Chiral quark model for meson production in the resonance region … · 2010. 9. 1. · Chiral quark...
Transcript of Chiral quark model for meson production in the resonance region … · 2010. 9. 1. · Chiral quark...
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Qiang Zhao
Institute of High Energy Physics, CAS
and Theoretical Physics Center for Science
Facilities (TPCSF), CAS
Chiral quark model for meson
production in the resonance region
July 30, 2010, Beijing
Institute of High Energy Physics, CAS
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Outline
The “missing baryon resonances” problem
Effective chiral Lagrangian for quark-
pseudoscalar-meson interaction
Baryon resonances in pseudoscalar meson
photoproduction and meson-nucleon
scatterings
Prospects
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• The non-relativistic constituent quark model (NRCQM) makes
great success in the description of hadron spectroscopy:
meson (qq), baryon (qqq).
• However, it also predicted a much richer baryon spectrum, where
some of those have not been seen in N scatterings.
– “Missing Resonances”.
, 0
N, ½+
N*, L2I,2J
P33(1232)
P11(1440)
S11(1535)
D13(1520)
…
1. “Missing baryon resonances in N scattering
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PDG2008: 22 nucleon resonances (uud, udd)
(**) not well-
established
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Dilemma:
a) The NRCQM is WRONG: quark-diquark configuration? …
b) The NRCQM is CORRECT, but those missing states have only weak
couplings to N, i.e. small gN*N. (Isgur, 1980)
Looking for “missing resonances” in N* N, K, K, N, N, N,
N …
(Exotics …)
N* uud
d
d
u
ud
n
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Questions:
Should we take the naïve quark model seriously?
What is the success and what is the failure?
… …
How far one can go with it?
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The first orbital excitation states in the NRCQM
In the nonstrange sector, NRCQM allows the
groundstate [56, 28] (p and n) to be excited
to [70, 28] and [70, 48] octets, and [70, 210]
decuplet via single photon absorption.
N
EM
N*,*
Confirmed recently by JLab Lattice calculation.
(Talk by D. Richards in MENU2010)
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The SU(6)O(3) symmetry must be broken due to spin-
dependent forces. Thus, state mixings are inevitable.
Several NRCQM selection rules are violated:
• Moorhouse selection rule (Moorhouse, PRL16, 771 (1966))
• selection rule (Zhao & Close, PRD74, 094014(2006)) in strong decays
• Faiman-Hendry selection rule (Faiman & Hendry, PR173, 1720 (1968)).
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An effective chiral Lagrangian for quark-pseudoscalar-meson coupling
to keep the meson-baryon interaction invariant under the chiral
transformation:
2. Effective chiral Lagrangian for quark-pseudoscalar-
meson interactions
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• Test of Goldberger-Treiman relation:
The axial vector coupling, gA, relates the hadronic operator to the
quark operator j for the j-th quark,
To equate the quark-level coupling to the hadronic level one for the
NN vertex, i.e. axial current conservation, one has
Ni Nf
NiNf
Ni Nf
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Baryon excitations in p n
Zhong, Zhao, He, and Saghai, PRC76, 065205 (2007);
Zhong and Zhao, Phys. Rev. C 79, 045202 (2009)
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, q, k
N, Pi N, Pf
, k , q
N, PfN, Pi
+N()
() N()
()
s-channel
Refs.
Zhao, Li, & Bennhold, PLB436, 42(1998); PRC58, 2393(1998);
Zhao, Didelez, Guidal, & Saghai, NPA660, 323(1999);
Zhao, PRC63, 025203(2001);
Zhao, Saghai, Al-Khalili, PLB509, 231(2001);
Zhao, Al-Khalili, & Bennhold, PRC64, 052201(R)(2001); PRC65, 032201(R) (2002);
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, k
N, PiN, Pf
, q
+
, q, k
N, PiN, PfN()
() N()
()
u-channel
, k , q
N, Pi N, Pf
a0
t-channel
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S-channel transition amplitude with quark level operators
Non-relativistic expansion:
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with
, q, k
N, Pi N, PfN()
()
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with
, q, k
N, Pi N, PfN()
()
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quark level hadron level
Define g-factors:
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, q, k
N, Pi N, Pf
, k , q
N, PfN, Pi
+N()
() N()
()
s-channel
Compared with Ms3, amplitude Ms
2 is relatively suppressed by a factor
of (-1/2)n for each n.
Higher excited states are relatively suppressed by (kq/32)n/n!
One can identify the quark motion correlations between the initial and
final state baryon
Similar treatment can be done for the u channel
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Separate out individual resonances
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In the SU(6) symmetry limit,
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Goldberger-Treiman relation:
Model parameters
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Differential cross sections
Left panel: Solid: full calculation
Dot-dashed: without nucleon
Born term
Right panel: Solid: full calculation
Dotted lines: exclusive S11(1535)
Dot-dashed: without S11(1650)
Dashed: without t-channel
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Left panel: Solid: full calculation
Dot-dashed: without nucleon
Born term
Dashed: without D13(1520)
Right panel: Solid: full calculation
Dotted lines: exclusive S11(1535)
Dot-dashed: without S11(1650)
Dashed: without t-channel
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Total cross sections
S11(1535) is dominant near
threshold. The exclusive cross
section is even larger than the
data.
