Nuclear Theory·nucl-th

Wednesday·November 23, 2022

14 papers—5 primary·9 cross-listed

01
[Submitted on 22 Nov 2022]
Pion Exchange Interaction in Bonn Potential and Relativistic and Non-relativistic Framework in Nuclear Matter
Jinniu Hu🇨🇳 · Chencan Wang🇨🇳
As the residual interaction of quantum chromodynamics in low-energy region, the nucleon-nucleon (NN) potential can only be exactly described by the model picture now. In the Bonn potential, one of the most well-known NN interaction models, the nucleons interact with each other through exchanging the pion and several heavier mesons, where the pion plays an essential role. It provides a partial contribution of tensor force in the intermediate-range region and the main component in the long-range region in NN potential. However, it is very difficult to be treated in the nuclear many-body system due to its pseudovector or pseudoscalar property. Recently, three high-precision charge-dependent Bonn potentials were proposed with pseudovector coupling types and different pion-nucleon coupling strengths and applied them to study the properties of nuclear matter and neutron stars in the non-relativistic and relativistic frameworks. Furthermore, to properly deal with the strong short-range repulsion and tensor force of the NN potential, some new relativistic {\it ab initio} methods have also been developed in the past decade to discuss the role of pion and relativistic effects in nuclear matter.
Comments:
29 pages, 12 figures, 6 tables. Contribution to the "Handbook of Nuclear Physics", Springer Nature, 2022, Eds. I. Tanihata, H. Toki and T. Kajino
Subjects:
Nuclear Theory (nucl-th)
arXiv:
2211.11976 [pdf]
0 citations
02
[Submitted on 22 Nov 2022]
Peculiarity of the stellar CNO cycle with energetic particles
Victor T. Voronchev
A peculiarity of the stellar CNO cycle caused by MeV alpha-particles and protons generated in exoergic nuclear processes is analyzed. The main parameters of these particles and suprathermal reactions induced by them in a stellar core are calculated. It is shown that these reactions can trigger an abnormal nuclear flow in the second branch of the stellar CNO cycle. A conjecture is made that the phenomenon is of a general nature and can manifest in various stars at non-exploding stages of their evolution. The influence of the abnormal flow on some CNO characteristics is demonstrated.
Comments:
6 pages, 8 figures
Subjects:
Nuclear Theory (nucl-th); Solar and Stellar Astrophysics (astro-ph.SR)
arXiv:
2211.12093 [pdf]
Phys.Scripta(2023)·0 citations
03
[Submitted on 22 Nov 2022]
Role of neutron transfer in the reaction mechanism of $^{9}$ Be+ $^{169}$ Tm, $^{181}$ Ta, $^{187}$ Re and $^{197}$ Au systems
Prasanna M. · V. V. Parkar · V. Jha · A. Parmar · Bhushan A. Kanagalekar · B. G. Hegde
The contribution of one neutron stripping cross section to the total reaction cross section has been studied for $^{9}$ Be projectile incident on $^{169}$ Tm, $^{181}$ Ta, $^{187}$ Re and $^{197}$ Au targets around Coulomb barrier energy. The measured one neutron stripping cross sections for these systems have been compared with the coupled channel calculations. The recently developed global set of optical model potential parameters for $^{9}$ Be projectile has been used in the present calculations. The cumulative of measured complete fusion (CF), incomplete fusion (ICF), one neutron stripping and calculated non-capture breakup (NCBU) cross sections is found to explain almost the reaction cross sections for all the targets. A very small contribution from target inelastic states and elastic breakup may contribute to the remaining part. The percentage fraction of cross section for CF, ICF, one neutron stripping, and NCBU over reaction cross section show the dominance of neutron transfer and NCBU at below barrier energies while CF and ICF processes have the major contribution at above barrier energies.
