New LHCb pentaquarks as hadrocharmonium states
New LHCb Collaboration results on pentaquarks with hidden charm1 are discussed. These results fit nicely in the hadrocharmonium pentaquark scenario. 2 , 3 , In the new data the old LHCb pentaquark P c ( 4 4 5 0 ) splits into two states P c ( 4 4 4 0 ) and P c ( 4 4 5 7 ) . We interpret these two alm...
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| Published in | Modern physics letters A Vol. 35; no. 18; p. 2050151 |
|---|---|
| Main Authors | , , |
| Format | Journal Article |
| Language | English |
| Published |
Singapore
World Scientific Publishing Company
14.06.2020
World Scientific Publishing Co. Pte., Ltd |
| Subjects | |
| Online Access | Get full text |
| ISSN | 0217-7323 1793-6632 |
| DOI | 10.1142/S0217732320501515 |
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| Abstract | New LHCb Collaboration results on pentaquarks with hidden charm1 are discussed. These results fit nicely in the hadrocharmonium pentaquark scenario.
2
,
3
,
In the new data the old LHCb pentaquark
P
c
(
4
4
5
0
)
splits into two states
P
c
(
4
4
4
0
)
and
P
c
(
4
4
5
7
)
. We interpret these two almost degenerated hadrocharmonium states with
J
P
=
1
/
2
−
and
J
P
=
3
/
2
−
, as a result of hyperfine splitting between hadrocharmonium states predicted in Ref. 2. It arises due to QCD multipole interaction between color-singlet hadrocharmonium constituents. We improve the theoretical estimate of hyperfine splitting
2
,
3
that is compatible with the experimental data. The new
P
c
(
4
3
1
2
)
state finds a natural explanation as a bound state of
χ
c
0
and a nucleon, with
I
=
1
/
2
,
J
P
=
1
/
2
+
and binding energy 42 MeV. As a bound state of a spin-
0
meson and a nucleon, hadrocharmonium pentaquark
P
c
(
4
3
1
2
)
does not experience hyperfine splitting. We find a series of hadrocharmonium states in the vicinity of the wide
P
c
(
4
3
8
0
)
pentaquark that can explain its apparently large decay width. We compare the hadrocharmonium and molecular pentaquark scenarios and discuss their relative advantages and drawbacks. |
|---|---|
| AbstractList | New LHCb Collaboration results on pentaquarks with hidden charm1 are discussed. These results fit nicely in the hadrocharmonium pentaquark scenario.2,3, In the new data the old LHCb pentaquark Pc(4450) splits into two states Pc(4440) and Pc(4457). We interpret these two almost degenerated hadrocharmonium states with JP = 1/2− and JP = 3/2−, as a result of hyperfine splitting between hadrocharmonium states predicted in Ref. 2. It arises due to QCD multipole interaction between color-singlet hadrocharmonium constituents. We improve the theoretical estimate of hyperfine splitting2,3 that is compatible with the experimental data. The new Pc(4312) state finds a natural explanation as a bound state of χc0 and a nucleon, with I = 1/2, JP = 1/2+ and binding energy 42 MeV. As a bound state of a spin-0 meson and a nucleon, hadrocharmonium pentaquark Pc(4312) does not experience hyperfine splitting. We find a series of hadrocharmonium states in the vicinity of the wide Pc(4380) pentaquark that can explain its apparently large decay width. We compare the hadrocharmonium and molecular pentaquark scenarios and discuss their relative advantages and drawbacks. New LHCb Collaboration results on pentaquarks with hidden charm1 are discussed. These results fit nicely in the hadrocharmonium pentaquark scenario. 2 , 3 , In the new data the old LHCb pentaquark P c ( 4 4 5 0 ) splits into two states P c ( 4 4 4 0 ) and P c ( 4 4 5 7 ) . We interpret these two almost degenerated hadrocharmonium states with J P = 1 / 2 − and J P = 3 / 2 − , as a result of hyperfine splitting between hadrocharmonium states predicted in Ref. 2. It arises due to QCD multipole interaction between color-singlet hadrocharmonium constituents. We improve the theoretical estimate of hyperfine splitting 2 , 3 that is compatible with the experimental data. The new P c ( 4 3 1 2 ) state finds a natural explanation as a bound state of χ c 0 and a nucleon, with I = 1 / 2 , J P = 1 / 2 + and binding energy 42 MeV. As a bound state of a spin- 0 meson and a nucleon, hadrocharmonium pentaquark P c ( 4 3 1 2 ) does not experience hyperfine splitting. We find a series of hadrocharmonium states in the vicinity of the wide P c ( 4 3 8 0 ) pentaquark that can explain its apparently large decay width. We compare the hadrocharmonium and molecular pentaquark scenarios and discuss their relative advantages and drawbacks. New LHCb Collaboration results on pentaquarks with hidden charm 1 are discussed. These results fit nicely in the hadrocharmonium pentaquark scenario.