phenomena, revealing a novel mechanism for critical flux behavior.
Area of Science:
- Condensed Matter Physics
- Quantum Fluids
Background:
- Solid helium-4 exhibits unique quantum phenomena, including quasi-one-dimensional superfluidity along dislocation cores.
- This superfluidity presents anomalous behaviors, such as pressure-dependent flow suppression and an unusual temperature dependence, contradicting existing theories like the Luttinger liquid paradigm.
Purpose of the Study:
- To investigate the underlying mechanisms responsible for the extraordinary features of the superflow-through-solid effect in solid helium-4.
- To explain the observed pressure suppression and temperature dependence of the superfluid flow rate.
Main Methods:
- The study employed ab initio and model simulations.
- Simulations focused on analyzing the impact of thermal fluctuations of dislocation shapes on the superfluid core.
Main Results:
- A strong correlation was found between thermal fluctuations of edge dislocations and asymmetric stress fields acting on the superfluid core.
- These stress fields were identified as the cause of the exponentially strong flow suppression with increasing pressure.
- The critical flux was shown to be highly sensitive to rare, strong fluctuations, leading to the observed sharp temperature dependence.
Conclusions:
- The anomalous superflow-through-solid effect in solid helium-4 is explained by thermal fluctuations of superclimbing edge dislocations.
- This provides a new understanding of critical flux behavior in quantum systems and challenges the standard Luttinger liquid model.
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