882 research outputs found
Shallow and diffuse spin-orbit potential for proton elastic scattering from neutron-rich helium isotopes at 71 MeV/nucleon
Vector analyzing powers for proton elastic scattering from 8He at 71
MeV/nucleon have been measured using a solid polarized proton target operated
in a low magnetic field of 0.1 T. The spin-orbit potential obtained from a
phenomenological optical model analysis is found to be significantly shallower
and more diffuse than the global systematics of stable nuclei, which is an
indication that the spin-orbit potential is modified for scattering involving
neutron-rich nuclei. A close similarity between the matter radius and the
root-mean-square radius of the spin-orbit potential is also identified.Comment: 6 pages, 4 figures, accepted for publication in Physical Review C
Rapid Communicatio
Large uniaxial magnetic anisotropy of Co-Pt perpendicular films induced by lattice deformation
14Be(p,n)14B reaction at 69 MeV in inverse kinematics
A Gamow-Teller (GT) transition from the drip-line nucleus 14Be to 14B was
studied via the (p,n) reaction in inverse kinematics using a secondary 14Be
beam at 69 MeV/nucleon. The invariant mass method is employed to reconstruct
the energy spectrum. A peak is observed at an excitation energy of 1.27(2) MeV
in 14B, together with bumps at 2.08 and 4.06(5) MeV. The observed forward
peaking of the state at 1.27 MeV and a good description for the differential
cross section, obtained with a DWBA calculation provide support for the 1+
assignment to this state. By extrapolating the cross section to zero momentum
transfer the GT-transition strength is deduced. The value is found to compare
well with that reported in a beta-delayed neutron emission study.Comment: 5 pages, 2 figure
CoPtCr-SiO2 perpendicular media for high density recording with a high order magnetic anisotropy energy term
Coulomb and nuclear breakup of a halo nucleus 11Be
Breakup reactions of the one-neutron halo nucleus 11Be on Pb and C targets at
about 70 MeV/u have been investigated by measuring the momentum vectors of the
incident 11Be, outgoing 10Be, and neutron in coincidence. The relative energy
spectra as well as the angular distributions of the 10Be+n center of mass have
been extracted for both targets. For the breakup on Pb target, the selection of
forward scattering angles is found to be effective to extract almost purely the
first-order E1 Coulomb breakup component, and to exclude the nuclear
contribution and higher-order Coulomb breakup components. This angle-selected
energy spectrum is thus used to deduce the spectroscopic factor for the
10Be(0+) 2s_1/2 configuration in 11Be which is found to be 0.72+-0.04 with
B(E1) up to Ex=4 MeV of 1.05+-0.06 e2fm2. The energy weighted E1 strength up to
Ex=4 MeV explains 70+-10% of the cluster sum rule, consistent with the obtained
spectroscopic factor. The non-energy weighted sum rule is used to extract the
root mean square distance of the halo neutron to be 5.77(16) fm, consistent
with previously known values. In the breakup with C target, we have observed
the excitations to the known unbound states in 11Be at Ex=1.78 MeV and 3.41
MeV. Angular distributions for these states show the diffraction pattern
characteristic of L=2 transitions, resulting in J^pi =(3/2,5/2)+ assignment for
these states. We finally find that even for the C target the E1 Coulomb direct
breakup mechanism becomes dominant at very forward angles.Comment: 14 pages, 7 figures, accepted for publication on Physical Review
One-neutron knockout reaction of 17C on a hydrogen target at 70 MeV/nucleon
First experimental evidence of the population of the first 2- state in 16C
above the neutron threshold is obtained by neutron knockout from 17C on a
hydrogen target. The invariant mass method combined with in-beam gamma-ray
detection is used to locate the state at 5.45(1) MeV. Comparison of its
populating cross section and parallel momentum distribution with a Glauber
model calculation utilizing the shell-model spectroscopic factor confirms the
core-neutron removal nature of this state. Additionally, a previously known
unbound state at 6.11 MeV and a new state at 6.28(2) MeV are observed. The
position of the first 2- state, which belongs to a member of the lowest-lying
p-sd cross shell transition, is reasonably well described by the shell-model
calculation using the WBT interaction.Comment: 15 pages, 3 figure
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