PaperPanorama

Nuclear Theory·nucl-th

Tuesday·June 18, 2019

10 papers6 primary·4 cross-listed

  1. 01

    Interpretable deep learning for nuclear deformation in heavy ion collisions

    Long-Gang Pang🇺🇸 · Kai Zhou🇩🇪 · Xin-Nian Wang🇺🇸

    The structure of heavy nuclei is difficult to disentangle in high-energy heavy-ion collisions. The deep convolution neural network (DCNN) might be helpful in mapping the complex final states of heavy-ion collisions to the nuclear structure in the initial state. Using DCNN for supervised regression, we successfully extracted the magnitude of the nuclear deformation from event-by-event correlation between the momentum anisotropy or elliptic flow () and total number of charged hadrons () within a Monte Carlo model. Furthermore, a degeneracy is found in the correlation between collisions of prolate-prolate and oblate-oblate nuclei. Using the Regression Attention Mask algorithm which is designed to interpret what has been learned by DCNN, we discovered that the correlation in total-overlapped collisions is sensitive to only large nuclear deformation, while the correlation in semi-overlapped collisions is discriminative for all magnitudes of nuclear deformation. The method developed in this study can pave a way for exploration of other aspects of nuclear structure in heavy-ion collisions.

    nucl-thhep-ph23 citations
  2. 02

    High-K isomer and the rotational properties in the odd-Z neutron-rich nucleus Eu

    Xiao-Tao He · Ze-Long Chen

    The newly observed isomer and ground-state band in the odd-Z neutron-rich rare-earth nucleus Eu are investigated by using the cranked shell model (CSM) with pairing treated by the particle-number conserving (PNC) method. This is the first time detailed theoretical investigations are performed of the observed keV isomer and ground-state rotational band in Eu. The experimental data are reproduced very well by the theoretical results. The configuration of the keV isomer is assigned as the three-particle state ). More low-lying multi-particle states are predicted in Eu. Due to its significant effect on the nuclear mean field, the high-order deformation plays an important role in the energy and configuration assignment of the multi-particle states. Compared to its neighboring even-even nuclei Sm and Gd, there is a increase of of the one-particle ground-state band in Eu. This is explained by the pairing reduction due to the blocking of the nucleon on the proton [413] orbital in Eu.

    nucl-thnucl-exCPC(2019)·4 citations
  3. 03

    A machine learning study to identify spinodal clumping in high energy nuclear collisions

    Jan Steinheimer🇩🇪 · LongGang Pang🇺🇸 · Kai Zhou🇩🇪 · Volker Koch🇺🇸 · Jørgen Randrup🇺🇸 · Horst Stoecker🇩🇪

    The coordinate and momentum space configurations of the net baryon number in heavy ion collisions that undergo spinodal decomposition, due to a first-order phase transition, are investigated using state-of-the-art machine-learning methods. Coordinate space clumping, which appears in the spinodal decomposition, leaves strong characteristic imprints on the spatial net density distribution in nearly every event which can be detected by modern machine learning techniques. On the other hand, the corresponding features in the momentum distributions cannot clearly be detected, by the same machine learning methods, in individual events. Only a small subset of events can be systematically differentiated if only the momentum space information is available. This is due to the strong similarity of the two event classes, with and without spinodal decomposition. In such scenarios, conventional event-averaged observables like the baryon number cumulants signal a spinodal non-equilibrium phase transition. Indeed the third-order cumulant, the skewness, does exhibit a peak at the beam energy ( A GeV), where the transient hot and dense system created in the heavy ion collision reaches the first-order phase transition.

    nucl-thhep-phJHEP(2019)·65 citations
  4. 04

    Comparison between Variational Monte Carlo and Shell Model Calculations of Neutrinoless Double Beta Decay Matrix Elements in Light Nuclei

    X.B. Wang🇨🇳 · A.C. Hayes🇺🇸 · J. Carlson🇺🇸 · G.X. Dong🇨🇳 · E. Mereghetti🇺🇸 · S. Pastore🇺🇸 · R.B. Wiringa🇺🇸

    Benchmark comparisons between many-body methods are performed to assess the ingredients necessary for an accurate calculation of neutrinoless double beta decay matrix elements. Shell model and variational Monte Carlo (VMC) calculations are carried out for and nuclei. Different variational wavefunctions are used to evaluate the uncertainties in the {\it ab initio} calculations, finding fairly small differences between the VMC double beta decay matrix elements. For shell model calculations, the role of model space truncation, radial wavefunction choices, and short-range correlation are investigated and all found to be important. Based on the detailed comparisons between the VMC and shell model approaches, we conclude that accurate descriptions of neutrinoless double beta decay matrix elements require a proper treatment of both long-range and short-range correlations.

    nucl-thPLB(2019)·32 citations
  5. 05

    Fusion hindrance effects in laser-induced non-neutral plasmas

    Salvatore Simone Perrotta (1, 2 3, and 4) · Aldo Bonasera (2 and 4) ((1) Dipartimento di Fisica e Astronomia, Università degli studi di Catania, (2) Scuola Superiore di Catania, Università degli studi di Catania, (3) Cyclotron Insitute, Texas A&M University, (4) Laboratori Nazionali del Sud, Istituto Nazionale di Fisica Nucleare)

    Inertial confinement fusion hotspots and cluster Coulomb explosion plasmas may develop a positive net electric charge. The Coulomb barrier penetrability and the rate of nuclear fusion reactions at ultra-low energies ( keV) are altered by such an environment. These effects are here studied via the screening potential approach. Approximate analytical results are developed by evaluating the average screening potential for some scenarios of interest. It is found that fusion is hindered for reactions between thermal fuel nuclei, while an enhancement is expected for secondary and "beam-target" reactions. Depending on the plasma conditions, the variations can be relevant even for relatively small net charges (several % difference or more in the fusion rate for an average net charge per nucleus of proton charges).

    nucl-thastro-ph.SRphysics.plasm-phNPA(2019)·3 citations
  6. 06

    B(He) from short range effective field theory

    Lorenzo Contessi🇮🇱 · Nir Barnea🇮🇱 · Avraham Gal🇮🇱

    We present an effective field theory (EFT) at leading order to describe light single- hypernuclei. Owing to the weak binding and to the short interaction range, meson exchange forces are approximated by contact interactions within a pionless EFT where the only degrees of freedom are baryons. At leading order, the -nuclear interaction contains two 2-body (singlet and triplet) and three 3-body interaction terms, a total of 5 terms associated with 5 coupling strengths or low energy constants (LECs). We adopt the 2-body LECs from hyperon-nucleon scattering data and interaction models that constrain the scattering lengths, while the 3-body LECs are adjusted using both 3-body and 4-body hypernuclear binding energies. To calculate the binding energies for A-body systems with A2, we expand the wavefunctions using a correlated Gaussian basis. The stochastic variational method is employed to select the non-linear parameters. The resulting \nopieft~is then applied to calculate the separation energy in He, where the adjusted 3-body interactions largely resolve the known overbinding problem of He.

    nucl-thAIP Conf.Proc.(2019)·6 citations

Affiliations

first authorsco-authorsvia INSPIRE