Title: Light scalars as tetraquark states
1Light scalars as tetraquark states
- Francesco Giacosa
- Hirschegg
- 18/01/07
2Francesco Giacosa
Scalar Quest
- Outline
- Problems of the light scalar mesons
- Interpretation of the light scalar mesons
interpreted as tetraquark-states (Strong and e.m.
decays, hadronic d.o.f) - Mixing of tetraquark and quarkonia
configurations - Outlook and Summary
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Scalar Quest
Scalar Mesons below 1.8 GeV listed in PDG
M lt 1 GeV 1
GeV lt M lt 1.8 GeV
Too many resonances than expected from
quark-antiquark states
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Francesco Giacosa
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M lt 1 GeV
interpretation
Assignement has problems!!!
5List of Problems
Francesco Giacosa
Scalar Quest
- Masses degeneracy of and
- Strong coupling of to
- The scalar quarkonia are p-wave states (L S
1), thus expected to be heavier than 1 GeV as
tensor and axial-vector mesons - Some Lattice results find
- Large behavior of light scalar not
compatible with quarkonia
from Prelovsek et al., Phys. Rev. D 70 (2004),
Burch et al., Phys. Rev. D 73 (2006)
from Pelaez, Phys. Rev. Lett. (2004),
Pelaez and Rios, hep-ph/0610397
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Tetraquark interpretation
- Jaffes four-quark states can
explain the scalar states below 1 GeV
- Out of a diquark and an anti-diquark one can
build a nonet of four-quark states with suitable
characteristics
- A spinless diquark in the flavor and color
antisymmetric combination (good diquark) forms a
compact object - (1-gluon exchange, instantons, NJL, DSE)
Example of a good diquark
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Under SU(3)-flavor the 3 diquarks behave like
antiquarks
Example
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M lt 1 GeV
Tetraquark interpretation
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Previous works and motivations
Strong decays of a tetraquark state
Jaffe-orig Jaffe, Phys. Rev. D 15 (1977),
Bugg-06 hep-ex/0603089 Maiani Maiani et al,
Phys. Rev. Lett. (2004)
Systematic evaluation of amplitudes My work
Giacosa, Phys. Rev. D 74 (2006)
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Strong decays within a hadronic model (never see
quarks and gluons, only hadrons)
Nonet of pseduoscalar states
Nonet of scalar tetraquark states
The phys. resonances result from mixing
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Write the flavor, P, C invariant interaction
Lagrangian for the scalar 4q decays
The trace structure corresponds to the
microscopic diagrams
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Decay amplitudes as functions of dominant and
subdominant constants
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(Bugg06)
Non-trivial agreement then all the other ratios
are determined
Imp without the subdmominant one has
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For the two-photon decays proceed in a similar
way
Outlook decay of (and into) vector mesons.
Through VMD no new parameters.
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M lt 1 GeV 1
GeV lt M lt 2 GeV
These are 4q-states!!!
These are quarkonia (with glueball-intrusion)!!!
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Extension tetraquark-quarkonia mixing (sketch)
- Scalar tetraquark and quarkonia states can mix
- (Black et al, Phys. Rev. D 64 (2001),
Fariborz et al. Phys. Rev. D 72 (2005) ) - Extension of the model
consider scalar and
pseudoscalar quarkonia meson and scalar
tetraquark states (Giacosa, hep-ph/0611388)
P, S
P, S
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Mixing in the isovector sector
In particular
One relates the tetraquark-decay parameters to
the mixing strenght then, one can evaluate the
mixing
The mixing is small !!!
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- Summary
- Scenario light scalars lt 1 GeV as 4q-states,
scalars between 1-1.8 GeV as quarkoniaglueball - Strong and e.m. decays (outlook about vector
mesons) - My last result mixing of 4q and quarkonium
occurs but it is small. - Understanding of the scalar sector lt 2 GeV is
important to study the decay of states in the
charmonia region.
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Thank you very much!!!