11,106 research outputs found
Nuclear magnetization distribution and hyperfine splitting in Bi ion
Hyperfine splitting in Bi and Pb ions was calculated using
continuum RPA approach with effective residual forces. To fix the parameters of
the theory the nuclear magnetic dipole moments of two one- particle and two
one-hole nuclei around Pb were calculated using the same approach. The
contribution from velocity dependent two-body spin- orbit residual interaction
was calculated explicitly. Additionally, the octupole moment of Bi and
the hfs in muonic bismuth atom were calculated as well in the same approach.
All the calculated observables, except the electronic hfs in Bi, are in
good agreement with the data. We argue for more accurate measurement of the
octupole moment and the muonic hfs for Bi.Comment: 11 pages, 5 figure
Impact of spin-orbit currents on the electroweak skin of neutron-rich nuclei
Background: Measurements of neutron radii provide important constraints on
the isovector sector of nuclear density functionals and offer vital guidance in
areas as diverse as atomic parity violation, heavy-ion collisions, and
neutron-star structure. Purpose: To assess the impact of spin-orbit currents on
the electromagnetic- and weak-charge radii of a variety of nuclei. Special
emphasis is placed on the experimentally accessible electroweak skin, defined
as the difference between weak-charge and electromagnetic-charge radii.
Methods: Two accurately calibrated relativistic mean field models are used to
compute proton, neutron, charge, and weak-charge radii of a variety of nuclei.
Results: We find that spin-orbit contributions to the electroweak skin of light
neutron-rich nuclei, such as 22O and 48Ca, are significant and result in a
substantial increase in the size of the electroweak skin relative to the
neutron skin. Conclusions: Given that spin-orbit contributions to both the
charge and weak-charge radii of nuclei are often as large as present or
anticipated experimental error bars, future calculations must incorporate
spin-orbit currents in the calculation of electroweak form factors.Comment: 17 pages, 2 figures, and 2 table
Decoherence in Solid State Qubits
Interaction of solid state qubits with environmental degrees of freedom
strongly affects the qubit dynamics, and leads to decoherence. In quantum
information processing with solid state qubits, decoherence significantly
limits the performances of such devices. Therefore, it is necessary to fully
understand the mechanisms that lead to decoherence. In this review we discuss
how decoherence affects two of the most successful realizations of solid state
qubits, namely, spin-qubits and superconducting qubits. In the former, the
qubit is encoded in the spin 1/2 of the electron, and it is implemented by
confining the electron spin in a semiconductor quantum dot. Superconducting
devices show quantum behavior at low temperatures, and the qubit is encoded in
the two lowest energy levels of a superconducting circuit. The electron spin in
a quantum dot has two main decoherence channels, a (Markovian) phonon-assisted
relaxation channel, due to the presence of a spin-orbit interaction, and a
(non-Markovian) spin bath constituted by the spins of the nuclei in the quantum
dot that interact with the electron spin via the hyperfine interaction. In a
superconducting qubit, decoherence takes place as a result of fluctuations in
the control parameters, such as bias currents, applied flux, and bias voltages,
and via losses in the dissipative circuit elements.Comment: review article, 66 pages, 10 figure
Renormalization of the weak hadronic current in the nuclear medium
The renormalization of the weak charge-changing hadronic current as a
function of the reaction energy release is studied at the nucleonic level. We
have calculated the average quenching factors for each type of current (vector,
axial vector and induced pseudoscalar). The obtained quenching in the axial
vector part is, at zero momentum transfer, 19% for the sd shell and 23% in the
fp shell. We have extended the calculations also to heavier systems such as
Ni and Sn, where we obtain stronger quenchings, 44% and 59%,
respectively. Gamow--Teller type transitions are discussed, along with the
higher order matrix elements. The quenching factors are constant up to roughly
60 MeV momentum transfer. Therefore the use of energy-independent quenching
factors in beta decay is justified. We also found that going beyond the zeroth
and first order operators (in inverse nucleon mass) does not give any
substantial contribution. The extracted renormalization to the ratio
at q=100 MeV is -3.5%, -7.1$%, -28.6%, and +8.7% for mass 16, 40, 56, and 100,
respectively.Comment: 28 pages, 6 figure
Anisotropy of the paramagnetic susceptibility in LaTiO: The electron-distribution picture in the ground state
The energy-level scheme and wave functions of the titanium ions in
LaTiO are calculated using crystal-field theory and spin-orbit coupling.
The theoretically derived temperature dependence and anisotropy of the magnetic
susceptibility agree well with experimental data obtained in an untwinned
single crystal. The refined fitting procedure reveals an almost isotropic
molecular field and a temperature dependence of the van Vleck susceptibility.
The charge distribution of the 3d--electron on the Ti positions and the
principle values of the quadrupole moments are derived and agree with NMR data
and recent measurements of orbital momentum and crystal-field splitting.
The low value of the ordered moment in the antiferromagnetic phase is
discussed.Comment: 6 pages, 2 figures, 3 table
First-Principles Calculation of Electric Field Gradients and Hyperfine Couplings in YBa2Cu3O7
The local electronic structure of YBa2Cu3O7 has been calculated using
first-principles cluster methods. Several clusters embedded in an appropriate
background potential have been investigated. The electric field gradients at
the copper and oxygen sites are determined and compared to previous theoretical
calculations and experiments. Spin polarized calculations with different spin
multiplicities have enabled a detailed study of the spin density distribution
to be made and a simultaneous determination of magnetic hyperfine coupling
parameters. The contributions from on-site and transferred hyperfine fields
have been disentangled with the conclusion that the transferred spin densities
essentially are due to nearest neighbour copper ions only with marginal
influence of ions further away. This implies that the variant temperature
dependencies of the planar copper and oxygen NMR spin-lattice relaxation rates
are only compatible with commensurate antiferromagnetic correlations. The
theoretical hyperfine parameters are compared with those derived from
experimental data.Comment: 14 pages, 12 figures, accepted to appear in EPJ
Disentangling the effects of spin-orbit and hyperfine interactions on spin blockade
We have achieved the few-electron regime in InAs nanowire double quantum
dots. Spin blockade is observed for the first two half-filled orbitals, where
the transport cycle is interrupted by forbidden transitions between triplet and
singlet states. Partial lifting of spin blockade is explained by spin-orbit and
hyperfine mechanisms that enable triplet to singlet transitions. The
measurements over a wide range of interdot coupling and tunneling rates to the
leads are well reproduced by a simple transport model. This allows us to
separate and quantify the contributions of the spin-orbit and hyperfine
interactions.Comment: 5 pages, 4 figure
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