Scalar D mesons in nuclear matter

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Presentation transcript:

Scalar D mesons in nuclear matter Taesoo Song, Woosung Park, Kie Sang Jeong and Su Houng Lee (Yonsei Univ.)

Procedure Motivation 2. QCD sum rule in vacuum & in nuclear matter 3. Application to Scalar D mesons 4. Conclusions

1. Motivation Charm-strange scalar meson Ds0+(2317) was discovered in 2003 Its mass is too lower than the expected values in quark models and other theoretical predictions. It has been interpreted as the isosinglet state (conventional scalar meson), a four-quark state, a mixed state of both, a DK molecule, … Later charm scalar meson D0*(2400) with broad width was discovered in 2004 Its mass is similar to or larger than that of D+s0(2317), even though Ds(0-) is 100 MeV higher than D(0-).

2. QCD sum rule OPE (operator product expansion) Phenomenological side Dispersion relation Borel transformation

2. 1. OPE (operator product expansion)

As an example, may be ignored

Perturbative quark propagator in a weak gluonic background field (The gluons are supposed to emerge from the ground state)

Perturbative part I : dimension 0 Gluon condensates <G2> : dimension 4 and more condensates with higher dimension or more strong couplings

Quark condensate <qq> : dimension 3 Quark-gluon mixed condensates <qGq> : dimension 5 and more condensates with higher dimension or more strong couplings

OPE up to dimension 5 in vacuum , where C0 (q2) is perturbative part

OPE up to dimension 5 in nuclear matter

List of employed condensate parameters

2.2. Phenomenological side

2.3. Dispersion relation (in vacuum) L.H.S .is a function of QCD parameters such as g, mq, <qq>, <G2>…, obtained from OPE. R.H.S. is a function of physical parameters such as mλ and s0

Dispersion relation (in nuclear matter)

2.4. Borel transformation

3. Application to scalar D mesons Charm scalar meson D0* in vacuum Charm scalar meson D0* in nuclear matter Charm-strange scalar meson Ds0 in vacuum & in nuclear matter

3.1. Charm scalar meson D0* in vacuum From the dispersion relation , the mass of scalar D meson is

Borel window The range of M2 satisfying below two conditions 1) continuum/total < 0.3 / < 0.3 2) Power correction/total < 0.3 / <0.3

Borel curve for D0*(2400) in vacuum (adjust s0 to obtain flattest curve within Borel window) S0=7.7 GeV2

3.2. Charm scalar meson D0* in nuclear matter Two dispersion relations for πe and πo exist ≡f(s0+,s0-) ≡g(s0+,s0-)

iteration No. D+ s0 D+ mass D- s0　 D- mass 7.7 2.392 1 7.55 2.373 2 7.8 2.391 3 7.5 2.371 4

Mass shift of D0*±(2400) in nuclear matter (The conditions for Borel window are continuum/total<0.5 & power correction/total <0.5)

Physical interpretation of the result

3.3. Charm-strange scalar meson Ds0 in vacuum & in nuclear matter

Borel curves for Ds0 (2317) in vacuum (The conditions for Borel window are continuum/total<0.5 & power correction/total <0.5)

Mass shift of Ds0±(2317) in nuclear matter (The conditions for Borel window are continuum/total<0.5 & power correction/total <0.5) Nuclear density (0.17 nucleon/fm3) Nuclear density (0.17 nucleon/fm3)

4. Conclusion We successfully reproduced the mass of charm scalar meson D0* in vacuum and that of charm-strange scalar meson Ds0 by using QCD sum rule Based on this success, their mass shifts in the nuclear matter are estimated by considering the change of condensate parameters and adding new condensate parameters which do not exist in vacuum state. The mass of D0*+ decreases in the nuclear matter more than that of D0*-, as naively expected. But the mass of Ds0+ increases a little in the nuclear matter, while that of Ds0- decreases. The quark component of these scalar particles are still in question, whether they are conventional mesons or quark-quark states or their combinations or others. We expect that the behavior of their masses in nuclear matter serves to determine the exact quark component of those scalar particles.

4.1. Future work QCD sum rule for pseudoscalar D meson, which is the chiral partner of charm scalar meson – the mass difference between scalar and pseudoscalar meson is expected to decrease in nuclear matter due to the partial restoration of chiral symmetry. QCD sum rule for charm scalar meson as four quark state – The comparison of its mass shift in nuclear matter with that of conventional meson will reveal the exact component of charm scalar meson.