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Qiang Zhao

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Title: Qiang Zhao


1
Institute of High Energy Physics, CAS
The role of electromagnetic transitions in V ? V
P
  • Qiang Zhao
  • Theory Division, Institute of High Energy
    Physics, CAS
  • Department of Physics, University of Surrey

11-th International conference on Meson-Nucleon
Physics, Jülich, Sept. 13, 2007
2
Topics
  • The role of the EM transitions in the explanation
    of ?? puzzle and 12 rule in J/?, ? ? V P (
    V ?, ?, ?, K P ?, ?, ??, K)
  • Isospin violations in V ? V P, e.g. ?, J/? ? ? ?0

3
Topics
  • The role of the EM transitions in the explanation
    of ?? puzzle and 12 rule in J/?, ? ? V P (
    V ?, ?, ?, K P ?, ?, ??, K)
  • Isospin violations in V ? V P, e.g. ?, J/? ? ? ?0

4
Motivation
  • Experimental observation of obvious isospin
    violations in ? ? ? ?0.
  • Mechanisms for OZI-rule violation in the low
    energy region.
  • Interferences between different isospin-violating
    sources.

5
Isospin violation in ? ? ? ?0
  • Flavor-changed transition via two processes
  • I) Isospin violation via electromagnetic decays
  • EM interaction does not conserve isospin
  • II) Isospin violation in strong decays
  • u and d quark have different masses

6
Electromagnetic transition in ? ? ? ?0
? (I0)
?
s
?
?
?
? (I0)
?0
?0
?0 (I1)
?s
7
  • Vector meson dominance model

??
??
e
e
?
?
V (?, ?, ? )

??
??
e-
e-
EM field in terms of vector meson fields
e
?
V
e-
V? effective coupling
8
Isospin violation in ? ? ? ?0
I) EM process in VMD
9
Decompose the EM field in terms of vector mesons
in Process-I
10
?-?0-?0 coupling
KLOE Collaboration, PLB561, 55 (2003)
is dominated by ?0, we extract
Assuming
11
II) Isospin violation in strong decays
  • Physical vacuum is not invariant under chiral
    symmetries
  • Chiral symmetry is spontaneously broken
  • Goldstone boson
  • Chiral symmetry is explicitly broken
  • mu ? md
  • Manifestations
  • Light 0? octet mesons (Goldstone bosons), ?, K, ?
  • Strong isospin violation m(?0) lt m(??) m(K0) gt
    m(K?) m(p) lt m(n)

12
Strong transition in ? ? ? ?0
? (I0)
g
s
? (I0)
?0 (I1)
?s
OZI evading process
K? (u?s)
K0 (d?s)
? (I0)
s
K
? (I0)
?0 (I1)
?s
?K0 (s?d)
K? (s?u)
13
  • Strong isospin violation
  • via intermediate meson exchanges

If mu md, (a) (b) 0 and (c) (d)
0. If mu ? md, (a) (b) ? 0 and (c) (d) ?
0.
Li, Zhao and Zou, arXiv0706.0384hep-ph
14
Isospin violated effective couplings
15
  • t-channel versus s-channel

Previous approach
?
mixing
?
?
?
?-?0, ?-?0 mixing
?0
?0
This approach
?
?
?, VMD
?
?
?
t-channel
?0
?0
?0
16
Three schemes for the numerical calculations of
the intermediate meson exchange loops
1. On-shell approximation 2. Feynman integration
with a monopole form factor 3. Feynman
integration with a dipole form factor
17
1. On-shell approximation
0, No form factor n 1, monopole
2, dipole
? (GeV) to be determined by experimental data.
18
Numerical results
Experimental branching ratio
On-shell approximation underestimates the data.
Exclusive KK(K) loop
19
  • ?-dependence of the sum of EM and KK(K) loop

EM and KK(K) out of phase
EM and KK(K) in phase
Still underestimate the experimental data.
20
2. Feynman integration with a monopole form factor
?
Similarly for the neutral meson loop
21
  • ?-dependence of the exclusive KK(K) loop with a
    monopole form factor

22
  • ?-dependence of the exclusive KK(K) loop with a
    monopole form factor

23
3. Feynman integration with a dipole form factor
Exclusive KK(K) loop contribution to BR
24
Exclusive KK(K) loop contribution to BR
25
Inclusive contributions from the isospin
violating transitions
Isospin violation EM ? Strong decay loops
V ? V P is a P-wave decay, favors a dipole form
factor.
In phase
Out of phase
Exp.
Exp.
26
A Brief Summary
  • The correlation between the OZI-rule violation
    and strong isospin violations makes the
    intermediate meson exchange process a possible
    dynamic solution for the study of isospin
    violations in ? ? ? ?0.
  • It provides an explicit way to separate the EM
    and strong isospin violation mechanisms, thus, is
    different from meson mixing scheme.

27
  • Application to J/?, ? ? VP is useful for the
    study of ?? puzzle (Zhao, Li and Chang, PLB645,
    173(2007) ) and search for pseudoscalar glueball
    (Li, Zhao and Chang, hep-ph/0701020).
  • Application to the study of a0(980)-f0(980)
    mixing in J/?? ? a0(980) ? ???0 (Wu, Zhao and
    Zou, PRD 75, 114012 (2007) ).
  • Experimental focuses of BES, CLEO-c, KLOE,
    B-factories

28
Thanks !
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