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論文

Chiral Dirac fermion in a collinear antiferromagnet

Zhang, A.*; Deng, K.*; Sheng, J.*; Liu, P.*; Kumar, S.*; 島田 賢也*; Jiang, Z.*; Liu, Z.*; Shen, D.*; Li, J.*; et al.

Chinese Physics Letters, 40(12), p.126101_1 - 126101_8, 2023/12

 被引用回数:1 パーセンタイル:0(Physics, Multidisciplinary)

In a Dirac semimetal, the massless Dirac fermion has zero chirality, leading to surface states connected adiabatically to a topologically trivial surface state as well as vanishing anomalous Hall effect. Recently, itis predicted that in the nonrelativistic limit of certain collinear antiferromagnets, there exists a type of chiral "Dirac-like" fermion, whose dispersion manifests four-fold degenerate crossing points formed by spin-degenerate linear bands, with topologically protected Fermi arcs. Here, by combining with neutron diffraction and first-principles calculations, we suggest a multidomain collinear antiferromagnetic configuration, rendering the existence of the Fermi-arc surface states induced by chiral Dirac-like fermions.

論文

The $$^{59}$$Fe(n,$$gamma$$)$$^{60}$$Fe cross section from the surrogate ratio method and its effect on the $$^{60}$$Fe nucleosynthesis

Yan, S. Q.*; Li, X. Y.*; 西尾 勝久; Lugaro, M.*; Li, Z. H.*; 牧井 宏之; Pignatari, M.*; Wang, Y. B.*; Orlandi, R.; 廣瀬 健太郎; et al.

Astrophysical Journal, 919(2), p.84_1 - 84_7, 2021/10

 被引用回数:1 パーセンタイル:8.87(Astronomy & Astrophysics)

The long-lived $$^{60}$$Fe (with a half-life of 2.62 Myr) is a crucial diagnostic of active nucleosynthesis in the Milky Way galaxy and in supernovae near the solar system. The neutron-capture reaction $$^{59}$$Fe(n,$$gamma$$)$$^{60}$$Fe on $$^{59}$$Fe (half-life=44.5 days) is the key reaction for the production of $$^{60}$$Fe in massive stars. This reaction cross section has been previously constrained by the Coulomb dissociation experiment, which offered partial constraint on the E1 $$gamma$$-ray strength function but a negligible constraint on the M1 and E2 components. In this work, for the first time, we use the surrogate ratio method to experimentally determine the $$^{59}$$Fe(n,$$gamma$$)$$^{60}$$Fe cross sections in which all the components are included. We derived a Maxwellian-averaged cross section of 27.5$$pm$$3.5 mb at $$kT$$ = 30 keV and 13.4$$pm$$1.7 mb at $$kT$$ = 90 keV, roughly 10%-20% higher than previous estimates. We analyzed the impact of our new reaction rates in nucleosynthesis models of massive stars and found that uncertainties in the production of $$^{60}$$Fe from the $$^{59}$$Fe(n,$$gamma$$)$$^{60}$$Fe rate are at most 25$$%$$. We conclude that stellar physics uncertainties now play a major role in the accurate evaluation of the stellar production of $$^{60}$$Fe.

論文

Search for $$XYZ$$ states in $$Upsilon(1S)$$ inclusive decays

Shen, C. P.*; 谷田 聖; Belle Collaboration*; 他153名*

Physical Review D, 93(11), p.112013_1 - 112013_11, 2016/06

AA2016-0391.pdf:1.04MB

 被引用回数:6 パーセンタイル:31.88(Astronomy & Astrophysics)

The branching fractions of the $$Upsilon(1S)$$ inclusive decays into final states with a $$J/psi$$ or a $$psi(2S)$$ are measured with improved precision to be $${cal B}(Upsilon(1S) to J/psi+ {rm anything})= (5.25 pm 0.13 ({rm stat}) pm 0.25({rm syst}))times10^{-4}$$ and $${cal B}(Upsilon(1S) to psi(2S)+ {rm anything})= (1.23 pm 0.17 ({rm stat}) pm 0.11({rm syst}))times10^{-4}$$. The first search for $$Upsilon(1S)$$ into $$XYZ$$ states that decay into a $$J/psi$$ or a $$psi(2S)$$ plus one or two charged tracks yields no significant signals for $$XYZ$$ states in any of the examined decay modes, and upper limits on their production rates in $$Upsilon(1S)$$ inclusive decays are determined.

論文

First observation of $$gammagamma to pbar{p} K^+K^-$$ and search for exotic baryons in $$pK$$ systems

Shen, C. P.*; 谷田 聖; Belle Collaboration*; 他177名*

Physical Review D, 93(11), p.112017_1 - 112017_9, 2016/06

AA2016-0387.pdf:0.89MB

 被引用回数:3 パーセンタイル:18.66(Astronomy & Astrophysics)

The process $$gammagamma to pbar{p} K^+K^-$$ and its intermediate processes are measured for the first time using a 980 fb$$^{-1}$$ data sample collected with the Belle detector at the KEKB asymmetric-energy $$e^+e^-$$ collider. The production of $$pbar{p} K^+K^-$$ and a $$Lambda(1520)^0$$ ($$bar{Lambda}(1520)^0$$) signal in the $$pK^-$$ ($$bar{p}K^+$$) invariant mass spectrum are clearly observed. However, no evidence for an exotic baryon near 1540 MeV/$$c^2$$, denoted as $$Theta(1540)^0$$ ($$bar{Theta}(1540)^0$$) or$$Theta(1540)^{++}$$ ($$bar{Theta}(1540)^{--}$$), is seen in the $$pK^-$$ ($$bar{p}K^+$$) or $$pK^+$$ ($$bar{p}K^-$$) invariant mass spectra. Cross sections for $$gammagamma to pbar{p} K^+K^-$$, $$Lambda(1520)^0bar{p}K^+ + c.c.$$ and the products $$sigma(gammagamma to Theta(1540)^0 bar{p} K^+ + c.c.){cal B}(Theta(1540)^0 to pK^-)$$ and $$sigma(gammagamma to Theta(1540)^{++} bar{p} K^- + c.c.){cal B}(Theta(1540)^{++} to pK^+)$$ are measured. We also determine upper limits on the products of the $$chi_{c0}$$ and $$chi_{c2}$$ two-photon decay widths and their branching fractions to $$pbar{p} K^+K^-$$ at the 90% credibility level.

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