Li Xue

Prof. Dr. Li Xue

orcid

Research Focus & Metrics

Academic Career Length

22Years (2005-Present)

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

Representative Publications

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1 May 2015 in The Astrophysical Journal Supplement Series
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Journal Article
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Tong LiuTong Liu
Tong Liu
SHShu-Jin Hou
Shu-Jin Hou
LXLi Xue
Li Xue
Weimin GuWeimin Gu
Weimin Gu

1 February 2021 in The Astrophysical Journal
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Tong LiuTong Liu
Tong Liu
YWYun-Feng Wei
Yun-Feng Wei
LXLi Xue
Li Xue
MSMou-Yuan Sun
Mou-Yuan Sun
A mass paucity of compact objects in the range of ∼2–5 M ⊙ has been suggested by X-ray binary observations, namely, the “lower mass gap.” Gravitational wave detections have unlocked another mass measurement method, and aLIGO/Virgo has observed some candidates in the gap. We revisit the numerical simulations on the core-collapse supernovae (CCSNe) for ∼20–40 M ⊙ progenitor stars with different initial explosion energies. As a result, the lower explosion energy naturally causes more efficient fallback accretion for low-metallicity progenitors, and then the newborn black holes (BHs) in the center of the CCSNe can escape from the gap, but neutron stars cannot easily collapse into BHs in the gap; nevertheless, the final remnants of the solar-metallicity progenitors stick to the gap. If we consider that only drastic CCSNe can be observed and that those with lower explosion energies are universal, the lower mass gap can be reasonably built. The width and depth of the gap are mainly determined by the typical CCSN initial explosion energy and metallicity. One can expect that the future multimessenger observations of compact objects delineate the shape of the gap, which might constrain the properties of the CCSNe and their progenitors.

1 September 2007 in The Astrophysical Journal
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SLShuang‐Liang Li
Shuang‐Liang Li
LXLi Xue
Li Xue
JLJu‐Fu Lu
Ju‐Fu Lu
We present a numerical method for spatially 1.5-dimensional, time-dependent studies of accretion disks around black holes. The method originates from a combination of the standard pseudospectral and adaptive domain decomposition methods found in the literature, but with a number of improvements in both the numerical and physical senses. In particular, we introduce a new treatment for the connection at the interfaces of decomposed subdomains, construct an adaptive function for the mapping between the Chebyshev-Gauss-Lobatto collocation points and the physical collocation points in each subdomain, and modify the oversimplified one-dimensional basic equations of accretion flows to account for the effects of viscous stresses in both the azimuthal and radial directions. Our method is verified by reproducing the best results obtained previously by Szuszkiewicz & Miller on the limit-cycle behavior of thermally unstable accretion disks with moderate viscosity. A new finding is that, according to our computations, the Bernoulli function of the matter in such disks is always and everywhere negative, so that outflows are unlikely to originate from these disks. We are encouraged to study the more difficult case of thermally unstable accretion disks with strong viscosity in ongoing work.

1 September 2007 in Astroparticle Physics
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MAM. Amenomori
M. Amenomori
SAS. Ayabe
S. Ayabe
BXBi Xiaojun
Bi Xiaojun
DCD. Chen
D. Chen
SCS.W. Cui
S.W. Cui
XZX.X. Zhou
X.X. Zhou
We have observed the shadowing of galactic cosmic ray flux in the direction of the moon, the so-called moon shadow, using the Tibet-III air shower array operating at Yangbajing (4300 m a.s.l.) in Tibet since 1999. Almost all cosmic rays are positively charged; for that reason, they are bent by the geomagnetic field, thereby shifting the moon shadow westward. The cosmic rays will also produce an additional shadow in the eastward direction of the moon if cosmic rays contain negatively charged particles, such as antiprotons, with some fraction. We selected 1.5 x10^{10} air shower events with energy beyond about 3 TeV from the dataset observed by the Tibet-III air shower array and detected the moon shadow at $\sim 40 \sigma$ level. The center of the moon was detected in the direction away from the apparent center of the moon by 0.23$^\circ$ to the west. Based on these data and a full Monte Carlo simulation, we searched for the existence of the shadow produced by antiprotons at the multi-TeV energy region. No evidence of the existence of antiprotons was found in this energy region. We obtained the 90% confidence level upper limit of the flux ratio of antiprotons to protons as 7% at multi-TeV energies.Comment: 13pages,4figures; Accepted for publication in Astroparticle Physic

1 January 2012 in Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Journal Article
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GAG. Aielli
G. Aielli
CBC. Bacci
C. Bacci
BBB. Bartoli
B. Bartoli
PBP. Bernardini
P. Bernardini
XBX.J. Bi
X.J. Bi
GZG. Zizzi
G. Zizzi
The ARGO-YBJ experiment at YangBaJing in Tibet (4300 m a.s.l.) has been taking data with its full layout since October 2007. Here we present a few significant results obtained in gamma-ray astronomy and cosmic-ray physics. Emphasis is placed on the analysis of gamma-ray emission from point-like sources (Crab Nebula, MRK 421), on the preliminary limit on the antiproton/proton flux ratio, on the large-scale cosmic-ray anisotropy and on the proton–air cross-section. The performance of the detector is also discussed, and the perspectives of the experiment are outlined

20 April 2016 in The Astrophysical Journal
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Tong LiuTong Liu
Tong Liu
LXLi Xue
Li Xue
XZXiao-Hong Zhao
Xiao-Hong Zhao
FZFu-Wen Zhang
Fu-Wen Zhang
BZBing Zhang
Bing Zhang
Black holes (BHs) hide themselves behind various astronomical phenomena and their properties, i.e., mass and spin, are usually difficult to constrain. One leading candidate for the central engine model of gamma-ray bursts (GRBs) invokes a stellar mass BH and a neutrino-dominated accretion flow (NDAF), with the relativistic jet launched due to neutrino-anti-neutrino annihilations. Such a model gives rise to a matter-dominated fireball, and is suitable to interpret GRBs with a dominant thermal component with a photospheric origin. We propose a method to constrain BH mass and spin within the framework of this model and apply the method to the thermally dominant GRB 101219B, whose initial jet launching radius, r 0, is constrained from the data. Using our numerical model of NDAF jets, we estimate the following constraints on the central BH: mass M BH ∼ 5–9 M ⊙, spin parameter a * ≳ 0.6, and disk mass 3 M ⊙ ≲ M disk ≲ 4 M ⊙. Our results also suggest that the NDAF model is a competitive candidate for the central engine of GRBs with a strong thermal component.