Comments:
12 pages, 3 figures
Subjects:
Nuclear Theory (nucl-th); Nuclear Experiment (nucl-ex)
arXiv:
2211.12113 [pdf]
NPA(2023)·9 citations
04
[Submitted on 22 Nov 2022]
Momentum transport of chiral modes in a thermal QCD medium
Pushpa Panday🇮🇳 · Binoy Krishna Patra🇮🇳
We have investigated the effect of a weak magnetic field on momentum transport in a thermal QCD medium at finite quark chemical potential using a semiclassical kinetic theory. In the presence of a magnetic field, the momentum transport coefficients acquire a tensor structure, reflected by the five shear $(η_{0}, η_{1}, η_{2}, η_{3}$ and $η_{4})$ and two bulk viscous components $(ζ_{0}$ and $ζ_{1})$ . The weak magnetic field removes the degeneracy in the effective mass of flavours, leading to different masses for the left-handed (L) and right-handed (R) chiral modes of quarks. The coefficients, $η_{0}, η_{1}$ and $η_{3}$ decrease with magnetic field in L mode and increase in $R$ mode, whereas, $η_{2}$ and $η_{4}$ increase in both L and $R$ mode. The bulk viscous coefficients, $ζ_{0}$ and $ζ_{1}$ increase with magnetic field for both L and R mode. The shear and bulk viscous coefficients positively amplify with baryon asymmetry.
Subjects:
Nuclear Theory (nucl-th); High Energy Physics — Phenomenology (hep-ph)
arXiv:
2211.12303 [pdf]
IJMPE(2024)·5 citations
05
[Submitted on 22 Nov 2022]
Signatures of the $Δ$ isobar in spin observables of $^{3} He$ electrodisintegration
A. Deltuva
The electrodisintegration of $^{3} He$ is considered focusing on the effects of the $Δ$ isobar excitation which is treated dynamically on the same footing as nucleons. In the region beyond the quasi-elastic peak the predicted transverse response functions $R_{T}$ and $R_{T^{'}}$ are visibly affected. This leads to sizable $Δ$ isobar effects for inclusive and exclusive electron polarization asymmetries in particular kinematic regions. A measurement performed in the proposed regime could provide judgment for models of nuclear forces and currents.
Comments:
5 pages, 4 figures
Subjects:
Nuclear Theory (nucl-th); Nuclear Experiment (nucl-ex)
arXiv:
2211.12413 [pdf]
PLB(2022)·1 citation
06
[Submitted on 21 Nov 2022] (cross-list from hep-ph)
Dead-cone searches in heavy-ion collisions using the jet tree
Leticia Cunqueiro🇮🇹 · Davide Napoletano🇮🇹 · Alba Soto-Ontoso🇨🇭
We explore the possibility of using the dead cone of heavy quarks as a region of the Lund plane where medium-induced gluon radiation can be isolated and characterised. The filling of the dead cone by medium-induced gluons is expected to be the result of the interplay between the minimum angle of such radiation due to transverse momentum broadening and the dead-cone angle. Since the measurement of a fully corrected Lund plane in heavy-ion collisions is currently challenging, we propose to use jet grooming techniques to identify a particular splitting in the jet tree that is both perturbative and sensitive to the dead-cone effect. To that end, we propose a new jet substructure groomer, dubbed Late- $k_{t}$ , that selects the most collinear splitting in a QCD jet above a certain transverse momentum cutoff $k_{t, cut}$ . The role of $k_{t, cut}$ is to guarantee perturbative splittings, while selecting the most collinear splitting enhances the sensitivity to mass effects. As a proof of concept, we study the angular distribution of the splitting tagged by Late- $k_{t}$ both analytically and with Monte Carlo simulations. First, we derive the logarithmic resummation structure in vacuum and demonstrate its capability to distinguish between inclusive and heavy-flavoured jets. Next, we extend the calculation for in-medium jets and show that medium-induced emissions lead to an enhancement of collinear emissions below the dead cone angle. Numerically, we demonstrate an excellent resilience of Late- $k_{t}$ against uncorrelated thermal background, thus confirming this observable as a potential candidate to unveil medium dynamics around the dead cone regime.
