Gluonic hadrons and charmless B decays Page: 4 of 4
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Table 1: Some possible experimentally accessible final states of J'O exotic charmed
hybrids and glueballs below D"D threshold. Note that open charm modes of 4
may be suppressed by a selection rule [4]. For hidden charm modes, the charmonia
tend to have the same C as that of the parent R,. The light hadron modes are
expected to be enhanced for 0, with C = +. See the main text for details. Decays
to pp{7r, , w, p, } are allowed for all states listed.
JPC Open charm Hidden charm Light hadrons
0+- Quantum J/O{fjo,ta,, (irr)s} ae.1.21p; afia{b1,7}
numbers hui; ikh bir; h1'73
forbid xCew {(rx)s,fo}{w,4'}
D(')D() Xe2a){whi, 7} f(1,1fw, hi,4, }
0-- D'D h.(rr)s a{o,1.}bi; a{i,2)(P,'7}
J/1#{f(1,2),1 } Pr
Xmehi; rk{w,0} fohi; 171{4,#}
Xe i,2) {w, h1, 7} f(1,2) {w, hi, 0,'y}
1-+ D*D, D*D' Xc(o.1,)(zr)s na1,i1ja{o,,2; a81,2)r
17e{f{1,2)C}, f( /0.,2)}f{0,1.1; f(1,2)t)
Xela)f (p,y}{p,bi}; bib,
(he, J/4}{w, hi, O, 7} {w, hi, ,7){w, hi, 4,7}
2+ D*D, D*D {h.,J/1}{f(0,1,2},(rr)s) aoij}{p,bi,-t}
{h., J/}fr) {p, 7, b}r
{r(., Xgeui.) }{w, hi, , '71} {'), f(,l,2)}{-, hi, 0',y1Table 2: Glueball masses in GeV in the 3 - 4.5 GeV mass range accessed by B -r
K(*)+glueball, according to lattice gauge theory [30]. The 0-- glueball mass is
poorly determined. No JP0 exotic glueballs are expected below 3 GeV.
JPc )+- 2-+ 3++ 1++ 2-- 1--
Mass 2.9 0.3 3.0 0.2 3.9 0.5 4.0 0.3 4.0 0.4 4.6 0.5
JPC 1-+ 0+- 2+-
Mass $ 4.1 < 3.7 3.9 t 0.712
11
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Close, F.E.; Dunietz, I.; Page, P.R.; Veseli, S. & Yamamoto, H. Gluonic hadrons and charmless B decays, article, August 1, 1997; Newport News, Virginia. (https://digital.library.unt.edu/ark:/67531/metadc703815/m1/4/: accessed April 18, 2024), University of North Texas Libraries, UNT Digital Library, https://digital.library.unt.edu; crediting UNT Libraries Government Documents Department.