how babar can decide what charmonium-like states 4260, 4360…. really are
DESCRIPTION
How BaBar can decide what charmonium-like states 4260, 4360…. really are. The accidental discovery of a new spectroscopy?. Work by FC with Clark Downum (in PRL) and Chris Thomas (preliminary). 4 to 4.5 GeV region. Gluonic charmonium (hybrid) predicted couples to DD1 and D*D0. - PowerPoint PPT PresentationTRANSCRIPT
How BaBar can decidewhat charmonium-like states4260, 4360…. really are
The accidental discovery of a new spectroscopy?
Work by FC with Clark Downum (in PRL) and Chris Thomas (preliminary)
4 to 4.5 GeV region
Gluonic charmonium (hybrid) predictedcouples to DD1 and D*D0
Strong attractive forces between D* D1 also between DD1 and D*D0
How BaBar can resolve the dynamics !
2
And enigmatic state(s) observed in expt
1++(3872) 1--(4260)
JPC?(4430)
I=1 !?
DD* DD1
D*D1
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1- - (4360) psiprime pipi
D*D1
3
1++(3872) 1--(4260)
JPC?(4430)
I=1 !?
DD* DD1
D*D1
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1- - (4360) psiprime pipi
D*D1
all areS wave in s-channel!
4
Why are nuclear binding energies \sim O(1) MeV per nucleon ?
5
Why are nuclear binding energies \sim O(1) MeV per nucleon ?
Pi exchange is in P-wave= penalty
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Why are nuclear binding energies \sim O(1) MeV per nucleon ?
=> binding energies \sim O(100) MeV per hadron
Pi exchange is in P-wave= penalty
What if Pi exchange is in S-wave= no penalty
7
Why are nuclear binding energies \sim O(1) MeV per nucleon ?
=> binding energies \sim O(100) MeV per hadron
Pi exchange is in P-wave= penalty
What if Pi exchange is in S-wave= no penalty
Can happen for D1 => D* pi in S wave
8
Why are nuclear binding energies \sim O(1) MeV per nucleon ?
=> binding energies \sim O(100) MeV per hadron
Pi exchange is in P-wave= penalty
What if Pi exchange is in S-wave= no penalty
Can happen for D1 => D* pi in S wave
D1D* deep bound molecules
And in S-wave = 1^{- -}Examples 4260; 4360 …..9
1++(3872) 1--(4260)
JPC?(4430)
I=1 !?
DD* D*D1
D*D1
17
1- - (4360) psiprime pipi
D*D1
all areS wave in s-channel!
gluonic degrees-of-freedom
Costs about 1 to 1.5GeV energy to excite phonon“pi/R”Hybrid qq* @ 2GeV; Hybrid cc* @ 4-4.5GeV
Barnes FC Swanson 93
11
R
Predicted 1-+ Hybrid masses (with spin splittings)
charmonium
Predicted 1-+ Hybrid masses (with spin splittings)
charmoniumNear D(L=0)+D(L=1) thresholds: DD0; DD1; D*D0;D*D1 and strongly coupled to these channels…..how distinguish hybrid from DD1 etc molecules?
Predicted 1-+ Hybrid masses (with spin splittings)
Spin hyperfine splittings
1- - (4.25) Y(4260?)1- + (4.1) HQLGT0- + (3.95) X(3940?)
Barnes FC 82Chanowitz Sharpe
e+e- feebly coupled
e+e- \to \psi + X?
14
Novel states in e+e- to + X
???
0-+;1-+
15
e+e- \to psi pi pi BaBar sees unusual vector cc*
Y(4260)
\Gamma(ee) 5-80eVCompare \sim 1 keV !!
But width 90MeV typical hadron !
psi pipi violate OZI
D
D_1 uu * pi pi
psi
16
To do more need dynamics:Production; decays; selection rules
Lattice hints about dynamicsHybrids and DD1 decays
35/18
Beyond Spectroscopy
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What properties
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What properties
Michael McNeile 06
FC Burns 06
confirms Flux Tube for hybrid:conventional
Lattice S-wave decays now calculated Michael McNeile
Exactly WHAT is Lattice revealing about dynamics:What significance if ratio \sim 2?
