368 research outputs found
Non-uniform Matter in Neutron Star Crusts Studied by the Variational Method with Thomas-Fermi Calculations
The equation of state (EOS) for neutron star (NS) crusts is studied in the
Thomas-Fermi (TF) approximation using the EOS for uniform nuclear matter
obtained by the variational method with the realistic nuclear Hamiltonian. The
parameters associated with the nuclear three-body force, which are introduced
to describe the saturation properties, are finely adjusted so that the TF
calculations for isolated atomic nuclei reproduce the experimental data on
masses and charge distributions satisfactorily. The resulting root-mean-square
deviation of the masses from the experimental data for mass-measured nuclei is
about 3 MeV. With use of the nuclear EOS thus determined, the nuclei in the
crust of NS at zero temperature are calculated. The predicted proton numbers of
the nuclei in the crust of NS are close to the gross behavior of the results by
Negele and Vautherin, while they are larger than those for the EOS by Shen et
al. due to the difference in the symmetry energy. The density profile of NS is
calculated with the constructed EOS.Comment: 38 pages, 9 figures, accepted for publication in PT
Variational Calculation for the Equation of State of Nuclear Matter at Finite Temperatures
An equation of state (EOS) for uniform nuclear matter is constructed at zero
and finite temperatures with the variational method starting from the realistic
nuclear Hamiltonian composed of the Argonne V18 and UIX potentials. The energy
is evaluated in the two-body cluster approximation with the three-body-force
contribution treated phenomenologically so as to reproduce the empirical
saturation conditions. The obtained energies for symmetric nuclear matter and
neutron matter at zero temperature are in fair agreement with those by Akmal,
Pandharipande and Ravenhall, and the maximum mass of the neutron star is 2.2
Msolar. At finite temperatures, a variational method by Schmidt and
Pandharipande is employed to evaluate the free energy, which is used to derive
various thermodynamic quantities of nuclear matter necessary for supernova
simulations. The result of this variational method at finite temperatures is
found to be self-consistent.Comment: Revised Versio
Measurement of scintillation from proportional electron multiplication in liquid xenon using a needle
Charge amplification in liquids could provide single-phase xenon time projection chambers with background discrimination and fiducialisation capabilities similar to those found in dual-phase detectors. Although efforts to achieve the high electric field required for charge amplification and proportional scintillation in liquid xenon have been previously reported, their application to large-scale detectors remains elusive. This work presents a new approach to this challenge, where — instead of the thin-wire approach of previous studies — a needle-like high-voltage electrode is employed to demonstrate proportional charge amplification and secondary scintillation production in liquid xenon. This is an important milestone towards the development of an electrode structure that could be utilised in a large-scale, single-phase time projection chamber with dual read-out
Search for exotic neutrino-electron interactions using solar neutrinos in XMASS-I
We have searched for exotic neutrino-electron interactions that could be
produced by a neutrino millicharge, by a neutrino magnetic moment, or by dark
photons using solar neutrinos in the XMASS-I liquid xenon detector. We observed
no significant signals in 711 days of data. We obtain an upper limit for
neutrino millicharge of 5.410 at 90\% confidence level
assuming all three species of neutrino have common millicharge. We also set
flavor dependent limits assuming the respective neutrino flavor is the only one
carrying a millicharge, for , for , and for .
These limits are the most stringent yet obtained from direct measurements. We
also obtain an upper limit for the neutrino magnetic moment of
1.810 Bohr magnetons. In addition, we obtain upper limits for
the coupling constant of dark photons in the model of
1.310 if the dark photon mass is 1 MeV,
and 8.810 if it is 10 MeV
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