Shuangshi Fang η and η’ physics at BESIII

Παρουσίαση με θέμα: "Shuangshi Fang η and η’ physics at BESIII"— Μεταγράφημα παρουσίασης:

1 Shuangshi Fang η and η’ physics at BESIII
(for the BESIII Collaboration ) Institute of High Energy Physics The 7th International Chiral Dynamics Workshop, August 6-10, 2012, Jefferson Lab,USA

2 OUTLINE Introduction η and η’ events at BESIII Recent results Summary
η´→π+π-η η (η´)→π+π-,π0π0 η´→π+π-π0,π0π0π0 η´→π+π-e+e-,π+π-μ+μ- invisible decays Summary

3 Introduction Discovered about 50 years ago
Phys. Rev. Lett. 7,421(1961) Phys. Rev. Lett. 12,567(1964) Discovered about 50 years ago Lightest pseudoscalar nonet Dominant decay modes were observed η’→ π+π-η % η’→γρ(γπ+π-) % η’→π0π0η % η’→2γ % η’→γω % η→2γ % η→π+π-π % η→π0π0π % η→γπ+π %

4 INTRODUCTION Still listed in many facilities’ physics program
（KLOE, WASA-at-COSY, CB at MAMI, GlueX, BESIII …） η/η’ : a rich physics field Unique place to test fundamental symmetries in QCD at low energy Probe physics beyond the Standard Model (SM) η/η’ →2γ chiral anomaly η/η’ →π+π-π quark masses η’→γπ+π box anomaly η/η’ →ππ CP violation η/η’ → μ+μ-π0 ,e+e-π0 C violation η/η’ → μ e LF violation ……

5 Bird view of BEPCII τ –charm physics Charmonium decays/transitions
Linac Storage ring τ –charm physics Charmonium decays/transitions Light hadron spectroscopy … η and η’ physics Charm physics τ physics 5/31/12 Meson2012

6 η and η’ events at BESIII
225million J/ events taken in 2009 ~ 1 billion J/ events taken in 2012 The results in this talk are based on the data sample of 225M J/ events η and η’ production in J/ decays BF(J/ →γη)~1.1×10-3 → 2.3×105 η events BF(J/ →γη’)~5.3×10-3 → 1.2×106 η’ events BF(J/ →ϕη)~7.5×10-4 → 1.7×105 η events BF(J/ →ϕη’)~4.0×10-4 → 0.9×105 η’ events

7 Recent η and η’ results from BESIII
Matrix element for η´→π+π-η Search for CP violation η/η´→π+π-,π0π0 BF measurement of η´→π+π-π0,π0π0π0 BF measurement of η´→π+π-e+e-,π+π-μ+μ- Search for η/η´ invisible decays

8 Matrix Element for the Decay η´→π+π-η Phys. Rev. D83,012003(2011)
Impact of gluon component on the dynamics of η´ decays Comparison to the theoretical calculations with the effective ChPT Previous measurements on the dalitz plot of η´→ππη are from VES,GAMS and CLEO

9 Flat, seems no dynamics is involved Two representations used

10 Results from the fit with two different representations
Phys. Lett.B651,22(2007) Eur. Phys.J.A26,383(2005) Phys. Rev,Lett.84,26(2000) Phys.At.Nucl.68,372(2005) Part of parameters are not consistent with previous work “c” , defined for C parity violation, is consistent with zero within 2 standard deviations

11 Search for CP violation in η/η´→ππ Phys. Rev. D84,032006(2011)
Offer an excellent laboratory for testing P and CP invariance Theoretically proceed via the weak interaction at a level of 10-15~10-27

12 @90% C.L.

13 BF measurement of η´→π+π-π0,π0π0π0
Isospin violating decay modes, related with the quarks Previous measurements are from GAM(S) and CLEOc η´→π+π-π0 O η´→π0π0π0 Phys. Rev.Lett.102,061801(2009) Phys. At.Nucl.71,2124(2008)

14 BF measurement of η´→π+π-π0,π0π0π0
PRL 108, (2012) PDG12: O PDG12: Comparison: Isospin violations in h’ppp :

15 Search for /invisible in J//
offer a window for physics beyond the standard model observation of the invisible final states (may) provides information of light dark matter easy to tag with J// : two body decays; ’s width is quite narrow Reconstructing K+K- and looking at recoiling mass of  Theoretical predictions: B. McElrath PRD 72, (2005) B() ~ 7.4  10-5 B() ~ 8.1  10-7

16 Search for /invisible in J// (Preliminary results)
BESIII Preliminary Result 3 Invisible Nup = %C.L.(Feldman-Cousins) An Unbinned extended Maximum Likelihood fit PDF = NsigPDFsig+ Nbkg1PDFbkg1 + NbkgPDFbkg 3 PDFsig: shape of J/(-+) from data PDFbkg1: shape of J/f0(980)(KLKL) from MC PDFbkg: 1st chebychev poly. Invisible Nup = %C.L.(Bayesian) M(recoiling )(GeV)

17 Search for /invisible in J// (Preliminary results)
B(’invisible)/B(’γγ)< 2.39  90% C.L. B(invisible)/B(γγ)< 3.37  90% C.L. Many uncertainty related to tag side and Detector noise cancelled in the ratio. B(invisible)< 5.31  90% C.L. Theory: B. McElrath PRD 72, (2005) B(invisible)< 1.32  90% C.L. BR() ~ 7.4  10-5 BR() ~ 8.1  10-7 B(invisible)< 1.4  90% C.L. BESII result: PRL 97, (2006) B(invisible)< 6.0  90% C.L.

18 BF measurement of η´→π+π-e+e-,π+π-μ+μ-
Theoretical predictions Decay Effective meson theory PRC 61, (2000) Chiral Unitary EPJA33,95(2007) B(η´→π+π-e+e-) 1.8×10-3 ( ) ×10-3 B(η´→π+π-μ+μ-) 2.0×10-4 ( ) ×10-3 η´→π+π-e+e- was first observed by CLEOc B(η´→π+π-e+e-)=( ±0.5) ×10-3 B(η´→π+π-μ+μ-)< 2.4× @90%C.L. Phys. Rev.Lett.102,061801(2009)

19 BF measurement of η´→π+π-e+e-,π+π-μ+μ- （Preliminary results）
No evident η´→π+π-μ+μ- η´→π+π-e+e- η´→γπ+π- MC M(π+π-μ+μ-) (GeV/c2 ) M(e+e-) (GeV/c2 ) B(η´→π+π-e+e-)=(2.13±0.13(stat)) ×10-3 B(η´→π+π-μ+μ-)< 2.65×10-5 @90%C.L. B(η´→π+π-e+e-)=( ±0.5) × (CLEOc) B(η´→π+π-μ+μ-)< 2.4× @90%C.L (CLEOc)

20 Summary η/η’ decays: a rich physics field
Recent results from BESIII are presented η´→π+π-η η (η´)→π+π-,π0π0 η´→π+π-π0,π0π0π0 η´→π+π-e+e-,π+π-μ+μ- invisible decays ~1 billion J/ events were taken this year more results are expected to come soon !

21 Thanks for you attention