walaa i. eshraim in collaboration with

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Walaa I. Eshraim In collaboration with Stanislaus Janowski , Francesco Giacosa, and Dirk H. Rischke Institut Für Theoretische Physik Goethe Universität Frankfurt am Main

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Institut Für Theoretische Physik. Goethe Universität Frankfurt am Main. Walaa I. Eshraim In collaboration with Stanislaus Janowski , Francesco Giacosa , and Dirk H. Rischke eQCD 2012, Peniche, May 8. 2012. Decays of The Pseudoscalar Glueball into Scalar and Pseudoscalar Mesons. - PowerPoint PPT Presentation

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Page 1: Walaa I.  Eshraim In collaboration with

Walaa I. Eshraim In collaboration with

Stanislaus Janowski , Francesco

Giacosa, and Dirk H. Rischke

eQCD 2012, Peniche, May 8. 2012

Institut Für Theoretische Physik Goethe Universität Frankfurt am Main

Page 2: Walaa I.  Eshraim In collaboration with

Quantum chromodynamic (QCD) is the theory of the strong interactions.

QCD predicts colorless bound states of the gluons. (the glueballs).

A glueball is a hypothetical particle. It consists of solely gluon particles, without valence quarks.

Important for phenomenology.Glueballs are a solid Lattice QCD prediction.

Page 3: Walaa I.  Eshraim In collaboration with

Lattice QCD calculations

[C. Morningstar and M. J. Peardon, AIP Conf. Proc. 688, 220 (2004)

[arXiv:nucl-th/0309068]]

[Y. Chen et al., Phys. Rev. D 73, 014516 (2006)]

There is a pseudoscalar glueball, with the mass around 2.5 GeV predicted by lattice QCD calculation.

Ğ gg 0PCJ

Page 4: Walaa I.  Eshraim In collaboration with

Two experiments related to our work :

1.PANDA able to study energies above 2.5 GeV.

2.BESIII found a pseudoscalar glueball candidate with a mass of about 2.3 GeV.

Page 5: Walaa I.  Eshraim In collaboration with

†det det , intĞ ĞL ic Ğ

Ğc

( )a a aS i P t

( )fU N

† , (3) (3)L R R LU U SU SU but breaks (1)AU

Page 6: Walaa I.  Eshraim In collaboration with

3fN

0 00

0

0 00 00

0 0

( )

2

( )1

2 2

N NS

N NS

S S S S

a ia i K iK

a ia i K iK

K iK K iK i

[D. Parganlija, F. Giacosa, D. H. Rischke, P. Kovacs, and G. Wolf, Int. J. Mod. Phys. A 26 607-609 (2011) [arXiv 1009.2250 [hep-ph]].

Page 7: Walaa I.  Eshraim In collaboration with

��������������

2 N Suu dd and ss

cos sin

sin cos

36

N S

N S

owhere is the mixing angle

[K. Nakamura et al. (Particle Data Group), J. Phys. G 37, 075021 (2010).]

Page 8: Walaa I.  Eshraim In collaboration with

0a��������������

0a SK*0K

2 N Suu dd and ss

0f 0f,N S

Page 9: Walaa I.  Eshraim In collaboration with

N N N

, , 2N S S S S K KZ f Z f

,N S

1.66 , 1.39kZ Z

[D. Parganlija, F. Giacosa and D. H. Rischke, Phys. Rev. D 82, 054024 (2010) [arXiv:1003.4934 [hep-ph]].

[D. Parganlija thesis]

,N S

Page 10: Walaa I.  Eshraim In collaboration with

2.6Ğ

M GeV

Ğ gg 0PCJ

2.3gg

M GeV

2.3gg

M GeV gg gg

Page 11: Walaa I.  Eshraim In collaboration with

Results for A Results for B

Decay channel of the pseudoscalar glueball

Page 12: Walaa I.  Eshraim In collaboration with

FIG. 1: BLUE LINE: Total decay width of the pseudoscalar glueball with the bare mass b) RED DASHED LINE: Total decay width of the pseudoscalar glueball with the physical mass

2.6Ğ

M GeV

2.3 gg

M GeV

Page 13: Walaa I.  Eshraim In collaboration with

3fN

Page 14: Walaa I.  Eshraim In collaboration with