The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April...
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Transcript of The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April...
![Page 1: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/1.jpg)
The XYZ Mesons
Stephen OlsenU. of Hawai’i
&高能所 北京
Nankai University 天津 April 7,2008
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Constituent Quark Model(CQM)
(& 6 antiquarks)
Mesons: q q
c: c+2/3
c: C-2/3
+ : s-1/3
s+1/3
s+1/3
c-2/3
u-2/3
b+1//3
u+2/3
- : b-1/3
S=1/3
b+1/3
t-2/3c+2/3
b-1/3
t+2/3
6 quarks
Baryons: qqq
u-2/3
d+1/3 s+1/3
u+2/3
d-1/3 s-1/3
Gell-Mann
Zweig
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Fabulously successful
mesons qq
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QCD suggests non-qq meson spectroscopies
Glueballs:gluon-gluon color singlet states
Multi-quark mesons:molecules: diquark-diantiquark:
qq-gluon hybrid mesons
d c
dc
c c
d c
dc
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Caution
Searching for non-QPMhadrons is a risky business
小心
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Remember the pentaquark
T.Nakano et al (LEPS) PRL 91 012002 (2003) 763 citations
+(1530)?
forget
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You never can be sure:
or something else.
Is mother nature is smiling at you?
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The XYZ mesons: candidates for non-qq states
c c
u cuc
4 quark candidates(from Belle)
“ hybrid” qq-gluon candidates(from Babar & Belle)
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Charmonium is of particular interest
because it is an especially good system
to use to search for non-qq mesons
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Primer on Charmonium
小学课本
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Charmonium
r
mesons formed from c- and c-quarks
c-quarks are heavy: mc ~ 1.5 GeV 2mp
velocities small: v/c~1/4
non-relativistic QM applies
c c
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QM of cc mesons
ErVmr
)(2
22
c cr
What is V(r) ??
“derive” from QCD
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“Cornell” potential
~0.1 fm
G.S.Bali hep-ph/0010032
“confining”large distance
component
slope~1GeV/fm
1/r “coulombic”short distance
component
c cr
V(r)
2 parameters:slope & intercept
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Charmonium spectrum
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1-- Charmonium states
J/’
D-meson + anti-D meson mass threshold
”
“narrow”(~100KeV)
e+
e-
Directly accessible via e+e- annihilation
(e+e-hadrons)
“narrow”(~300KeV)“wide”(~25 MeV) ” DD decay
channel is openDD)25MeV
(4
040)
(4
160)
(4
415)
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P-wave states Gamma energy spectrum from ’ X decays
Gaiser et al (Crystal Ball) PRD 34 711
accessible via E1 transitions from ’
23S1 (’)13P2 (c2) 17 keV
23S1 (’)13P1 (c1) 24 keV
23S1 (’)13P0 (c0) 24 keV
13P2 (c2) 13S1(J/) 420 keV
13P1 (c1) 13S1(J/) 290 keV
13P0 (c0) 13S1(J/) 120 keV
E1 Transition Partial width
Calculable from”1st prin
ciples”
Good agreement with
measurements
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Hadronic transitions
(’J/) 70 keV“allowed”
(”J/) 50 keV“allowed”
(’J/) 5 keVSUF(3) violating
(’J/) 0.3 keVisospin violating
“reasonable” agreement between
measurement & th
eory
c.f. Kuang & Yan PRD 41 155
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Recent results
13D1 13P1seen by CLEO hep-ex/0509030
(meas) = 75 18 keV(theor) 59~77 keV
11P1 found by CLEOhep-ex/0508037properties as expected
23P2 found by Bellehep-ex/0507033properties as expected
21S0 found by BelleS.K.Choi et al PRL 89 102001
properties as expected
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The potential model for cc charmonium
mesons is robust and reliable
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a cc meson has to fit into one of these slots:
If it doesn’t, it is a good candidate for a non qq meson
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B-factories produce lots of cc pairs
0-+, 1- - or 1++
0-+, 0++, 2++
C =+ states
1- - only
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Lots new on the “XYZ” particles
• X(3872)– J/ in BKJ/
• Z(3930)– DD in DD
• Y(3940)– J/ in BK J/
• X(3940)– e+e- J/X & e+e- J/ DD*
• Y(4260)– J/ in e+e- J/
• Y(4325)– +-’ in e+e-+-’
Y(4008)?
Y(4250)
Y(4370)
Y(4660)
X(3880)DD- e+e- J/ DD
X(4160)D*D*- e+e- J/ D*D*
Z+(4430)+ - BK+’
New Belle/BaBar results:(Summer 2007)
Status spring 2007:
confirmed by BaBar
updated by Belle
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I’ll concentrate on recent results.
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X(3872)
>300 citations
’ ’
’
X(3872)
X(3872)
X(3872)
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X(3872) properties (PDG2007)
MD0 + MD*0 = 3.871.8 ± 0.4
MeV
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M() looks like
2/dof = 43/39 (CL=28%)
kinematiclimit≈m
PRL 96 102002
CDFBelle
• Belle & CDF: JPC = 1++ most likely
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What’s new with the X(3872)?