[Formula: see text] In the new data the old LHCb pentaquark [Formula: see text] splits into two states [Formula: see text] and [Formula: see text]. We interpret these two almost degenerated hadrocharmonium states with [Formula: see text] and [Formula: see text], as a result of hyperfine splitting between hadrocharmonium states predicted in Ref. 2. It arises due to QCD multipole interaction between color-singlet hadrocharmonium constituents. We improve the theoretical estimate of hyperfine splitting[Formula: see text] that is compatible with the experimental data. The new [Formula: see text] state finds a natural explanation as a bound state of [Formula: see text] and a nucleon, with [Formula: see text], [Formula: see text] and binding energy 42 MeV. As a bound state of a spin-[Formula: see text] meson and a nucleon, hadrocharmonium pentaquark [Formula: see text] does not experience hyperfine splitting. We find a series of hadrocharmonium states in the vicinity of the wide [Formula: see text] pentaquark that can explain its apparently large decay width. We compare the hadrocharmonium and molecular pentaquark scenarios and discuss their relative advantages and drawbacks. |
| Author | Eides, Michael I. Petrov, Victor Yu Polyakov, Maxim V. |
| Author_xml | – sequence: 1 givenname: Michael I. surname: Eides fullname: Eides, Michael I. – sequence: 2 givenname: Victor Yu surname: Petrov fullname: Petrov, Victor Yu – sequence: 3 givenname: Maxim V. surname: Polyakov fullname: Polyakov, Maxim V. |
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| Cites_doi | 10.1016/j.ppnp.2019.04.003 10.1016/j.physletb.2015.08.032 10.1016/j.physletb.2015.08.008 10.1103/PhysRevD.99.091501 10.1103/PhysRevD.72.094011 10.1103/PhysRevD.96.014022 10.1016/0550-3213(79)90200-1 10.1103/PhysRevLett.122.222001 10.1103/PhysRevLett.110.261601 10.1016/S0550-3213(98)81017-1 10.1103/PhysRevLett.67.556 10.1007/JHEP05(2019)061 10.1103/PhysRevLett.115.072001 10.1142/S0217732314500606 10.1007/JHEP10(2019)256 10.1103/PhysRevD.99.094006 10.1016/S0370-2693(02)03015-0 10.1016/0550-3213(95)00675-3 10.1140/epjc/s10052-017-5437-x 10.1007/BF01413192 10.1017/CBO9780511565045 10.1103/PhysRevD.88.036016 10.1007/JHEP06(2016)160 10.1016/0550-3213(84)90432-2 10.1016/0370-2693(93)90957-J 10.1016/j.physletb.2019.05.002 10.1103/PhysRevD.98.114037 10.1103/PhysRevD.80.034030 10.1140/epjc/s10052-019-6906-1 10.1140/epjc/s10052-018-5530-9 10.1016/j.physletb.2008.07.086 10.1103/PhysRevD.100.011502 10.1103/PhysRevD.94.054024 10.1103/PhysRevLett.122.242001 10.1016/0550-3213(79)90199-8 10.1016/0370-2693(92)91114-O 10.1016/j.ppnp.2008.02.001 10.1103/PhysRevD.93.054039 10.1016/j.physletb.2018.09.047 10.1103/PhysRevD.71.076005 10.1103/PhysRevLett.64.1011 10.1103/PhysRevD.90.016001 10.1016/0550-3213(86)90011-8 |
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| Snippet | New LHCb Collaboration results on pentaquarks with hidden charm1 are discussed. These results fit nicely in the hadrocharmonium pentaquark scenario.
2
,
3
,
In... New LHCb Collaboration results on pentaquarks with hidden charm 1 are discussed. These results fit nicely in the hadrocharmonium pentaquark scenario.[Formula:... New LHCb Collaboration results on pentaquarks with hidden charm1 are discussed. These results fit nicely in the hadrocharmonium pentaquark scenario.2,3, In the... |
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| Title | New LHCb pentaquarks as hadrocharmonium states |
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