575 research outputs found

    Λ hyperon spin polarization and CP tests at BESIII

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    In these proceedings two preliminary results from the BESIII collaboration on polarized Λ and Λ¯Λˉ\bar \Lambda are reported. Both results are first observations and concern the resonant and non-resonant processes e−e+→J/ψ→ΛΛ¯ee+J/ψΛΛˉ{e^ - }{e^ + } \to J/\psi \to \Lambda \bar \Lambda and e−e+→γ*→ΛΛ¯ee+γΛΛˉ{e^ - }{e^ + } \to {\gamma ^\ast} \to \Lambda \bar \Lambda at s=2.396 GeVs=2.396GeV\sqrt s = 2.396\,{\rm{GeV}}, respectively. For J/ψ→ΛΛ¯J/ψΛΛˉJ/\psi \to \Lambda \bar \Lambda the relative phase between the electric and magnetic form factors, ΔΦ, has for the first time been determined, ΔΦ=42.4(6)stat(5)syst°\Delta \Phi = 42.4{(6)_{{\rm{stat}}}}(5)_{_{{\rm{syst}}}}^^\circ. That ΔΦ≠0ΔΦ0\Delta \Phi \ne 0 allows for a simultaneous measurement also of the asymmetry decay parameters Λ→pπ− (α−)Λpπ(α)\Lambda \to p{\pi ^ - }\,({\alpha _ - }), Λ¯→p¯π+ (α+)Λˉpˉπ+(α+)\bar \Lambda \to \bar p{\pi ^ + }\,({\alpha _ + }) and Λ¯→n¯π0 (α¯0)Λˉnˉπ0(αˉ0)\bar \Lambda \to \bar n{\pi ^0}\,({\bar \alpha _0}). The measured value of α−=0.750±0.009±0.004α=0.750±0.009±0.004{\alpha _ - } = 0.750 \pm 0.009 \pm 0.004 differs by 17(3)% from the PDG value. The simultaneous measurement for the asymmetry parameters allows for the most precise test of CP violation conducted for Λ decays, ACP = −0.006(12)stat(7)syst. The reaction e−e+→ΛΛ¯ee+ΛΛˉ{e^ - }{e^ + } \to \Lambda \bar \Lambda at s=2.396 GeVs=2.396GeV\sqrt s = 2.396\,{\rm{GeV}} is the first complete measurement of the time-like electric (GE) and magnetic (GM) form factor of any baryon as also the ratio R = |(GE/(GM)| and ΔΦ have been determined: R = 0.96(14)(12) and ΔΦ=37(12)stat(6)stat°ΔΦ=37(12)stat(6)stat\Delta \Phi = 37{(12)_{{\rm{stat}}}}(6)_{{\rm{stat}}}^\circ. The obtained cross-section and effective form factor are σ = 119.0(53)stat(51)syst pb and |G| = 0.123(3)stat(3)syst, respectively

    Lambda hyperon spin polarization and CP tests at BESIII

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    In these proceedings two preliminary results from the BESIII collaboration on polarized Lambda and (Lambda) over bar are reported. Both results are first observations and concern the resonant and non-resonant processes e(-)e(+) -> J/psi -> Lambda(Lambda) over bar and e(-)e(+) -> gamma* -> Lambda Lambda at root s = 2.396 GeV, respectively. For J/psi -> Lambda Lambda the relative phase between the electric and magnetic form factors, Delta Phi, has for the first time been determined, Delta Phi = 42.4(6)(stat) (5)(stat degrees). That Delta Phi not equal 0 allows for a simultaneous measurement also of the asymmetry decay parameters Lambda -> p pi(-) (alpha_), (Lambda) over bar -> (p) over bar pi(+) (alpha(+)) and (Lambda) over bar -> (n) over bar pi(0) ((alpha) over bar (0)). The measured value of alpha_ = 0.750 +/- 0.009 +/- 0.004 differs by 17(3)% from the PDG value. The simultaneous measurement for the asymmetry parameters allows for the most precise test of CP violation conducted for A decays, A(cp) = - 0.006(12)(stat) (7)(syst). The reaction e(-)e(+) -> Lambda(Lambda) over bar at root s = 2.396 GeV is the first complete measurement of the time-like electric (G(E)) and magnetic (G(M)) form factor of any baryon as also the ratio R = vertical bar(GE)/(G(M))vertical bar and Delta Phi have been determined: R = 0.96(14)(12) and Delta Phi = 37(12)(stat) (6)(stat)degrees. The obtained cross-section and effective form factor are sigma = 119.0(53)(stat)(51)(syst) pb and vertical bar G vertical bar = 0.123 (3)(stat) (3)(syst), respectively

