Youngman Kim

Dr. Youngman Kim

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Research Focus & Metrics

Academic Career Length

20Years (2007-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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22 October 2007 in Physical Review D
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YKYoungman Kim
Youngman Kim
BLBum-Hoon Lee
Bum-Hoon Lee
SNSiyoung Nam
Siyoung Nam
CPChanyong Park
Chanyong Park
SSSang-Jin Sin
Sang-Jin Sin
In the framework of a holographic QCD approach we study the influence of matter on the deconfinement temperature Tc. We first consider the quark flavor number (Nf) dependence of Tc. We observe that Tc decreases with Nf, which is consistent with a lattice QCD result. We also delve into how the quark number density ρq affects the value of Tc. We find that Tc drops with increasing ρq. In both cases, we confirm that the contributions from quarks are suppressed by 1/Nc, as it should be, compared to the ones from a gravitational action (pure Yang-Mills theory).

9 February 2022 in Physical Review C
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YCYong-Beom Choi
Yong-Beom Choi
CLChang-Hwan Lee
Chang-Hwan Lee
MMMyeonghwan Mun
Myeonghwan Mun
YKYoungman Kim
Youngman Kim
The shape of a nucleus is one of the fundamental nuclear properties. We perform a systematic investigation of bubble nuclei that also exhibit shape coexistence in Hf, W, Os, Pt, and Hg even-even isotopes using the deformed relativistic Hartree-Bogoliubov theory in continuum. For a systematic study, we first consider nuclear bubble structures and shape coexistence separately. We confirm that deformations and pairing correlations hinder bubble structures by comparing our results with those from relativistic continuum Hartree-Bogoliubov theory that assumes spherical symmetry in nuclei. We then predict candidate isotopes with both bubble structure and shape coexistence. We observe that the depletion fraction factor that characterizes bubble structure is mostly smaller in oblate deformation than in prolate, while some isotopes such as Os206 have bubble structures both in oblate and prolate deformations. We compare the proton single-particle energy levels for the candidates of shape coexistence both with only prolate bubble structure and with prolate and oblate bubble structures.

26 November 2019 in Physical Review C
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NSNadezda Smirnova
Nadezda Smirnova
BBB. R. Barrett
B. R. Barrett
YKYoungman Kim
Youngman Kim
ISI. J. Shin
I. J. Shin
ASA. M. Shirokov
A. M. Shirokov
JVJames P Vary
James P Vary
We perform a quantitative study of the microscopic effective shell-model interactions in the valence sd shell, obtained from modern nucleon-nucleon potentials, chiral N3LO, JISP16, and Daejeon16, using no-core shell-model wave functions and the Okubo-Lee-Suzuki transformation. We investigate the monopole properties of those interactions in comparison with the phenomenological universal sd-shell interaction, USDB. Theoretical binding energies and low-energy spectra of O isotopes and of selected sd-shell nuclei, are presented. We conclude that there is a noticeable improvement in the quality of the effective interaction when it is derived from the Daejeon16 potential. We show that its proton-neutron centroids are consistent with those from USDB. We then propose monopole modifications of the Daejeon16 centroids in order to provide an adjusted interaction yielding significantly improved agreement with the experiment. A spin-tensor decomposition of two-body effective interactions is applied in order to extract more information on the structure of the centroids and to understand the reason for deficiencies arising from our current theoretical approximations. The issue of the possible role of the three-nucleon forces is addressed.

21 January 2016 in Physical Review C
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YLYeunhwan Lim
Yeunhwan Lim
XXXuewei Xia
Xuewei Xia
YKYoungman Kim
Youngman Kim
We investigate spherical proton emitters in the region from I (Z=53) to Bi (Z=83) isotopes as a crucial application of the relativistic energy density functional PC-PK1 beyond the drip line. The continuum effect is treated carefully by using the relativistic continuum Hartree-Bogoliubov theory. We calculate the half-lives of the proton emitters using the Wentzel-Kramers-Brillouin (WKB) method and observe that the calculated values are in reasonable agreement with experimental results for most of emitters considered in this study. We also discuss a clue to improve the functional PC-PK1 in future.

1 February 2015 in Journal of the Korean Physical Society
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YKYoungman Kim
Youngman Kim
ISIk Jae Shin
Ik Jae Shin
CLChang-Hwan Lee
Chang-Hwan Lee
MWMew-Bing Wan
Mew-Bing Wan
We study the effects of flavor symmetry breaking on holographic dense matter and compact stars in the D4/D6 model. To this end, two light flavors and one intermediate mass flavor are considered. For two light quarks, we investigate how the strong isospin violation affects the properties of holographic dense matter and compact stars. We observe that quark-antiquark condensates are flavor dependent and show interesting behavior near the transition from dense matter with only one flavor to matter with two flavors. An intermediate mass quark is introduced to investigate the role of the third flavor. The mass-radius relations of holographic compact stars with three flavors show that the mass-radius curve changes drastically at a transition density from which the third flavor begins to appear in the matter.

25 September 2017 in Physical Review D
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YKYoungman Kim
Youngman Kim
BLBum-Hoon Lee
Bum-Hoon Lee
DPD. G. Pak
D. G. Pak
CPChanyong Park
Chanyong Park
TTTakuya Tsukioka
Takuya Tsukioka
The problem of the existence of a stable vacuum field in pure QCD is revised. Our approach is based on using classical stationary nonlinear wave type solutions with an intrinsic mass scale parameter. Such solutions can be treated as quantum-mechanical wave functions describing massive spinless states in quantum theory. We verify whether nonlinear wave type solutions can form a stable vacuum field background within the framework of the effective action formalism. We demonstrate that there is a special class of stationary generalized Wu-Yang monopole solutions that are stable against quantum gluon fluctuations.