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# Träfflista för sökning "WFRF:(Gao Yu Tang) "

Sökning: WFRF:(Gao Yu Tang)

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1.
• Ablikim, M., et al. (författare)
• Amplitude analysis of the π$^0$π$^0$ system produced in radiative J/ψ decays
• 2016
• Ingår i: PHYSICAL REVIEW D. - 2470-0010. ; 93:3
• Tidskriftsartikel (refereegranskat)abstract
• An amplitude analysis of the π0π0 system produced in radiative J/ψ decays is presented. In particular, a piecewise function that describes the dynamics of the π0π0 system is determined as a function of Mπ0π0 from an analysis of the (1.311±0.011)×109 J/ψ decays collected by the BESIII detector. The goal of this analysis is to provide a description of the scalar and tensor components of the π0π0 system while making minimal assumptions about the properties or number of poles in the amplitude. Such a model-independent description allows one to integrate these results with other related results from complementary reactions in the development of phenomenological models, which can then be used to directly fit experimental data to obtain parameters of interest. The branching fraction of J/ψ→γπ0π0 is determined to be (1.15±0.05)×10-3, where the uncertainty is systematic only and the statistical uncertainty is negligible.
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2.
• Ablikim, M., et al. (författare)
• An improved limit for Gamma(ee) of X(3872) and Gamma(ee) measurement of psi(3686)
• 2015
• Ingår i: Physics Letters B. - 0370-2693 .- 1873-2445. ; 749, s. 414-420
• Tidskriftsartikel (refereegranskat)abstract
• Using the data sets taken at center-of-mass energies above 4 GeV by the BESIII detector at the BEPCII storage ring, we search for the reaction e(+)e(-) -&gt; gamma(ISR) X(3872) -&gt; gamma(ISR)pi(+)pi(-) J/psi via the Initial State Radiation technique. The production of a resonance with quantum numbers J(PC) = 1(++) such as the X(3872) via single photon e(+)e(-) annihilation is forbidden, but is allowed by a next-to-leading order box diagram. We do not observe a significant signal of X(3872), and therefore give an upper limit for the electronic width times the branching fraction Gamma B-X(3872)(ee)(X(3872) -&gt; pi(+)pi(-) J/psi) &lt; 0.13 eVat the 90% confidence level. This measurement improves upon existing limits by a factor of 46. Using the same final state, we also measure the electronic width of the psi(3686) to be Gamma(psi)(ee)(3686) ee = 2213 +/- 18(stat) +/- 99(sys) eV.
3.
• Ablikim, M., et al. (författare)
• Confirmation of a charged charmoniumlike state Z(c)(3885)(-/+) in e(+)e(-) -&gt; pi(+/-) (D(D)over-bar*)(-/+) with double D tag
• 2015
• Ingår i: Physical Review D. - 1550-7998 .- 1550-2368. ; 92:9
• Tidskriftsartikel (refereegranskat)abstract
• We present a study of the process e(+)e(-) -&gt; pi(+/-) (D (D) over bar*)(-/+) using data samples of 1092 pb(-1) at root s = 4.23 GeV and 826 pb(-1) at root s = 4.26 GeV collected with the BESIII detector at the BEPCII storage ring. With full reconstruction of the D meson pair and the bachelor pi(+) in the final state, we confirm the existence of the charged structure Z(c) (3885)(-/+) in the (D (D) over bar*)(-/+) system in the two isospin processes e(+)e(-) -&gt; pi(+DD)-D-0*(-) and e(+)e(-) -&gt; pi+D-D*(0). By performing a simultaneous fit, the statistical significance of Zc(3885)(-/+) signal is determined to be greater than 10 sigma, and its pole mass and width are measured to be M-pole = (3881.7 +/- 1.6(stat) +/- 1.6(syst)) MeV/c(2) and Gamma(pole) = (26.6 +/- 2.0(stat) +/- 2.1(syst)) MeV, respectively. The Born cross section times the (D (D) over bar*)(-/+) branching fraction (sigma(e(+)e(-) -&gt; pi(+/-)Z(c)(3885)(-/+)) x Br(Z(c)(3885)(-/+) -&gt; (D (D) over bar*)(-/+) )) is measured to be (141.6 +/- 7.9(stat) +/- 12.3(syst)) pb at root s = 4.23 GeV and (108.4 +/- 6.9(stat) +/- 8.8(syst)) pb at root s = 4.26 GeV. The polar angular distribution of the pi(+) - Z(c)(3885)(-/+) system is consistent with the expectation of a quantum number assignment of J(P) = 1(+) for Z(c)(3885)(-/+).
