σ Production at BES

19
σ Production at BES Gang LI For BES Collaboration IHEP, Beijing,100039,China

description

σ Production at BES. Gang LI For BES Collaboration IHEP, Beijing,100039,China MENU04, Beijing, Aug. 29th — Sep.4th. Outline. Motivation Production in Production in Summary. Motivation. One Boson Exchange Potential ( OBEP ) introduce σ particle . - PowerPoint PPT Presentation

Transcript of σ Production at BES

Page 1: σ Production at BES

σ Production at BES

Gang LI For BES Collaboration IHEP, Beijing,100039,China

MENU04, Beijing, Aug. 29th—Sep.4th

Page 2: σ Production at BES

Outline

Motivation Production in Production in Summary

/)2( JS /J

Page 3: σ Production at BES

Motivation

One Boson Exchange Potential (OBEP) introduce σ particle.OBEP is successful to describe nuclear forces.

Linear model (LM ) also introduced .LM naturally realized the spontaneous breaking of chiral symmetry and PCAC, also the SU(2)×SU(2) current algebra.

σ has disappeared for a long time from PDG due to negative phase shift results of π –π scattering.

New analysis strongly suggest the existence of σ .

But properties of σ still need to be clarified.

Page 4: σ Production at BES

Current states of (PDG2004)Different exp. results not consistent .

Mass and width of σ have large uncertainty .

Page 5: σ Production at BES

σ production in

Two PWA method used : Covariant Helicity Amplitude and Covariant Tensor

Several B-W parameterizations describe σ .

/J

Page 6: σ Production at BES

B-W parameterizations

Page 7: σ Production at BES

Sample of /J

Page 8: σ Production at BES

Fit to J/→+ (Method I)

0++ contribution 2++ contribution

preliminary

b1(1235)Channels fitted to the data:

J/f2(1270) f0(980) b1(1235) ’(1450) f2(1565) f2(2240)

++0 2++

Page 9: σ Production at BES

Fit to J/→+ (Method II)

Channels fitted to the data:

J/f2(1270) f0(980) b1(1235) phase space

2++

0++

Page 10: σ Production at BES

Fit results:

Averaged pole position:

(541 39) (252 42)i MeV

Method I

Method II

Page 11: σ Production at BES

σ production in

pion-pion rescattering corrections and Ψ-πInteractions both small.

(Brown&Cahn, PRL,35:1(1975))

Dipion S-wave dominant (small D-wave).

(J.Z. Bai et.al, PRD62:032002(2000))

Very pure sample obtained with J/Ψ tagged by muon pair;

Contaminations from other decay channels very small (<0.2%).

Good place to study σ.

/)2( JS

Page 12: σ Production at BES

Some distribution of /)2( JS

Dipion invariant mass spectrum Dipion recoiling mass spectrum

cosθ of pion in lab. System cosθ of muon in lab. System

Page 13: σ Production at BES

cosθand φdistribution of and πin lab. and rest frame system respectively

Page 14: σ Production at BES

Analysis Method

Covariant helicity amplitude method used;

Three components are put into fit : (0+), 2+, IPS

A non-interference bkgd to estimate the pions decay effect.

Interference phase space

M. Ishida,hep-ph/0212383

Page 15: σ Production at BES

Fit results

B-W + IPS + interference fit data well.Strong destructive interference required by chiral constraint.Pole position consistent with that of J/Ψ ωππ.

Preliminary

Page 16: σ Production at BES

dipion invariant mass Cosθ of π+

Cosθ of σ

Page 17: σ Production at BES

Summary

Isospin scalar particle studied at BES

with different decay channels of J/Ψ and Ψ(2S)

Different analysis methods were used;

All results are consistent .

Page 18: σ Production at BES

Fit Method

Max. Likelihood method is used;M.C integration is used to do efficiency correction .

Page 19: σ Production at BES

Strong cancellation