How to understand the X(2900)?
In this work, the S - and P -wave D ¯ ∗ K ∗ interactions are studied in a coupled-channel formalism to understand the recently observed X 0 ( 2900 ) and X 1 ( 2900 ) at LHCb. The experimental event distributions can be well described, and two states with I ( J P ) = 0 ( 0 + ) and 0 ( 1 - ) are yield...
Gespeichert in:
Veröffentlicht in: | The European physical journal. C, Particles and fields Particles and fields, 2022-05, Vol.82 (5), p.1-8, Article 419 |
---|---|
Hauptverfasser: | , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | In this work, the
S
- and
P
-wave
D
¯
∗
K
∗
interactions are studied in a coupled-channel formalism to understand the recently observed
X
0
(
2900
)
and
X
1
(
2900
)
at LHCb. The experimental event distributions can be well described, and two states with
I
(
J
P
)
=
0
(
0
+
)
and
0
(
1
-
)
are yielded in a unified framework. The masses of the
0
+
and
1
-
states are consistent with the experimental data, but the width of the
0
+
state is larger than that of the
1
-
one. The
X
1
(
2900
)
can be interpreted as the
P
-wave excitation of the ground-state
X
0
(
2900
)
in the hadronic molecular picture. The
S
- and
P
-wave multiplets in the
D
¯
∗
K
∗
system have many members, so the present peak in the
D
-
K
+
invariant mass distributions might contain multi substructures. |
---|---|
ISSN: | 1434-6052 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-022-10396-9 |