18
2
qq* create in S=1
qq* create in S=0 0
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J – S = “L” Factorisation of S and L
qq* created in S=1
Factorisation and S=1 creationis powerful result if generally true.
Determine nature of Y(4260) by DD_1 pattern
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SL Factorisation and S=1selection rules for psi*(cc*) \to DD_1
Also applies to KK_1 decays of ss* vectorse.g. ISR around 2.2 GeV
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4260 decays….
…using strong selection rulesto distinguish candidates…
Conventional charmoniumHybrid charmonium Tetraquark csc*s*; Charm molecule D*D1 or DD1
22
flux-tube breaking and hybrid decays
c.m
.c.m
.
e.g. p=1e.g. p=1
Break tube: S+P states yes; S+S suppressed
Isgur Paton 92 light exotics
FC Page 95 all
Look for DD_1 and D*D_0 near threshold
Absence of DD; DD*; DsDs …
24
Y(4260): D_s and D_s* channels
NoDsDsresonance
eliminatestetraquarkcsc*s*
25
Y(4260): D and D* channels
NoDDDD* orD*D*resonance
25
All consistent with predictions for hybrid charmoniumFC+Page 1995
Search DD_1 and D*D_0 in DD\pi\pi
If NOT hybrid cc* then why not/where is it ?!27
The large psi +pi pi = hint of large D(*)D1
D
D_1 uu * pi pi
psi
e+e- psi(hybrid) D(*)D_1
S-wave, relative mom \sim 0; DD_1 interchange constituents to make psi pipi “strongly”
28
The large psi +pi pi = hint of large D(*)D1
D
D_1 uu * pi pi
psi
e+e- psi(hybrid) D(*)D_1
S-wave, relative mom \sim 0; DD_1 interchange constituents to make psi pipi “strongly”
28
Problem: Heavy cc* preserve their spin. Psi has cc* with S=1 Hybrid has cc* with S=0 (h1c eta or etac omega ?)
Problem: and other states: 4360;4430…
Hybrid affected by thresholds
Attractive force from pi exchange:
4260 a result of D1D* (!!) threshold: look for e+e- \to DDbar + 3pi
And what about 4360 in psiprime pipiand 4430 in psiprime pi …..????
29
The Answer: A new spectroscopy?
• At least…..something unexpected!
• 1++(3872) DD* via \pi exchange in p-wave
• 1– (4260 etc) D1D* via \pi exchange
………
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The Answer: A new spectroscopy?
• At least…..something unexpected!
• 1++(3872) DD* via \pi exchange in p-wave
• 1– (4260 etc) D1D* via \pi exchange
in s-wave!
