Mini-workshop on “$T_{cc}^+$ and beyond”, Online
Tuesday, 14 September 2021 -
12:00
Monday, 13 September 2021
Tuesday, 14 September 2021
13:00
Welcome
Welcome
13:00 - 13:05
13:05
$T_{cc}^+$: now + next steps
-
Vanya Belyaev
(
NRC "Kurchatov Institute" (ITEP) (RU)
)
$T_{cc}^+$: now + next steps
Vanya Belyaev
(
NRC "Kurchatov Institute" (ITEP) (RU)
)
13:05 - 13:30
13:30
Beyond $T_{cc}^+$ : $T_{bb}$, $T_{bc}$, ...
-
Steven R. Blusk
(
Syracuse University (US)
)
Beyond $T_{cc}^+$ : $T_{bb}$, $T_{bc}$, ...
Steven R. Blusk
(
Syracuse University (US)
)
13:30 - 14:00
14:00
What can we learn from the width of the $T_{cc}^+$ tetraquark?
-
Mitja Rosina
What can we learn from the width of the $T_{cc}^+$ tetraquark?
Mitja Rosina
14:00 - 14:20
The width of the $T_{cc}^+$ tetraquark (dimeson) is expected to differ considerably from the widths of its constituent $D^{*0}$ and $D^{*+}$. Unfortunately, reliable values of the $D^{*0}$ and $T_{cc}^+$ widths are not yet known and at least theoretical estimates would be welcome. An interesting effect is due to the charge splitting of the $(D^{*+})D^0$ and $(D^{*0})D^+$ thresholds, therefore $T_{cc}^+$ will not have a pure isospin coupling $T_{cc}^+ = [(D^{*+})D^0 - (D^{*0})D^+]/\sqrt{2}$ and the actual composition may be seen in branching ratios. The width of $T_{cc}^+$ may depend strongly on threshold effects since its energy is not discrete and its peak extends beyond the lowest threshold, making it partially unstable and therefore broader. I shal try to estimate some of these effects.
14:20
$T_{cc}^+$ and its cousins
-
Marek Karliner
$T_{cc}^+$ and its cousins
Marek Karliner
14:20 - 14:50
14:50
Triangle singularities in the production of $T_{cc}^+$ and a soft pion
-
Eric Braaten
Triangle singularities in the production of $T_{cc}^+$ and a soft pion
Eric Braaten
14:50 - 15:20
15:20
Coffee/tea break
Coffee/tea break
15:20 - 15:40
15:40
Generality of near-threshold structures and a survey of hidden-charm and double-charm hadronic molecules
-
Feng-Kun Guo
(
Insitute of Theoretical Physics, Chinese Academy of Sciences
)
Generality of near-threshold structures and a survey of hidden-charm and double-charm hadronic molecules
Feng-Kun Guo
(
Insitute of Theoretical Physics, Chinese Academy of Sciences
)
15:40 - 16:10
16:10
Heavy tetraquark states from Lattice QCD
-
Nilmani Mathur
Heavy tetraquark states from Lattice QCD
Nilmani Mathur
16:10 - 16:30
16:30
$T_{cc}$ and its heavier cousins: Structure and binding in lattice QCD
-
Randy Lewis
(
York University
)
Anthony Sebastian Francis
(
Universitaet Bern (CH)
)
$T_{cc}$ and its heavier cousins: Structure and binding in lattice QCD
Randy Lewis
(
York University
)
Anthony Sebastian Francis
(
Universitaet Bern (CH)
)
16:30 - 16:50
16:50
Some reflections on tetraquarks and molecules
-
Antonio Polosa
(
Sapienza Universita e INFN, Roma I (IT)
)
Antonio Polosa
(
Universita' La Sapienza, Roma - Italy
)
Some reflections on tetraquarks and molecules
Antonio Polosa
(
Sapienza Universita e INFN, Roma I (IT)
)
Antonio Polosa
(
Universita' La Sapienza, Roma - Italy
)
16:50 - 17:20
17:20
Stability of the double-heavy tetraquark: lessons from atomic physics
-
Jean-Marc Rene Richard
(
Centre National de la Recherche Scientifique (FR)
)
jean-marc Richard
(
IPNL
)
Stability of the double-heavy tetraquark: lessons from atomic physics
Jean-Marc Rene Richard
(
Centre National de la Recherche Scientifique (FR)
)
jean-marc Richard
(
IPNL
)
17:20 - 17:40
17:40
Closing remarks
-
Marco Pappagallo
(
Universita e INFN, Bari (IT)
)
Closing remarks
Marco Pappagallo
(
Universita e INFN, Bari (IT)
)
17:40 - 17:50