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Andreev transport at the boundary between quark-gluon plasma and color superconductor

Original: "Nonequilibrium Andreev transport at the QGP-2SC interface"
arXiv:2606.30521 · 2026-06-29 · CC BY · 4 min · Nuclear Theory High Energy Superconductivity
A theoretical study of non-equilibrium transport across the interface of two exotic phases of matter reveals microscopic mechanisms crucial for neutron star dynamics.
Abstract

This study tackles nonequilibrium Andreev reflection at the interface between quark-gluon plasma (QGP) and a two-color superconducting phase (2SC). Using Schwinger-Keldysh formalism and a relativistic tunneling model, they calculated the momentum-resolved current driven by the chemical potential mismatch between the phases. The reflection appears in the fourth order of the tunneling constant: a quark from the QGP turns into a reflected hole while a Cooper pair is injected into the 2SC condensate. It turns out the reflection is amplified when the voltage bias nears the superconducting gap and gets quenched at higher voltages—just like in ordinary superconductors. This approach paves a field-theoretic path to describing strongly correlated transport across dense-matter interfaces, key for nonequilibrium dynamics in compact stars.

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Context

Born in the aftermath of supernova explosions, neutron stars are natural laboratories for studying matter at extreme densities. In their central regions, where density exceeds nuclear density, hadrons can dissolve into quark-gluon plasma (QGP), and further compression, as predicted in the works of Murray Gell-Mann on quarks and Subrahmanyan Chandrasekhar on mass limits, leads to the formation of color superconductivity (CS). In this phase, quarks form Cooper pairs obeying Bose–Einstein statistics, radically altering the properties of matter. Interfaces between QGP and CS may play a key role in neutron star evolution, influencing heat transport, dissipation of rotational energy, and even the generation of magnetic fields. However, a microscopic description of non-equilibrium transport across such boundaries has long been a gap, especially in the relativistic regime accounting for color and flavor degrees of freedom.

Methods

To overcome the limitations of previous approaches based on wavefunction matching, the authors employed the non-equilibrium Green's function method in the Schwinger-Keldysh formalism — a powerful tool of quantum field theory for systems out of equilibrium. The interface was described by an effective tunneling Hamiltonian with coupling constant T, while the two-flavor CS phase (2SC) was treated via a mean field with a gap Δ introduced into the Nambu-Gorkov Green's functions. The current was computed in the frequency representation using Langreth rules, taking into account both single-particle tunneling and fourth-order contributions in T that involve anomalous (pairing) propagators. This approach preserved the Lorentz-covariant Dirac structure and explicitly included the color-flavor pairing matrix, which is crucial for dense quark matter.

Results

The analysis showed that the Andreev current IA and the intermediate current Iint, associated with virtual pairs, sharply increase when the chemical potential difference Δμ becomes comparable to the gap Δ (about 100 MeV for typical parameters). When Δμ >> |Δ|, Andreev reflection is suppressed, reminiscent of the behavior of ordinary NS contacts. The momentum dependence revealed resonances at k ≈ μQGP − Δμ ± |Δ|, corresponding to the quark energy matching the peak of the anomalous spectral function of the CS phase. In the low-temperature limit (the realm of quantum thermodynamics at T≈25 MeV), the hole branch contributes only to the Andreev current, since for Iint it is blocked by the Pauli principle. The total anomalous current, at small deviations from equilibrium, can dominate over ordinary quasiparticle tunneling, determining the relaxation of the density difference between the phases. Additionally, it was found that due to differences in the tunneling of color charges (red and green quarks are paired, while blue ones are not), color transport occurs, requiring a self-consistent treatment of effective chemical potentials.

Implications

This work provides, for the first time, a microscopic description of Andreev transport across a relativistic interface involving color superconducting phases. This is important for understanding dissipative processes in the interiors of neutron stars, especially shortly after equilibrium-disrupting events — for instance, during accretion or starquakes. The revealed asymmetry of color currents points to a mechanism for generating strong gluon fields, which may influence the evolution of magnetic fields and even observable glitches. Moreover, the results lay the groundwork for studying nucleosynthesis under extreme conditions and contribute to the Standard Model of particle physics, extending it to the non-equilibrium dynamics of strong interactions. The legacy of John Bardeen, the creator of BCS theory, finds new resonance in the context of dense quark matter.

Future development

In the future, the method can be extended to the three-color CFL phase and interfaces with hadronic matter. It would be interesting to investigate the non-equilibrium evolution of color and pressure equilibration due to quantum fluctuations. Combining the developed formalism with numerical simulations of superfluid quark matter hydrodynamics will open the way to predicting cooling curves and seismic activity of compact objects, which can be tested by future astrophysical observations.

Impact

The results will directly impact the theory of compact objects, high-density physics, and quantum transport in relativistic media, and will serve as a starting point for modeling non-equilibrium processes in neutron star astrophysics.

Next steps

Immediate next steps include a quantitative analysis of color charge relaxation, taking into account the back-reaction of gluon fields, and computing the damping time of density imbalance under realistic conditions.

Key open problems

The study touches upon the fundamental problem of the equation of state of cold dense matter and the mechanisms for achieving color neutrality in color superconductors, and also contributes to solving the puzzle of glitches and the thermal evolution of isolated neutron stars.

🎯 A tablespoon of neutron star material weighs about a billion tons: if you could bring it to Earth, it would punch right through the planet under its own weight. In quark matter, this madness is compounded by exotic quantum processes like Andreev reflection.

🎬 In Robert Forward's novel 'Dragon's Egg', life is depicted on the surface of a neutron star, where monstrous gravity and magnetic fields create an incredible world. The ideas of multiphase interiors and quantum interfaces add realism to such visions, hinting at the complex internal dynamics of these objects.

k \approx \mu_{\rm QGP} - \Delta\mu \pm |\Delta|
The momentum of the incident quark must satisfy this equality for maximum current.
\frac{d\Delta N}{dt} = -\frac{G}{\chi}\Delta N
The density difference decays exponentially with a characteristic time χ/G, where G is the conductance and χ is the susceptibility.

Key numbers

  • 2SC energy gap (|Δ|): ≈ 100 MeV (typical value)
  • Quark chemical potential (μ_QGP): ≈ 500 MeV
  • Temperature inside a neutron star: ≈ 25 MeV (~2.9×10^11 K)
  • Enhancement of Andreev current at Δμ ≈ |Δ|: up to several times
  • Order of tunneling current expansion: fourth (T^4) for anomalous processes
Scientists
Wolfgang PauliErwin SchrödingerPaul DiracEmmy NoetherAlbert EinsteinHans Bethe
Tags
superconductivity neutron star plasma Quantum Field Standard Model quantum thermodynamics supernova nucleosynthesis stellar evolution numerical simulation
Laws
Pauli exclusion principleNoether's theoremmass–energy equivalenceFermi–Dirac statisticsspin–statistics theoremFermi's golden rule
Original: arXiv:2606.30521 · CC BY · bridge42worlds