    Study of hc → 3(π+ π- )π0, hc → (π+ π-) ω, hc → 2(π+ π-)π0η, hc → 2(π+ π -) η, and hc → p‾p

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    Based on (2712.4±14.1)×106 ⁡(3686) events collected with the BESIII detector, we study the decays ℎ→3⁢(+⁢−)⁢0, ℎ→2⁢(+⁢−)⁢, ℎ→2⁢(+⁢−)⁢0⁢, ℎ→2⁢(+⁢−)⁢, and ℎ→⁢¯via ⁡(3686)→0⁢ℎ. The decay channel ℎ→3⁢(+⁢−)⁢0 is observed for the first time, and its branching fraction is determined to be (9.28±1.14±0.77)×10−3, where the first uncertainty is statistical and the second is systematic. In addition, first evidence is found for the modes ℎ→2⁢(+⁢−)⁢0⁢ and ℎ→2⁢(+⁢−)⁢ with significances of 4.8⁢ and 4.7⁢, and their branching fractions are determined to be (7.55±1.51±0.77)×10−3 and (4.00±0.86±0.35)×10−3, respectively. No significant signals of ℎ→2⁢(+⁢−)⁢ and ℎ→⁢¯are observed, and the upper limits of the branching fractions of these decays are determined to be &lt;6.19×10−4 and &lt;4.40×10−5 at the 90% confidence level, respectively.For complete list of authors see http://dx.doi.org/10.1103/PhysRevD.109.072018</p

    Observation of the Anomalous Shape of X(1840) in J/Ï\u88 â\u86\u92 γ3(Ï\u80+ Ï\u80-) Indicating a Second Resonance Near p(p)over-bar Threshold

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    Using a sample of (10087 +/- 44) x 10(6) J/psi events, which is about 45 times larger than that was previously analyzed, a further investigation on the J/psi -&gt; gamma 3(pi(+) pi(-)) decay is performed. A significant distortion at 1.84 GeV/c(2) in the line shape of the 3(pi(+) pi(-)) invariant mass spectrum is observed for the first time, which could be resolved by two overlapping resonant structures, X(1840) and X(1880). The new state X(1880) is observed with a statistical significance larger than 10 sigma. The mass and width of X(1880) are determined to be 1882.1 +/- 1.7 +/- 0.7 MeV/c(2) and 30.7 +/- 5.5 +/- 2.4 MeV, respectively, which indicates the existence of a p (p) over bar bound state.For complete list of authors see http://dx.doi.org/10.1103/PhysRevLett.132.151901</p

    MEASUREMENT OF dd -&gt; (3)He p pi(-) WITH WASA-at-COSY

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    The measurment of the charge symmetry conserving reactions dd -&gt; (3)He p pi(-) and dd -&gt; (3)He n pi(0) is the first step of the charge symmetry breaking physics program with WASA-at-COSY. The analysis of these channels helps to understand the experimental conditions and provides additional parameters for theoretical studies. The data have been collected in November 2007.</p

    Observation of eta(c)(2S) -&gt; 3(pi(+)pi(-)) and measurements of chi(cJ) -&gt; 3(pi(+)pi(-)) in psi (3686) radiative transitions

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    The hadronic decay eta(c) (2S) -&gt; 3 (pi(+)pi(-)) is observed with a statistical significance of 9.3 standard deviations using (448.1 +/- 2.9) x 10(6) psi(3686) events collected by the BESIII detector at the BEPCII collider. The measured mass and width of eta(c) (2S) are (3643.4 +/- 2.3 (stat) +/- 4.4 (syst)) MeV/c(2) and 19.8 +/- 3.9 (stat) +/- 3.1 (syst)) MeV, respectively, which are consistent with the world average values within two standard deviations. The product branching fraction B[psi(3686) -&gt; gamma eta(c) (2S)] X B[eta(c)(2S) -&gt; 3(pi(+)pi(-))] is measured to be (9.2 +/- 1.0(stat)+/- 1.2(syst)10(-6). Using B[psi(3686) -&gt; gamma eta(c) (2S)] = (7.0(-2.5)(+3.4)) x 10(-4), we obtain B[eta(c)(2S) -&gt; 3 (pi(+)pi(-))] = (1.31 +/- 0.15 (stat) +/- 0.17 (syst) ((+0.64)(-0.47)) (extr))x 10(-2), where the third uncertainty is from B [psi(3686)-&gt;gamma eta(c)(2S)]. We also measure the chi(cJ)-&gt; 3(pi(+)pi(-)) (J = 0, 1, 2) decays via psi' -&gt; gamma chi(cJ) transitions. The branching fractions are B[chi(c0) 3(pi(+)pi(-))] = (2.080 +/- 0.006(stat)+/- 0.068(syst))x10(-2), B [chi c(2) -&gt; (pi(+)pi(-))]=1.092 x 0.004(stat)+/- 0.035(syst))x10(-2), and B[chi(C2) -&gt; 3 (pi(+)pi(-))] = 1.565 +/- 0.005 (stat) +/- 0.048 (syst)) x 10(-2).For complete list of authors see http://dx.doi.org/10.1103/PhysRevD.106.032014</p