31
D* to D pi (P wave) O(q^2)DD* to D*D binding O(1 MeV)X(3872)
N N pi: deuteron; O(1 MeV)
32
D* to D pi (P wave) O(q^2)DD* to D*D binding O(1 MeV)X(3872)
N N pi: deuteron; O(1 MeV)
32
1++(3872)DD*
D* to D pi (P wave) O(q^2)DD* to D*D binding O(1 MeV)X(3872)
N N pi: deuteron; O(1 MeV)
D1 to D* pi (S wave) O(mA-mB)^2D1 D* binding O(100 MeV)
M = D*D1(4440) - O(100MeV) 4260; 4360 ??33
Look at I=1 D1D* 1^{--}S wave pi exchangeFind it does NOT bind
34
I=1 feeble binding if anyZ(4430)Liu et al PRD77 034003
35
I=1 feeble binding if anyZ(4430)Liu et al PRD77 034003
I=0 strong binding
36
Binding Energy: variational wfns
Ground state B.E can be 100-200 MeV !! Radial excitation bound also??37
Psi(1S)pipi (4260)
Psi(2S)pipi (4360) and (?) 4600
38
2S
1S
4360
4260
D*D1 threshold 4430 I=1
D*D1 spectroscopy
1P 4350
Potential is similar to Coulomb
39
2S
1S
4360
4260
D*D1 threshold 4430 I=1
Vector D*D1 spectroscopy
D*
D_1 uu * pi pi
cc* psi
40
2S
1S
4360
4260
D*D1 threshold 4430 I=1
Vector D*D1 spectroscopy
D*
D_1 uu * pi pi
cc* psi
1S; 2S
(1S; 2S)
41
2S
1S
4360
4260
D*D1 threshold 4430 I=1
Vector D*D1 spectroscopy
Psi(2S) pi pi
Psi(1S) pi pi
42
2S
1S
4360
4260
D*D1 threshold 4430 I=1
Vector D*D1 spectroscopy
Psi(2S) pi pi
Psi(1S) pi pi
DD pi pi pi
43
The immediate test is 4260 decay to
Then look for other exotica. Also in Bottomonium and strangeonium
Phys Rev Letters (in press)
44
Since PRL: (n.b. preliminary - not yet guaranteed)
Sensitivity to D1 and D0 widths for pointlike mesons (value of h)
Effect of finite D meson size (h function of momentum)
Effect of extended pion (Lambda)
And discovery of DD1/D*D0 molecules too: including exotic J(PC)=1(-+)
45
h^2 width of D_1 to D^* \pi
D and pi pointlike:
Data: h \sim 0.7 – 0.8
h=1 3800
h=0.9 4050
h=0.8 4250
h=0.7 4350
Pion size (Lambda)
Reduces BE:
Extended pion provides smaller force
BE tends to zero.
Bad news
Pion size (Lambda)
Reduces BE:
Extended pion provides smaller force
BE tends to zero.
Bad news
Good newsFinite D size:
h(q) => h(0) increases to > 1
Scale of BE increases
51
52
4260
4360
Threshold 4440
52
Surprisingly robust !
Can force-fit because so sensitive so not a real “pre”-diction
Need direct unambiguous tests = decay channels
53
Surprisingly robust !
Can force-fit because so sensitive so not a real “pre”-diction
Need direct unambiguous tests = decay channels
Look for D Dbar pi pi pi (for D1 D* deep bound molecules)
Look for D Dbar pi pi (not D*D*) for DD1/D*D0 molecules and threshold “accidents”
53
Surprisingly robust !
Can force-fit because so sensitive so not a real “pre”-diction
Need direct unambiguous tests = decay channels
Look for D Dbar pi pi pi (for D1 D* deep bound molecules)
Look for D Dbar pi pi (not D*D*) for DD1/D*D0 molecules and threshold “accidents”
DD1/D*D0 molecules also: and exotic 1-+
Look in e+e- \to (D Dbar pi pi) gamma
54
D*D1 threshold4430
D D1 threshold4290
4260
4360
55
D*D1 threshold4430
D D1 threshold4290
D D1 b state or hybrid at threshold4260
spurious4360
Option 1: 4360 spurious; 4260 hybrid or cc* attracted to DD1 threshold
D D pi pi ( DD1 or D*D0; not D*D* )
560
D*D1 threshold4430
D D1 threshold4290
1S psi pi pi4260
2S psiprime pi pi4360
Option 2: 4360 and 4260 D*D1 molecules
D D pi pi pi57
4260 in psi pi pi @ 90 MeV width MUST be due to some charm meson pair
Finding which => reveals dynamicsin the 4 to 4.5 GeV region where hybridsalso predicted.
DDpipi (not D*D*) and DDpipipiare where the answers are to be found
The antidote to Angels and Demons: available from Amazon et al
e+e- KK_1
phi pi pi
Intriguing resonantsignal at 2175
2175 – m(phi)=4265 – m(psi)!!??
41/12
Study KK1 pattern
Psi(1S)pipi (4260)
BaBar and Belle and CLEO
Psi pipi (4260)