1 / 69

Binding Energy effects in the Decay Properties of Charmonia

Binding Energy effects in the Decay 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.

duyen
Download Presentation

Binding Energy effects in the Decay Properties of Charmonia

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Binding Energy effects in the Decay Properties of Charmonia P C Vinodkumar Department of Physics Sardar Patel University Vallabh Vidyanagar-388 120, Gujarat, INDIA

  2. Outline… • Introduction. • Spectroscopic Properties of Heavy Flavour Mesons in Coulomb plus Power Potential. • Decay Properties of Heavy Flavour Mesons. • Conclusion.

  3. Introduction

  4. 3872 DD

  5. [Bhavin Patel JPG 36, (2009)]

  6. Di-gamma BR:

  7. Conclusions • 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.

  8. Thank you

  9. Thanks • To our research group : Dr. J N Pandya (MSU,Vadodara), Dr. Ajay Kumar Rai (SVNIT, Surat), Dr. C J Clement (St. Xavier Sci. College, Ahmedabad), Dr. R H Parmar (Modasa Sci. College, Modasa) Dr. Bhavin K Patel Mr. Ajay Majethiya (KITRC, Kalol), Ms. Shereena Joseph (Delhi), Mr. Arpit Parmar and Mr. Kaushal Thakkar. • To the organizers • CSIR, New Delhi • Sardar Patel University, Vallabh Vidyanagar Part of this work is done with a financial support from DST, New Delhi, under a Major Research Project SR/S2-HEP-20/2006.

  10. New open-charm and charmonium like states • 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. Light - heavy mesons sector Charmonia sector DsJ*(2317) - JP=0+ • P cs ~ 2.48 GeV •  < 4.6 MeV DsJ(2460) - JP=1+ • P cs ~ 2.55 GeV •  < 5.5 MeV X (3872) - JPC=1++ (2–+) • P cc ~ 3.9-4.0 GeV •  < 2.3 MeV Y(4260) : ?? Y(4385) : 43S1,33D1 Open charm Charmonium D0*(2308) - JP=0+ • P cn ~ 2.46 GeV •  ~ 276 MeV DsJ(2632) (Selex) DsJ*(2715) (Belle) DsJ(2860) (Babar) ....... X (3940) Y (3940):23PJ=1,2,3 Z (3940) – –

  11. Backup Slide

More Related