Quantum fluctuations in hydrodynamics and quantum long-time tails
summary
The gist
Quantum corrections within an effective field theory framework reveal that fluctuation-dissipation relations mandate intrinsically non-Gaussian noise, leading to a quantum generalization of
In short
The study develops a quantum effective field theory for diffusive hydrodynamics using Schwinger-Keldysh formalism and KMS symmetry to incorporate fluctuation-dissipation theorems at finite temperature and quantum levels. This leads to intrinsically non-Gaussian noise, resulting in a quantum generalization of hydrodynamic long-time tails characterized by specific non-analytic corrections.
Key concepts
- Schwinger-Keldysh (SK) Effective Field Theory
- This framework uses a closed time contour to systematically include quantum corrections in the description of diffusive hydrodynamics. It is built upon the SK formalism, which is essential for computing correlation functions at finite temperatures while maintaining consistency with quantum fluctuation-dissipation theorems.
- KMS Symmetry
- Dynamical Kubo-Martin-Schwinger symmetry enforces the fluctuation-dissipation theorem at the full non-linear level. It acts on fields with a relative phase shift in imaginary time, ensuring that quantum effects correctly relate stochastic fluctuations to dissipation in the system.
- Hydrodynamic Long-Time Tails
- These are specific features of correlation functions in diffusive systems that describe their behavior at very long times. The paper shows that quantum corrections modify these tails, leading to a non-analytic branch cut starting at a specific frequency point, indicating fundamentally different long-time dynamics.
- Non-Gaussian Noise
- The KMS symmetry necessarily generates fluctuation contributions in the effective action at all orders in the noise field. This means the resulting noise is not simple Gaussian noise but possesses complex, non-linear characteristics derived from quantum constraints.
Terminology used across episodes
This episode discusses
- Quantum fluctuations in hydrodynamics and quantum long-time tails · Paper Radio
- Viscosity and dissipative hydrodynamics from effective field theory
- On thermal fluctuations and the generating functional in relativistic hydrodynamics
- Effective field theory of dissipative fluids
- Topological sigma models & dissipative hydrodynamics
- Effective Action for Relativistic Hydrodynamics: Fluctuations, Dissipation, and Entropy Inflow
- Dissipative hydrodynamics in superspace
- Schwinger-Keldysh effective field theory for stable and causal relativistic hydrodynamics
- Lectures on hydrodynamic fluctuations in relativistic theories
- Theory of diffusive fluctuations
- Non-universality of hydrodynamics
- Lectures on non-equilibrium effective field theories and fluctuating hydrodynamics
- Schwinger-Keldysh formalism I: BRST symmetries and superspace
- Ghostbusters: Unitarity and Causality of Non-equilibrium Effective Field Theories
- Effective field theory for non-relativistic hydrodynamics
- Effective field theory for hydrodynamics without boosts
- Holographic Schwinger-Keldysh effective field theories
- A prescription for holographic Schwinger-Keldysh contour in non-equilibrium systems
- Emergent Supersymmetry in Local Equilibrium Systems
- A panoply of Schwinger-Keldysh transport
The paper
Quantum fluctuations in hydrodynamics and quantum long-time tails · Read on arXiv
Akash Jain
Mathematical Institute, University of Oxford
We construct a quantum Schwinger-Keldysh (SK) effective field theory for the diffusive hydrodynamics of a conserved scalar field. Quantum corrections within the SK framework are guided by fluctuation-dissipation relations, enforced via a dynamical Kubo-Martin-Schwinger (KMS) symmetry. We find that the KMS symmetry necessarily generates fluctuation contributions in the SK effective action at all orders in the noise field, thereby giving rise to intrinsically non-Gaussian noise. We use our results to compute one-loop quantum corrections to the two-point density-density retarded correlation function, leading to a quantum generalization of hydrodynamic long-time tails. Our results apply at arbitrarily high orders in. The one-loop results for retarded correlation functions have been expressed in terms of a family of polynomials. We also provide a closed-form expression for the one-loop results at leading order in the wavevector expansion.
DOI: 10.21468/SciPostPhys.21.4.083
Transcript
Introduction to the show: ident: Quantum Radio. Generated commentary on the latest quantum physics and condensed matter papers.
Kai: Today's paper: "Quantum fluctuations in hydrodynamics and quantum long-time tails".
Mira: Quantum corrections within an effective field theory framework reveal that fluctuation-dissipation relations mandate intrinsically non-Gaussian noise, leading to a quantum generalization of hydrodynamic long-time tails.