Comments:
v2: fixed typo in vacuum splitting function. Conclusions remain unchanged
Subjects:
High Energy Physics — Phenomenology (hep-ph); High Energy Physics — Experiment (hep-ex); Nuclear Experiment (nucl-ex); Nuclear Theory (nucl-th)
arXiv:
2211.11789 [pdf]
PRD(2023)·27 citations
07
[Submitted on 22 Nov 2022] (cross-list from nucl-ex)
Measurement of global spin alignment of vector mesons at RHIC
Subhash Singha (For STAR collaboration)🇨🇳
We report the measurements of spin alignment ( $ρ_{00}$ ) for $K^{* 0}$ , $K^{* 0}$ , $K^{*+}$ , and $K^{*-}$ vector mesons in RHIC isobar collisions (Zr+Zr and Ru+Ru) at $s_{NN}$ = 200 GeV. We observe the first non-zero spin alignment for $K^{*\pm}$ in heavy-ion collisions. The $K^{*\pm}$ $ρ_{00}$ is about 3.9 $σ$ larger than that of $K^{* 0}$ . The observed difference and the ordering between $K^{*\pm}$ and $K^{* 0}$ are surprising, and require further inputs from theory. When comparing between the isobar and Au+Au collisions, no significant system size dependence in $K^{* 0}$ $ρ_{00}$ is observed within uncertainties.
Comments:
Quark Matter 2022 proceedings
Subjects:
Nuclear Experiment (nucl-ex); High Energy Physics — Experiment (hep-ex); Nuclear Theory (nucl-th)
arXiv:
2211.12013 [pdf]
Acta Phys.Polon.Supp.(2023)·4 citations
08
[Submitted on 22 Nov 2022] (cross-list from hep-ph)
Pseudoscalar and Scalar Meson Photoproduction Interpreted by Regge Phenomenology
Igor I. Strakovsky (GWU)🇺🇸 · William J. Briscoe (GWU)🇺🇸 · Olga Cortes Becerra (GWU)🇺🇸 · Michael Dugger (ASU)🇺🇸 · Gary Goldstein (Tufts U.)🇺🇸 · Victor L. Kashevarov (Mainz U.)🇩🇪 · Axel Schmidt (GWU)🇺🇸 · Peter Solazzo (GWU)🇺🇸 · Byung-Geel Yu (Korea Aerospace U.)🇰🇷
We have evaluated pseudoscalar and scalar neutral pion photoproduction in $γ p \to π^{0} p$ and $γ p \to a_{0}^{0} p$ above the resonance region and within Regge phenomenology. Our fit, including GlueX $Σ$ pseudoscalar photoproduction data, shows that previous SLAC $Σ$ measurements for $γ p \to π^{0} p$ above $E_{γ} = 4 GeV$ are at variance with SLAC data with more recent measurements made by GlueX in vicinity of $E_{γ} = 9 GeV$ . The Regge model predicts that the beam polarization asymmetry $Σ$ of the scalar meson is opposite to that of pseudoscalar meson photoproduction, however, the cross sections are similar. While the vector natural parity meson exchange is dominant in both cases, the contribution of the pseudovector unnatural parity meson exchange is very small. Using Regge phenomenology, we predicted high energy behavior for double polarized observables $E$ , $F$ , $G$ , and $H$ for the reactions $γ p \to π^{0} p$ and $γ p \to a_{0}^{0} p$ .
Comments:
8 pages, 5 figures, several small glitches were fixed
Subjects:
High Energy Physics — Phenomenology (hep-ph); High Energy Physics — Experiment (hep-ex); Nuclear Experiment (nucl-ex); Nuclear Theory (nucl-th)
arXiv:
2211.12029 [pdf]
PRC(2023)·3 citations
09
[Submitted on 22 Nov 2022] (cross-list from astro-ph.HE)
Hybrid stars may have an inverted structure
Chen Zhang🇨🇳 · Jing Ren🇨🇳
We propose a new stellar structure of compact stars, the ``cross stars" that consist of a hadronic matter core and a quark matter crust, with an inverted structure compared to the conventional hybrid stars. This distinct stellar structure naturally arises from the quark matter to hadronic matter transition associated with the chemical potential crossing, in the context of the quark matter hypothesis that either strange or up-down quark matter is the ground state of baryonic matter at low pressure. We find that the interplay between the hadronic matter and quark matter compositions of cross stars can help to reconcile the small radii constraints indicated by the LIGO/Virgo GW170817 event, the large radii constraints set for massive compact stars by recent NICER X-ray observations, and the recent observation of the most-massive pulsar PSR J0952-0607. This leaves more space open for the equation of states of both hadronic matter and quark matter.