4.
• Ablikim, M., et al. (författare)
• Dark photon search in the mass range between 1.5 and 3.4 GeV/c
• 2017
• Ingår i: Physics Letters B. - 0370-2693 .- 1873-2445. ; 774, s. 252-257
• Tidskriftsartikel (refereegranskat)abstract
• Using a data set of 2.93 fb taken at a center-of-mass energy root s = 3.773 GeV with the BESIII detector at the BEPCII collider, we perform a search for an extra U(1) gauge boson, also denoted as a dark photon. We examine the initial state radiation reactions e(+)e(-) -&gt; e(+)e(-) gamma(ISR) and e(+)e(-) -&gt; mu(+)mu(-) gamma(ISR) for this search, where the dark photon would appear as an enhancement in the invariant mass distribution of the leptonic pairs. We observe no obvious enhancement in the mass range between 1.5 and 3.4 GeV/c(2) and set a 90% confidence level upper limit on the mixing strength of the dark photon and the Standard Model photon. We obtain a competitive limit in the tested mass range.
5.
• Ablikim, M., et al. (författare)
• Determination of the number of J/psi events with inclusive J/psi decays
• 2017
• Ingår i: Chinese Physics C, High Energy Physics & Nuclear Physics. - 1674-1137 .- 0899-9996. ; 41:1
• Tidskriftsartikel (refereegranskat)abstract
• A measurement of the number of J/psi events collected with the BESIII detector in 2009 and 2012 is performed using inclusive decays of the J/psi. The number of J/psi events taken in 2009 is recalculated to be (223.7 +/- 1.4) x 10(6), which is in good agreement with the previous measurement, but with significantly improved precision due to improvements in the BESIII software. The number of J/psi events taken in 2012 is determined to be (1086.9 +/- 6.0) x 10(6). In total, the number of J/psi events collected with the BESIII detector is measured to be (1310.6 +/- 7.0) x 10(6), where the uncertainty is dominated by systematic effects and the statistical uncertainty is negligible.
6.
• Ablikim, M., et al. (författare)
• Evidence for $e^+e^-\to\gamma\chi_{c1, 2}$ at center-of-mass energies from 4.009 to 4.360 GeV
• 2015
• Ingår i: CHINESE PHYSICS C. - 1674-1137. ; 39:4
• Tidskriftsartikel (refereegranskat)abstract
• Using data samples collected at center-of-mass energies of √s = 4.009, 4.230, 4.260, and 4.360 GeV with the BESIII detector operating at the BEPCII collider, we perform a search for the process e(+)e(−) → γχ(c)J (J=0, 1, 2) and find evidence for e(+)e(−) → γχ(c1) and e(+)e(−) → γχ(c2) with statistical significances of 3.0σ and 3.4σ, respectively. The Born cross sections σ(B)(e(+)e(−) → γχ(c)J), as well as their upper limits at the 90% confidence level (C.L.) are determined at each center-of-mass energy.
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7.