    Measurement of e plus e- ? : ?p plus p - cross sections at center-of-mass energies from 2.00 to 3.08 GeV

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    Using data corresponding to an integrated luminosity of 651 pb-1 accumulated at 22 center-of-mass energies from 2.00 to 3.08 GeV by the BESIII experiment, the process e+e- &amp; RARR; 0ic+ic- is studied. The cross sections for e+e- &amp; RARR; 0ic+ic- are consistent with previous results, but with improved precision. To measure the mass and width of the structure observed in the cross section line shape, a combine fit is performed after enhancing the contribution from 0f0(980). The fit reveals a structure with the mass of M = 2178 +20 +5 MeV=c2 and the width of &amp; UGamma; = 140 +36 +16 MeV, where the first uncertainties are statistical and the second ones are systematic.For complete list of authors see http://dx.doi.org/10.1103/PhysRevD.108.032011</p

    Observation of χcJ → 3( K+ K-)

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    By analyzing (27.12 ± 0.14) x 108 Ψ(3686) events collected with the BESIII detector operating at the BEPCII collider, the decay processes χcJ → 3(K+ K-) (J = 0, 1, 2) are observed for the first time with statistical significances of 8.2σ, 8.1σ, and 12.4σ, respectively. The product branching fractions of Ψ(3686) → γχcJ , χcJ → 3(K+K-) are presented and the branching fractions of χcJ → 3(K+K-) decays are determined to be Bχc0 → 3(K+K-) = (10.7 ± 1.8 ± 1.1) x 10-6, Bχc1 →3(K+K-) = (4.2 ± 0.9 ± 0.5) x 10-6, and Bχc2 → 3(K+K-) = (7.2 ± 1.1 ± 0.8) x 10-6, where the first uncertainties are statistical and the second are systematic.For complete list of authors see http://dx.doi.org/10.1103/PhysRevD.109.072016</p

    Measurements of the branching fractions of the P-wave charmonium spin-singlet state hc(1P1) →\u86\u92 h+h-π\u800/η

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    Based on (2712.4 ± 14.3) x 106 ψ(3686) events, we investigate four hadronic decay modes of the P-wave charmonium spin-singlet state hc(1P1) → h+h-π0/η(h =π or K) via the process ψ(3686) → π0hc at BESIII. The hc → π+π-π0 decay is observed with a significance of 9.6σ after taking into account systematic uncertainties. Evidences for hc → K+K-π0 and hc → K+K-η are found with significances of 3.5σ and 3.3σ, respectively, after considering the systematic uncertainties. The branching fractions of these decays are measured to be B(hc → π+π-π0) = (1.36 ± 0.16 ± 0.14)x10-3, B(hc → K+K-π0) = (3.26 ± 0.84 ± 0.36) x 10-4, and B(hc → K+K-η) = (3.13 ± 1.08 ± 0.38) x 10-4, where the first uncertainties are statistical and the second are systematic. No significant signal of hc → π+π-η is found, and the upper limit of its decay branching fraction is determined to be B(hc → π+π-η) &lt; 4.0 x 10-4 at the 90% confidence level.For complete list of authors see http://dx.doi.org/10.1103/PhysRevD.110.032023</p

    Measurement of the absolute branching fraction of the inclusive decay Ds plus ? p plus p plus p-X

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    Using an e thorn e- collision data sample with a total integrated luminosity of 3.19 fb-1 collected with the BESIII detector at a center-of-mass energy of 4.178 GeV, the branching fraction of the inclusive decay of the D thorn s meson to final states including at least three charged pions is measured for the first time to be BoD thorn s &amp; RARR; &amp; pi; thorn &amp; pi; thorn &amp; pi;-X thorn 1/4 o32.81 â \u820.35stat â \u820.63syst thorn %. In this measurement the charged pions from K0S meson decays are excluded. The partial branching fractions of D thorn s &amp; RARR;&amp; pi; thorn &amp; pi; thorn &amp; pi;-X are also measured as a function of the &amp; pi; thorn &amp; pi; thorn &amp; pi;- invariant mass.For complete list of authors see http://dx.doi.org/10.1103/PhysRevD.108.032001</p
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