SCALAR MESONS IN QCD Stephan Narison CNRS - Montpellier HEPMAD07, - - PowerPoint PPT Presentation

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SCALAR MESONS IN QCD Stephan Narison CNRS - Montpellier HEPMAD07, - - PowerPoint PPT Presentation

SCALAR MESONS IN QCD Stephan Narison CNRS - Montpellier HEPMAD07, Antananarivo (10-15th September 2007) p. 1/5 Light Hadrons Spectroscopy Light Quarks: u,d,s : m q QCD 350 MeV ; Q u = 2 / 3; Q d = Q s = 1 / 3 HEPMAD07,


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SLIDE 1

SCALAR MESONS IN QCD

Stephan Narison

CNRS - Montpellier

HEPMAD07, Antananarivo (10-15th September 2007) – p. 1/5

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SLIDE 2

Light Hadrons Spectroscopy

♣ Light Quarks:

u,d,s : mq ≤ ΛQCD ≈ 350 MeV;

Qu = 2/3;Qd = Qs = −1/3

HEPMAD07, Antananarivo (10-15th September 2007) – p. 2/5

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SLIDE 3

Light Hadrons Spectroscopy

♣ Light Quarks:

u,d,s : mq ≤ ΛQCD ≈ 350 MeV;

Qu = 2/3;Qd = Qs = −1/3 ♦ Light Baryons

proton= uud; neutron= udd,...

HEPMAD07, Antananarivo (10-15th September 2007) – p. 2/5

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SLIDE 4

Light Hadrons Spectroscopy

♣ Light Quarks:

u,d,s : mq ≤ ΛQCD ≈ 350 MeV;

Qu = 2/3;Qd = Qs = −1/3 ♦ Light Baryons

proton= uud; neutron= udd,...

♥ Light Ordinary Mesons π−≡ ¯ ud : JPC = 0−+; ρ−≡ ¯ ud : JPC = 1−−; A1≡ ¯ ud : JPC = 1++

Well understood in QCD : associated resp. to the pseudoscalar, vector and axial-vector currents.

HEPMAD07, Antananarivo (10-15th September 2007) – p. 2/5

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SLIDE 5

Scalar Mesons

➳ Long standing puzzle

  • Difficult to identify experimentally :

too wide (σ) or near the ¯ KK threshold (a0).

HEPMAD07, Antananarivo (10-15th September 2007) – p. 3/5

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SLIDE 6

Scalar Mesons

➳ Long standing puzzle

  • Difficult to identify experimentally :

too wide (σ) or near the ¯ KK threshold (a0).

  • Can be produced from: φ, J/ψ, ϒ, B and D - decays

γγ, ππ and πN scatterings

HEPMAD07, Antananarivo (10-15th September 2007) – p. 3/5

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SLIDE 7

Scalar Mesons

➳ Long standing puzzle

  • Difficult to identify experimentally :

too wide (σ) or near the ¯ KK threshold (a0).

  • Can be produced from: φ, J/ψ, ϒ, B and D - decays

γγ, ππ and πN scatterings

  • Different interpretations
  • ordinary ¯

qq

  • four-quark states
  • gluon bound states for the I=0

HEPMAD07, Antananarivo (10-15th September 2007) – p. 3/5

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SLIDE 8

¯ qq and gluonium interpretations

➳ I=1 scalar : a0(980), κ(800)

  • Can be explained as ¯

qq states : associated to the

divergence of the QCD vector current : JS = (mi −m j) ¯ ψi(i) ¯ ψj

HEPMAD07, Antananarivo (10-15th September 2007) – p. 4/5

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SLIDE 9

¯ qq and gluonium interpretations

➳ I=1 scalar : a0(980), κ(800)

  • Can be explained as ¯

qq states : associated to the

divergence of the QCD vector current : JS = (mi −m j) ¯ ψi(i) ¯ ψj

➳ I=0 scalar : σ(800), f0(980)

  • Can be explained as 1/2 ¯

qq and 1/2 gluonium states : associated to Trace of the QCD energy-momentum

tensor current : Θµ

µ = ∑m j ¯

ψj ¯ ψj +(1/4)β(αs)G2.

HEPMAD07, Antananarivo (10-15th September 2007) – p. 4/5

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SLIDE 10

Using QCD Spectral Sum Rules

HEPMAD07, Antananarivo (10-15th September 2007) – p. 5/5

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SLIDE 11

Using QCD Spectral Sum Rules

Introduced by Shifman-Vainshtein-Zakharov

HEPMAD07, Antananarivo (10-15th September 2007) – p. 5/5

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SLIDE 12

Using QCD Spectral Sum Rules

Introduced by Shifman-Vainshtein-Zakharov Improved dispersion relation :

duality between measured and QCD observables

HEPMAD07, Antananarivo (10-15th September 2007) – p. 5/5

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SLIDE 13

Using QCD Spectral Sum Rules

Introduced by Shifman-Vainshtein-Zakharov Improved dispersion relation :

duality between measured and QCD observables

SN-Veneziano 88, Bramon-SN 89

HEPMAD07, Antananarivo (10-15th September 2007) – p. 5/5

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SLIDE 14

Using QCD Spectral Sum Rules

Introduced by Shifman-Vainshtein-Zakharov Improved dispersion relation :

duality between measured and QCD observables

SN-Veneziano 88, Bramon-SN 89 SN 84, 96, 2005

HEPMAD07, Antananarivo (10-15th September 2007) – p. 5/5

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SLIDE 15

Using QCD Spectral Sum Rules

Introduced by Shifman-Vainshtein-Zakharov Improved dispersion relation :

duality between measured and QCD observables

SN-Veneziano 88, Bramon-SN 89 SN 84, 96, 2005 Dosch-SN 2000

HEPMAD07, Antananarivo (10-15th September 2007) – p. 5/5

slide-16
SLIDE 16

Using QCD Spectral Sum Rules

Introduced by Shifman-Vainshtein-Zakharov Improved dispersion relation :

duality between measured and QCD observables

SN-Veneziano 88, Bramon-SN 89 SN 84, 96, 2005 Dosch-SN 2000 Minkowski-Mennessier-SN-Ochs 2007

HEPMAD07, Antananarivo (10-15th September 2007) – p. 5/5