Comments:
10 pages, 6 figures. Published version. Typo fixed
Subjects:
High Energy Astrophysical Phenomena (astro-ph.HE); General Relativity and Quantum Cosmology (gr-qc); High Energy Physics — Phenomenology (hep-ph); Nuclear Theory (nucl-th)
arXiv:
2211.12043 [pdf]
PRD(2023)·16 citations
10
[Submitted on 22 Nov 2022] (cross-list from hep-lat)
Non-perturbative insights into the spectral properties of QCD at finite temperature
Peter Lowdon🇩🇪 · Owe Philipsen🇩🇪
In quantum field theories at finite temperature spectral functions describe how particle systems behave in the presence of a thermal medium. Although data from lattice simulations can in principle be used to determine spectral function characteristics, existing methods rely on the extraction of these quantities from temporal correlators, which requires one to circumvent an ill-posed inverse problem. In these proceedings we report on a recent approach that instead utilises the non-perturbative constraints imposed by field locality to extract spectral function information directly from spatial correlators. In particular, we focus on the application of this approach to lattice QCD data of the spatial pseudo-scalar meson correlator in the temperature range $220 - 960 MeV$ , and outline why this data supports the conclusion that there exists a distinct pion state above the chiral pseudo-critical temperature $T_{pc}$ .
Comments:
8 pages, 2 figures; talk presented at the XVth Quark confinement and the Hadron Spectrum conference, 1-6 August 2022, Stavanger, Norway
Subjects:
High Energy Physics — Lattice (hep-lat); High Energy Physics — Phenomenology (hep-ph); High Energy Physics — Theory (hep-th); Nuclear Theory (nucl-th)
arXiv:
2211.12073 [pdf]
EPJ Web Conf.(2022)·5 citations
11
[Submitted on 22 Nov 2022] (cross-list from hep-ph)
Molecular state interpretation of charmed baryons in the quark model
Ye Yan🇨🇳 · Xiaohuang Hu🇨🇳 · Yuheng Wu🇨🇳 · Hongxia Huang🇨🇳 · Jialun Ping🇨🇳 · Youchang Yang🇨🇳
Stimulated by the observation of $Λ_{c} (2910)^{+}$ by the Belle Collaboration, the $S$ -wave $q q q q ˉ c (q = u or d)$ pentaquark systems with $I$ = 0, $J^{P}$ = $\frac{1}{2}^{-}, \frac{3}{2}^{-} an d \frac{5}{2}^{-}$ are investigated in the framework of quark delocalization color screening model(QDCSM). The real-scaling method is utilized to check the bound states and the genuine resonance states. The root mean square of cluster spacing is also calculated to study the structure of the states and estimate if the state is resonance state or not. The numerical results show that $Λ_{c} (2910)$ cannot be interpreted as a molecular state, and $Σ_{c} (2800)$ cannot be explained as the $N D$ molecular state with $J^{P} = 1/ 2^{-}$ . $Λ_{c} (2595)$ can be interpreted as the molecular state with $J^{P} = \frac{1}{2}^{-}$ and the main component is $Σ_{c} π$ . $Λ_{c} (2625)$ can be interpreted as the molecular state with $J^{P} = \frac{3}{2}^{-}$ and the main component is $Σ_{c}^{*} π$ . $Λ_{c} (2940)$ is likely to be interpreted as a molecular state with $J^{P} = 3/ 2^{-}$ , and the main component is $N D^{*}$ . Besides, two new molecular states are predicted, one is the $J^{P} = 3/ 2^{-}$ $Σ_{c} ρ$ resonance state with the mass around 3140 MeV, another one is the $J^{P} = \frac{5}{2}^{-}$ $Σ_{c}^{*} ρ$ with the mass of 3188.3 MeV.
