Binding Energy effects in the Decay Properties of Charmonia

Binding Energy effects in the Binding Energy effects in the Decay Properties of CharmoniaDecay Properties of Charmonia Binding Energy effects in the Binding Energy effects in the

Decay Properties of CharmoniaDecay Properties of Charmonia

P C Vinodkumar

Department of Physics Sardar Patel University

Vallabh Vidyanagar-388 120, Gujarat, INDIA

Outline…

Introduction.

Spectroscopic Properties of Heavy Flavour Mesons in Coulomb plus Power Potential.

Decay Properties of Heavy Flavour Mesons.

Conclusion.

Introduction

3872

DD

[Bhavin Patel JPG 36, (2009)]

Di-gamma BR:

• The present study clearly indicates that the coulomb plus linear potential is not adequate enough to explain observed properties of charmonia.

• A stronger inter quark potential (confinement part of the potential; i.e, \nu~ 1.1) is required for the spectra.

• The E1 transition results from the present study support this observation as they match with the known experimental values near the potential index, \nu = 1.1.

• A similar conclusion from M1 transition warranted experimental supports.

• However, their digamma, dilepton, digluon decay occur at a weaker inter quark potential; i.e, \nu~ 0.7 to 0.8).

• It is also observed that there is an interplay between the quark mass parameter of the model and the confinement potential. The constituent quark mass no more found to be the same for the spectra and for the decay.

• The mass of the constituent quark do depend on the interaction process in which they are involved as well as on their partner.

Conclusions

Thanks

Dr. J N Pandya (MSU,Vadodara), Dr. J N Pandya (MSU,Vadodara), Dr. Ajay Kumar Rai (SVNIT, Surat),Dr. Ajay Kumar Rai (SVNIT, Surat),Dr. C J Clement (St. Xavier Sci. College, Ahmedabad),Dr. C J Clement (St. Xavier Sci. College, Ahmedabad),Dr. R H Parmar (Modasa Sci. College, Modasa)Dr. R H Parmar (Modasa Sci. College, Modasa)Dr. Bhavin K PatelDr. Bhavin K PatelMr. Ajay Majethiya (KITRC, Kalol),Mr. Ajay Majethiya (KITRC, Kalol),Ms. Shereena Joseph (Delhi),Ms. Shereena Joseph (Delhi),

Mr. Arpit Parmar and Mr. Kaushal ThakkarMr. Arpit Parmar and Mr. Kaushal Thakkar..

Part of this work is done with a financial support from DST, New Delhi, under a

Major Research Project SR/S2-HEP-20/2006.

To our research group :

To the organizers CSIR, New Delhi Sardar Patel University, Vallabh Vidyanagar

• The area that is phenomenologically understood extends to: Heavy-light mesons, states where the quark-antiquark pair is in relative S wave; Heavy-heavy meson: states below the DD (BB) threshold

• In the positive parity sector (P wave, L=1) a number of states have been discovered with masses and widths much different than expected from quark potential models.

Op

en c

har

m

DsJ(2632) (Selex)

DsJ*(2715) (Belle)

DsJ(2860) (Babar)

.......

DsJ*(2317)

- JP=0+

- P cs ~ 2.48 GeV

- < 4.6 MeV

DsJ(2460)

- JP=1+

- P cs ~ 2.55 GeV

- < 5.5 MeV

D0*(2308)

- JP=0+

- P cn ~ 2.46 GeV

- ~ 276 MeVC

har

mon

ium

X (3872)

- JPC=1++ (2–+)

- P cc ~ 3.9-4.0 GeV

- < 2.3 MeV

Y(4260) : ??

Y(4385) : 43S1,33D1

X (3940)

Y (3940):23PJ=1,2,3

Z (3940)

Light - heavy mesons sector Charmonia sector

– –

New open-charm and charmonium like states

Backup Slide

Challenges in Heavy Flavour Hadron Spectroscopy

Experimental Status