Abstract
The mass spectrum and decay modes of the (cc)-(anti canti c) states are estimated in a quark-gluon model. We argue that the peculiar resonance-like structures of R(e/sup +/e/sup -/ ..-->.. hadrons) for ..sqrt..s = 6 to 7 GeV may be due to production of the P-wave (cc)-(anti canti c) states. They are predicted to lie in the range 6.4 to 6.8 GeV and mainly decay into charmed mesons.
Chao, K T
[1]
- Fermi National Accelerator Lab., Batavia, IL (USA)
Citation Formats
Chao, K T.
(cc)-(anti canti c) (diquark-antidiquark) states in e/sup +/e/sup -/ annihilation.
Germany: N. p.,
1981.
Web.
Chao, K T.
(cc)-(anti canti c) (diquark-antidiquark) states in e/sup +/e/sup -/ annihilation.
Germany.
Chao, K T.
1981.
"(cc)-(anti canti c) (diquark-antidiquark) states in e/sup +/e/sup -/ annihilation."
Germany.
@misc{etde_6359345,
title = {(cc)-(anti canti c) (diquark-antidiquark) states in e/sup +/e/sup -/ annihilation}
author = {Chao, K T}
abstractNote = {The mass spectrum and decay modes of the (cc)-(anti canti c) states are estimated in a quark-gluon model. We argue that the peculiar resonance-like structures of R(e/sup +/e/sup -/ ..-->.. hadrons) for ..sqrt..s = 6 to 7 GeV may be due to production of the P-wave (cc)-(anti canti c) states. They are predicted to lie in the range 6.4 to 6.8 GeV and mainly decay into charmed mesons.}
journal = []
volume = {7:4}
journal type = {AC}
place = {Germany}
year = {1981}
month = {Jan}
}
title = {(cc)-(anti canti c) (diquark-antidiquark) states in e/sup +/e/sup -/ annihilation}
author = {Chao, K T}
abstractNote = {The mass spectrum and decay modes of the (cc)-(anti canti c) states are estimated in a quark-gluon model. We argue that the peculiar resonance-like structures of R(e/sup +/e/sup -/ ..-->.. hadrons) for ..sqrt..s = 6 to 7 GeV may be due to production of the P-wave (cc)-(anti canti c) states. They are predicted to lie in the range 6.4 to 6.8 GeV and mainly decay into charmed mesons.}
journal = []
volume = {7:4}
journal type = {AC}
place = {Germany}
year = {1981}
month = {Jan}
}