• Ablikim, M., et al. (författare)
• Measurement of azimuthal asymmetries in inclusive charged dipion production in $e^+e^-$ annihilations at $\sqrt{s}$ = 3.65 GeV
• 2016
• Ingår i: PHYSICAL REVIEW LETTERS. - 0031-9007. ; 116:4
• Tidskriftsartikel (refereegranskat)abstract
• We present a measurement of the azimuthal asymmetries of two charged pions in the inclusive process $e^+e^-\rightarrow \pi\pi X$ based on a data set of 62 $\rm{pb}^{-1}$ at the center-of-mass energy $\sqrt{s}=3.65$ GeV collected with the BESIII detector. These asymmetries can be attributed to the Collins fragmentation function. We observe a nonzero asymmetry, which increases with increasing pion momentum. As our energy scale is close to that of the existing semi-inclusive deep inelastic scattering experimental data, the measured asymmetries are important inputs for the global analysis of extracting the quark transversity distribution inside the nucleon and are valuable to explore the energy evolution of the spin-dependent fragmentation function.
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8.
• Ablikim, M., et al. (författare)
• Measurement of B(psi(3770) -&gt; gamma chi(c1)) and search for psi(3770) -&gt; gamma chi(c2)
• 2015
• Ingår i: Physical Review D. - 1550-7998 .- 1550-2368. ; 91:9
• Tidskriftsartikel (refereegranskat)abstract
• We report a measurement of the branching fraction for psi(3770) -&gt; gamma chi(c1) and search for the transition psi(3770) -&gt; gamma chi(c2) based on 2.92 fb(-1) of e(+)e(-) data accumulated at root s = 3.773 GeV with the BESIII detector at the BEPCII collider. We measure B(psi(3770) -&gt; gamma chi(c1)) = (2.48 +/- 0.15 +/- 0.23) x 10(-3), which is the most precise measurement to date. The upper limit on the branching fraction of psi(3770) -&gt; gamma chi(c2) at a 90% confidence level is B(psi(3770) -&gt; gamma chi(c2)) &lt; 0.64 x 10(-3). The corresponding partial widths are Gamma(psi(3770) -&gt; gamma chi(c1)) = (67.5 +/- 4.1 +/- 6.7)keV and Gamma(psi(3770) -&gt; gamma chi(c2)) &lt; 17.4 keV.
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9.
• Ablikim, M., et al. (författare)
• Measurement of the Absolute Branching Fraction for Lambda(+)(c) -&gt; Lambda e(+)nu(e)
• 2015
• Ingår i: Physical Review Letters. - 0031-9007 .- 1079-7114. ; 115:22
• Tidskriftsartikel (refereegranskat)abstract
• We report the first measurement of the absolute branching fraction for Lambda(+)(c) -&gt; Lambda e(+)nu(e). This measurement is based on 567 pb(-1) of e(+)e(-) annihilation data produced at root s = 4.599 GeV, which is just above the Lambda(+)(c)Lambda(-)(c) threshold. The data were collected with the BESIII detector at the BEPCII storage rings. The branching fraction is determined to be B(Lambda(+)(c) -&gt; Lambda e(+)nu(e)) = [3.63 +/- 0.38(stat) +/- 0.20(syst)] %, representing a significant improvement in precision over the current indirect determination. As the branching fraction for Lambda(+)(c) -&gt; Lambda e(+)nu(e) is the benchmark for those of other Lambda(+)(c) semileptonic channels, our result provides a unique test of different theoretical models, which is the most stringent to date.
10.
• Ablikim, M., et al. (författare)
• Measurement of the branching fraction for psi(3770) -&gt; gamma chi c0
• 2016
• Ingår i: Physics Letters B. - 0370-2693 .- 1873-2445. ; 753, s. 103-109
• Tidskriftsartikel (refereegranskat)abstract
• By analyzing a data set of 2.92 fb(-1) of e(+) e(-) collision data taken at root s = 3.773 GeVand 106.41 x 10(6) psi(3686) decays taken at root s = 3.686 GeVwith the BESIII detector at the BEPCII collider, we measure the branching fraction and the partial decay width for psi(3770)-&gt;gamma chi c0 to be B(psi(3770)-&gt;gamma chi c0) = (6.88 +/- 0.28 +/- 0.67) x 10(-3) and Gamma[psi(3770)-&gt;gamma chi c0] = (187 +/- 8 +/- 19) keV, respectively. These are the most precise measurements to date.
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