Kai: First, who's behind it and why it matters.
Paper summary: Kai: So, we've talked about what the authors are claiming regarding the "Quantum fluctuations in hydrodynamics and quantum long-time tails" paper, focusing on how their work addresses fluctuation-dissipation relations within an effective field theory. Mira, can you elaborate on what the core thesis is and why they feel this distinction between thermal and quantum fluctuations matters?
Mira: The core claim is that they construct a "quantum Schwinger-Keldysh (SK) effective field theory" specifically for the diffusive hydrodynamics of a conserved scalar field, aiming to include quantum corrections consistent with fluctuation-dissipation theorems. They use the dynamical Kubo-Martin-Schwinger (KMS) symmetry as their guiding principle for introducing fluctuations at the full non-linear level, which ensures consistency at every order.
Lev: That sounds like they are building a very sophisticated mathematical structure before even looking at the results, which is impressive because implementing that KMS symmetry on a closed time contour in SK-EFTs is notoriously difficult to manage.
Kai: It really is; they spend time showing how this symmetry acts on the fields with a relative phase-shift of i beta in imaginary time, and that it becomes local only when goes to zero, which hints at where the classical limit lies.
Mira: And that transition is key because it shows that the KMS symmetry generates terms in the effective action at all orders in the noise field, meaning they necessarily generate intrinsically non-Gaussian noise structures. That's a big statement about how quantum mechanics impacts these systems.
Lev: If you can get the framework right to this extent, what does that suggest about the feasibility of applying these ideas to real-world quantum hardware simulations?
Kai: Well, it suggests that we have a mathematically consistent way to derive the noise structure required by fluctuation-dissipation relations in a quantum hydrodynamic setting, even if we can't build the perfect physical system just yet.
Mira: And their subsequent work then takes this complete effective action and applies it to compute one-loop corrections to the two-point retarded correlation function, which is where they reveal the quantum generalization of hydrodynamic long-time tails.
Lev: That's what I was interested in; those long-time tails are usually where things get messy in simulations, because you need extremely long time scales or very high precision to see them clearly.
Kai: They find that this resulting expression involves a sum over polynomials P d,2n(z), and the important finding there is that these polynomials are identically zero for even n <ref:2601.22140#pg1>.
Mira: That vanishing condition on those polynomials is significant because it simplifies the final closed-form result considerably, leading to their final expression for the one-loop corrections.
Lev: It’s interesting how a constraint derived from symmetry translates into such a neat simplification in the resulting physics, which is exactly what we look for when trying to simplify complex theoretical models for practical use.
Conclusion: Kai: So, wrapping up this discussion on the "Quantum fluctuations in hydrodynamics and quantum long-time tails" paper, we've covered how they used the SK effective field theory and KMS symmetry to derive intrinsically non-Gaussian noise that governs long-time hydrodynamic tails. What are your thoughts on what this means for the broader landscape?
Mira: I think the authors successfully showed that enforcing fluctuation-dissipation relations via KMS symmetry is a valid way to introduce quantum fluctuations, and their derivation of the one-loop corrections provides a specific mathematical structure for these corrections involving those polynomials.
Lev: From an error correction standpoint, the implication is that if we are modeling systems where dissipation is key, we can't ignore these non-Gaussian features; they have shown that the quantum mechanics demands them.
Kai: It means future work needs to focus on extending this framework beyond just one-loop corrections to see how these effects scale up in more complex hydrodynamic scenarios, and whether this structure holds true when we move away from the leading order wavevector expansion.
Mira: The paper's limitation is that it focuses on the one-loop results and provides a closed form only at leading order in the wavevector expansion, so they haven't fully mapped out the behavior at higher orders yet.
Lev: That’s fair; I think extending this to full hydrodynamics would be a natural next step, and perhaps investigating ghost fields could help with regulating frequency integrals, which might open up avenues for non-equilibrium renormalization group flows.
Kai: So, in short, the paper gives us a very solid quantum framework consistent with fluctuation-dissipation requirements, showing that the noise isn't simple Gaussian stuff but something more complex than we initially thought.
Mira: And it does establish a robust method for generating these specific non-Gaussian features through symmetry enforcement within an effective field theory approach.
Lev: It's a very rigorous piece of theoretical work, and it sets a high bar for what we need to achieve when translating these ideas into practical quantum simulations.
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