S11(1650) has a destructive
interference with the S11(1535),
and appears to be a dip in the
total cross section.
States from n=2 shell
account for the second
enhancement around 1.7 GeV.
Zhong, Zhao, He, and Saghai,
PRC76, 065205 (2007)
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S-channel resonance excitations in K–p 0 0
Zhong and Zhao, PRC79, 045202 (2009)
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We thus determine the mixing angle by experimental data which
requires
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Diff. Xsect. for K–p 0 0
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s-channel
=0
is the only s-channel amplitude
K– (su)
p
U-channel turns to be important
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Quark-photon electromagnetic coupling:
Transition amplitudes in terms of the Mandelstam variables:
Zhao et al, PRC65, 065204 (2002)
Baryon excitations in meson photoproduction
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The seagull term is composed of two parts,
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Transition amplitudes in the harmonic oscillator basis
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Compared with Ms3, amplitude Ms
2 is
relatively suppressed by a factor of (-1/2)n
for each n.
Higher excited states are relatively
suppressed by (kq/32)n/n!.
One can identify the quark motion
correlations between the initial and final
state baryon.
Similar treatment can be done for the u
channel.
In principle, all the s- and u-channel
states have been included in the
amplitudes, and the quark level operators
have been related to the hadronic level
ones through g-factors defined as follows.
Then, one has to separate out the
amplitudes for each single resonance (see
Ref. Zhao et al, PRC65, 065204 (2002) ).
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Some numerical results for pion photoproduction
magnetic dipole moment:
Zhao et al, PRC65, 065204 (2002)
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Differential cross sections for
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Polarized beam asymmetry for
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Polarized target asymmetry for
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Recoil polarization asymmetry for
Simultaneous account for p 0 p and n p reaction and
other relevant reactions.
Zhao et al, PRC65, 065204 (2002)
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M (,, K …)
N N (N, , …)
EM StrongN*,*
n N* K
n N* (*) N 27 states
p N* (*) N 19 states
n N* N
p N* N
16 states
8 states
p N* K 8 states
Due to selection rule
Number of states with the principle quantum number n 2:
Selection rule: Zhao & Close, PRD74, 094014(2006)
Difference due to Moorhouse
section rule
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Prospects - I
1. For the purpose of searching for individual resonance
excitations, it is essential to have a quark model guidance for
both known and “missing” states. And then allow the data to
tell:
i) which state is favored;
ii) whether a state beyond the conventional quark model is
needed;
iii) how quark model prescriptions for N*NM form factors
complement with isobaric models.
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Prospects - II
2. Understanding the non-resonance background
A reliable estimate of the non-resonance background, such as the
t- and u-channel. Their interferences with the resonances are
essentially important.
3. Unitarity constraint
A coherent study of the pseudoscalar photoproduction and meson-
baryon scattering is needed. In particular, a coupled channel study
will put a unitary constraint on the theory.
Photoproduction of pseudoscalar mesons (, , , K); and N N;
Kp , and more are coming out soon…
Q. Z., PRC 63, 035205 (2001) ;
Q. Z., J.S. Al-Khalili, Z.P. Li, and R.L. Workman, PRC 65, 065204 (2002);
Q. Z., B. Saghai and Z.P. Li, JPG 28, 1293 (2002);
X.H. Zhong, Q. Z., J. He, and B. Saghai, PRC 76, 065205 (2007)
X.H. Zhong and Q. Z., arXiv:0811.4212, PRC79, 045202(2009)
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Thanks !
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A revisit to the S-wave state mixing
, , K …
N, , …
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, , K …
N, , …
S11(1535) S11(1650)
0
The physical states should be orthogonal which means:
This expectation can be examined by the K-matrix propagator between
[70, 2 8] and [70, 4 8] mixing states:
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Recalling that
The N* NM transition amplitudes can be expressed as
with
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We can then extract the N*NM form factors given by the chiral effective
Lagrangian in the NRCQM, e.g.
where
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N threshold
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Relative signs for the N*NM couplings are given by the NRCQM
Indication of a destructive sign between S11(1535) and
S11(1650) amplitudes in p p, and p n.
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arXiv: 0810.0997[nucl-th] by Aznauryan, Burkert and Lee.
It is important to have a correct definition of the common sign
of amplitudes and relative sign between helicity amplitudes, i.e.
A1/2, A3/2, and S1/2.
N*
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p S11 (1535): 3q picture
Opposite sign
of S1/2!!!
LF RQM:
Capstick, Keister,PR D51 (1995) 3598
Pace, Simula et.al.,
PR D51 (1995) 3598
Combined with the difficultiesin the description of large width of S11(1535) N and largeS11(1535) N,K couplings, this shows that 3q picture for S11(1535) should be complemented
Impossible to change
in quark model !!!
From I. Aznauryan, Electromagnetic N-N*
Transition Form Factors Workshop, 2008
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