Comments:
12 pages, 3 figures
Subjects:
High Energy Physics — Phenomenology (hep-ph); Nuclear Theory (nucl-th)
arXiv:
2211.12129 [pdf]
EPJC(2023)·19 citations
12
[Submitted on 22 Nov 2022] (cross-list from hep-ph)
Charmed hadron production in high-energy nuclear collisions
Andrea Beraudo🇮🇹 · Arturo De Pace🇮🇹 · Marco Monteno🇮🇹 · Marzia Nardi🇮🇹 · Daniel Pablos🇮🇹 · Francesco Prino🇮🇹
We present a new model for the description of heavy-flavor hadronization in high-energy nuclear (and possibly hadronic) collisions, where the process takes place not in the vacuum, but in the presence of other color charges. We explore its effect on the charmed hadron yields and kinematic distributions once the latter is applied at the end of transport calculations used to simulate the propagation of heavy quarks in the deconfined fireball produced in nuclear collisions. The model is based on the formation of color-singlet clusters through the recombination of charm quarks with light antiquarks or diquarks from the same fluid cell. This local mechanism of color neutralization leads to a strong space-momentum correlation, which provides a substantial enhancement of charmed baryon production -- with respect to expectations based on $e^{+} e^{-}$ collisions -- and of the collective flow of all charmed hadrons. We also discuss the similarities between our model and recently developed mechanisms implemented in QCD event generators to simulate medium corrections to hadronization in the presence of other nearby color charges.
Comments:
6 pages, proceedings of ICHEP-2022. arXiv admin note: substantial text overlap with arXiv:2209.04239
Subjects:
High Energy Physics — Phenomenology (hep-ph); Nuclear Experiment (nucl-ex); Nuclear Theory (nucl-th)
arXiv:
2211.12170 [pdf]
0 citations
13
[Submitted on 22 Nov 2022] (cross-list from nucl-ex)
Investigation of octupole collectivity near the $A = 72$ shape-transitional point
M. Spieker · L.A. Riley · P.D. Cottle · K.W. Kemper · D. Bazin · S. Biswas · P.J. Farris · A. Gade · T. Ginter · S. Giraud · J. Li · S. Noji and 4 other authors
Enhanced octupole collectivity is expected in the neutron-deficient Ge, Se and Kr isotopes with neutron number $N \approx 40$ and has indeed been observed for $^{70, 72}$ Ge. Shape coexistence and configuration mixing are, however, a notorious challenge for theoretical models trying to reliably predict octupole collectivity in this mass region, which is known to feature rapid shape changes with changing nucleon number and spin of the system. To further investigate the microscopic configurations causing the prolate-oblate-triaxial shape transition at $A \approx 72$ and their influence on octupole collectivity, the rare isotopes $^{72}$ Se and $^{74, 76}$ Kr were studied via inelastic proton scattering in inverse kinematics. While significantly enhanced octupole strength of $\sim 32$ Weisskopf units (W.u.) was observed for $^{72}$ Se, only strengths of $\sim 15$ W.u. were observed for $^{74, 76}$ Kr. In combination with existing data, the new data clearly question a simple origin of enhanced octupole strengths around $N = 40$ . The present work establishes two regions of distinct octupole strengths with a sudden strength increase around the $A = 72$ shape transitional point.
Subjects:
Nuclear Experiment (nucl-ex); Nuclear Theory (nucl-th)
arXiv:
2211.12288 [pdf]
PRC(2022)·9 citations
14
[Submitted on 22 Nov 2022] (cross-list from hep-ph)
$QQq q q ˉ$ Quark System, Compact Pentaquark, and Gauge/String Duality
Oleg Andreev🇩🇪
For the case of two light flavors we propose the stringy description of the system consisting of two heavy and three light quarks, with the aim of exploring the quark organization inside the system and its low-lying Born-Oppenheimer potentials as a function of the heavy quark separation. Our analysis reveals several critical separations related to the processes of string reconnection, breaking and junction annihilation. We find that a compact pentaquark configuration makes the dominant contribution to the potential of the first excited state at small separations, and for separations larger than $0.1 fm$ , the antiquark-diquark-diquark structure emerges. Moreover, it turns out that the length scale of string junction annihilation is the same as that for the $QQ q ˉ q ˉ$ system. We also discuss the relation to the potential of the $QQq$ system and some relations among the masses of hadrons in the heavy quark limit.
Comments:
26 pages, many figures. arXiv admin note: text overlap with arXiv:2205.12119; v2: minor corrections; v3: clarification added, typos fixed, to appear in PRD
Subjects:
High Energy Physics — Phenomenology (hep-ph); High Energy Physics — Lattice (hep-lat); High Energy Physics — Theory (hep-th); Nuclear Theory (nucl-th)
arXiv:
2211.12305 [pdf]
PRD(2023)·13 citations

Affiliations

first authorsco-authorsvia INSPIRE