21 research outputs found
Slope parameters determined from CREX and PREX2
[Background] Very lately, the CREX group presents a skin value ~fm. Meanwhile, the PREX group reported a skin value
~fm.
In our previous paper, we determined both the --
relation and the -- one, using 206 EoSs, where
is a slope parameter. [Purpose] We determine from and , using
207 EoSs. [Results] The yields ~MeV and the does
~MeV. [Conclusion] There is no overlap between
and . This is a big problem to be solved
C+C scattering as the reference system for reaction cross section
In our previous paper, we tested the chiral (Kyushu) folding model for
C+C scattering, since the profile function in the Glauber mode is
constructed for the system. We found that the folding model is reliable for
reaction cross sections in 30 \lsim E_{\rm lab} \lsim 100
~MeV and 250 \lsim E_{\rm lab} \lsim 400 ~MeV. Accurate data are available
for C scattering on Be, C, Al targets in 30 \lsim
E_{\rm lab} \lsim 400 ~MeV. We determine matter radius of
C from the accurate , using the Kyushu
-matrix folding model. Our result is ~fm for C. The model is applied for the accurate data on
C+Al scattering, and yields ~fm for Al. Our conclusion is that ~fm agrees with ~fm determined
from interaction cross sections by Tanihata {\it et. al.}.Comment: arXiv admin note: text overlap with arXiv:2306.0960
Neutron skin thickness of Sn determined from reaction cross sections of proton scattering
The cross sections of SDR in the Sb isotopes have been measured. Within the
model used, the neutron-skin thicknesses deduced
fm for Sn, fm for Sn, fm for Sn, fm for Sn, fm for
Sn. We tested the chiral (Kyushu) -matrix folding model for
C+C scattering, and found that the Kyushu -matrix folding
model is reliable for reaction cross sections in MeV and MeV. We determine neutron skin
thickness , using measured of
He+Sn scattering. The results are fm for Sn, fm for Sn, fm for
Sn. The are available for proton scattering on
Sn with high accuracy. Our aim is to determine for Sn with small errors by using the
Kyushu -matrix folding model. Our model is the folding model with the
densities scaled from the D1S-GHFB+AMP neutron density. The proton radii of
D1S-GHFB+AMP agree with those calculated with the isotope shift method based on
the electron scattering. We then scale the neutron densities so as to reproduce
the . In MeV, we determine
from measured . The values are
~fm for Sn, fm for Sn, fm for Sn, fm for Sn. As for Sn, the skin value in MeV is fm. Our results are consistent with the previous
values.Comment: arXiv admin note: text overlap with arXiv:2211.1668
Determination of matter radius and neutron-skin thickness of Ni from reaction cross section of proton scattering on Ni targets
In our previous work, we determined matter radii and
neutron-skin thickness from reaction cross sections
of proton scattering on Pb, Ni,
Ca, C targets, using the chiral (Kyushu) -matrix folding
model with the densities calculated with Gogny-D1S-HFB (D1S-GHFB) with angular
momentum projection (AMP). The resultant agree with
the PREX2 and CREX values. As for Ni, our value is consistent with one
determined from the differential cross section for Ni+He
scattering. As for p+N scattering, are
available as a function of incident energies , where ~MeV for Ni, ~MeV for Ni,
~MeV for Ni. Our aim is to determine matter radii
for Ni from the . Our method is the Kyushu -matrix folding model with the densities
scaled from D1S-GHFB+AMP densities, Our skin values are ~fm, and ~fm for
Ni, respectively
Folding-model approach to reaction cross section of He+C scattering at 790 MeV
Tanihata {\it et al.} determined matter radii for
He from interaction cross sections of
He+C scattering at 790 MeV per nucleon, using the optical
limit of the Glauber model. Lu {\it et al.} determined proton radii for He with the atomic isotope shifts (AIS). We investigate
whether the Love-Franey -matrix folding model is good for
He+C scattering at 790 MeV per nucleon
Reaction cross section of proton scattering consistent with PREX-II
Background: The neutron skin thickness of PREX-II is
presented in Phys. Rev. Lett. {\bf 126}, 172502 (2021). The reaction cross
section is useful to determine the matter radius and . For proton scattering, the reaction cross section are
available for MeV.
Method and results: We determine fm and
fm from = 5.444 fm and . The calculated with D1S-GHFB with the angular
momentum projection (AMP). agrees with . The neutron density
calculated with GHFB+AMP is scaled so as to fm. The
Love-Franey -matrix model with the scaled densities reproduces the data on
.
Aim: Our aim is to find the of proton scattering consistent with
.
Conclusion: The of proton scattering consistent with are at MeV.Comment: arXiv admin note: text overlap with arXiv:2010.0245
Neutron-skin values and matter and neutron radii determined from reaction cross sections of proton scattering on C, Ca, Ni, Pb
Very lately, the PREX and the CREX collaboration present skin values, and , respectively. We recently determined a neutron-skin
value fm from measured reaction cross
sections of p+Pb scattering in a range of
incident energies 10 \lsim E_{\rm in} \lsim 100 MeV where the chiral (Kyushu)
-matrix folding model is reliable for C+C scattering. The data
are available for proton scattering on Ni,
Ca, C targets. Our first aim is to test the Kyushu -matrix
folding model for p+Pb scattering in 20 \lsim E_{\rm in} \lsim 180
MeV. Our second aim is to determine skin values and matter and
neutron radii, and , for Pb, Ni,
Ca, C from the . Our method is the
Kyushu -matrix folding model with the densities scaled from the D1S-GHFB+AMP
densities, where D1S-GHFB+AMP stands for Gogny-D1S HFB (GHFB) with the angular
momentum projection (AMP). As for proton scattering, we find that our model is
reliable in 20 \lsim E_{\rm in} \lsim 180 MeV. For Pb, the skin value
deduced from in 20 \lsim E_{\rm in} \lsim 180 MeV
is fm. Our results on
are compared with the previous works. Our result fm agrees with fm. In addition, our result fm is consistent with the CREX value