Allard Valentin
Neutrons stars are leftovers of supernovae and contain crushed matter at densities up to those exceeding the atomic nuclei. Such compact stars are good laboratories to study new states of matter which are impossible to recreate on Earth. In particular, the (outer) core of neutron star is made of normal electrons, normal muons and a mixture of neutrons-protons at the superfluid phase. Although such quantum liquids (which flow without any resistance) are well studied in laboratories, the properties of their stellar counterparts still remain uncertain.
Particularly, neutrons and protons do not flow freely from each other, contrary to what could be expected by the definition of superfluidity : due to nuclear interactions, neutrons and protons are mutually entrained (similarly to superfluid 3He-4He mixture, in laboratories) giving rise to a non-dissipative coupling between both superfluids. Such temperature and velocity-dependent entrainment, called Andreev-Bahskin effects (or Entrainment effects) can be studied, microscopically, using energy-density functional theory (which have been widely used in condensed matter) assuming that the total energy of the system can be written as a functional of the density whose minimisation gives the equations of evolution describing such superfluid mixture of neutrons and protons.
Entrainment effects are expected to play a role in the dynamics of neutron stars : a rotating neutron star (also named “pulsar”) is pierced by quantum superfluid neutron vortices which, due to the Andreev-Bahskin effect, entrain the superfluid protons in the opposite direction which induces a magnetic field. Electrons and muons can be scattered off this magnetic field which induces a coupling between the core of the neutron star and its crust. Such core-crust coupling scenario could be a key to explain pulsar frequency glitches (defined as the sudden spin up of some pulsars followed by a long relaxation ranging from days to years).
Despite the absence of a viscous drag, neutrons and protons cannot flow independently and are, due to strong nuclear interactions, mutually entrained : the mass current of one nucleon species is thus given as a combination of the superfluid velocities of both species and of the normal velocity Vex of thermal excitations. Such effect is also encountered, with the name "Andreev-Bashkin effect" or "Entrainment effects", in laboratory superfluid mixtures (like 4He-3He mixtures) and it is described using an entrainment matrix whose elements, the entrainment coefficients, characterize the coupling between the various (superfluid) species constituting the mixture. Andreev-Bashkin effects are supposed to play a role in the global dynamics of rotating neutron stars : as known in terrestrial experiments, a rotating superfluid is pierced by vortices so rotating neutron stars are supposed to contain neutron vortices which will, due to entrainment, induce proton circulation and, consequently, a magnetic field with which electrons and muons will interact giving birth to a frictional coupling between the neutron superfluid and the normal charged particles.
Entrainment matrix can be studied microscopically using the tools of condensed matter, in particular, the energy-density functional which postulates the energy of the neutron-proton system can be written as a functional of density matrices characterizing protons and neutrons. Minimizing this energy at fixed temperature and nucleon number will give the equations of evolution for the density matrices called the time-dependent Hartree-Fock Bogoliubov (TDHFB) equations which are highly non-linear equations due to their self-consistency : the solution define the equations of evolution which, in their turn, give the solution, and so on (see the consistency loop). Working with TDHFB equations, one can find a continuity equation giving the expression of the mass currents. To find the entrainment matrix, one needs to chose the energy-density functional : if the functional was known, one could have solved exactly the N-body problem but, in practice, the exact form of the functional is unknown so we use phenomenological functionals which are functionals whose parameters are fitted to nuclear experiments, astrophysical observations and N-body computations.
Specifying the functional, one can find the form of the entrainment matrix for every temperature T giving consistent entrainment coefficients : for temperatures T above the critical proton (resp. neutron) temperature (temperature above which the proton (resp. neutron) superfluid is destroyed) the proton (resp. neutron) superfluid do not contribute to the mixture anymore so the associated entrainment coefficients rho_np = rho_pn and rho_pp (resp rho_nn) vanish. The results are also consistent with previous theories using low temperature approximation (Fermi-Liquid theory) and can be used to investigate the induced neutron vortex magnetic field or the NS oscillations. These results can also be used to improve the nuclear energy-density functionals and giving a better understanding of matter at huge densities.