BaBar confirms Belle’s DD threshold enhancement
Mass is 3.8±1.2 MeV above WAvg X(3872)J/ mass;
(~3is this significant?
Both groups see a high mass value
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Belle’s BKSX & BK±X comparison
M = 0.22 ± 0.90 ± 0.27 MeV
KS mode K± mode
“molecular” modelspredicted this to be <<1(Braaten et al PRD 71 074005)
“diquark-diantiquark” modelspredicted this to be 8±3 MeV
(Maiani et al PRD 71 014028)
Confirms an earlier BaBar result
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Is there a cc slot for the X(3872)?
3872 M=3872 MeV is too low
Expect:rJ/>>Br(J/)Meas:r(J/)>>Br(J/)
1++(c1’)
cJ/ ispin forbidden D0D00 @ thresh.suppressed BKcc(J=2) suppressed
2-+(c2)
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Y(3940) in BK J/
M≈3940 ± 11 MeV≈ 92 ± 24 MeV
S.-K. Choi et al (Belle) PRL94, 182002 (2005)
M(J/) MeVM2(K) GeV2
M2(
J
) G
eV2
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Y(3940) properties
Belle PRL94, 182002 (2005)
M(J/) MeV
(Y3940 J/) > 7 MeV~very large for charmonium
the Y(3940) mass seems toohigh for it to be the c1’
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Confirmed by BaBar last summer
B±K±J/ B±K±J/
B0KSJ/
M2(K)
J)
ratio
Some discrepancy in M & ; general features agree
B.Aubert et al (BaBar) arXiv 0711.2047
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Is there a cc slot for Y(3940) ?
Can M(c1’)>M(c2’)?c1’
Mass is lowc”
“ “ “ “c0
’
39403931
For any charmonium assignment, [Y(3940) J/ is too large.
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Belle updates e+e-J/D(*)D(*)
D(*)
Use “partial reconstruction technique”
reconstructthese
J/
D(*)
“Recoil” D(*) undetected(inferred fromkinematics)
Continuum
e+ e
-
annihila
tion
e+ e-
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J/D(*) recoil mass
J/
DD
J/
DD
*
J/
D*D
*
J/
DD
*
Partial reconstruction
reconstruct
Belle arXiv:0708.3812
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M(DD*): Confirm X(3940)DD*
D-reconstructed D*-tag
D sidebands
6.0
Bg subtracted
M = 3942 +7 ± 6 MeV
tot = 37 +26 ±12 MeV
Nsig =52 +24 ± 11evts
-6
-15
-16
Previous values:M = (3943 ± 6 ± 6) MeV = (15.4 10.1) MeV< 52 MeV at 90%CL
PRL 98, 802001 (2007)
arXiv:0708.3812
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Is there a cc slot for X(3940) ?
Mass is > M(c2’) &no c1 recoil seen
c1’
Mass is ~ 60 MeV low(if (3S) = (4040))c”
c0
’
39403931
Mass is > M(c2’) &DD decays not seen
Maybe the c”
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M(D*D*)a new state at ~4160 MeV
D*-reconstructed + D*-tag
5.5
M = 4156 +25 ± 15 MeV
tot = 139 +111 ± 21MeV
Nsig =24 +12 ± 11evts
-20
-61
-8
arXiv:0708.3812
It has to have C=+; most likely 0-+,... possibly 0++
if 0++, why is it
not seen in DD?
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A cc assignment for X(4160) ?
Mass is far too low(unless (4S)=(4160),but, then, where is (2D?))
c’’’
Mass is too high(if (3S)=(4040))
or too low(if (3S) = (4160))
c”
39403931
Can place either theX(3940) or X(4160),but probably not both.
4160
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The 1-- states seen in ISR
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e+e- isr Y(4260) at BaBar
233 fb-1
Y(4260)
BaBar PRL95, 142001 (2005)
~50pb
M=4259 8 +2 MeV
= 88 23 +6 MeV -6
-9
fitted values:
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Not seen in e+e- hadrons
(Y4260 J/) > 1.6MeV @ 90% CL
X.H. Mo et al, PL B640, 182 (2006)
4260
4260
BES data
~3nb
peakY(4260)+J/pb
Huge by charm
onium
standards
J.Z.Bai et al (BES), PRL 88, 101802 (2006)
(e+e- hadrons)(e+e- +-)
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“Y(4260)” at Belle (New) M=4247 12 +17 MeV
= 108 19 ±10 MeV -32
M=4008 40 +114 MeV
= 226 44 ±87 MeV -28
???
C.Z Yuan et al (Belle) arXiv:0707.2541 PRL 99, 182004
M=4259 8 +2 MeV
= 88 23 +6 MeV -6
-9
BaBar values:
Resonance?Thresh effect?…?
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No 1-- cc slot for the Y(4260)
42604260
X.H. Mo et al, hep-ex/0603024
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Is the Y(4260) a cc-gluon hybrid?
c c
• qq-gluon excitations predicted 30 yrs ago • lowest 1-- cc-gluon mass expected at ~4.3 GeV • relevant open charm threshold is D**D (~4.28 GeV) • (J/) larger than that for normal charmonium • (e+e-) smaller than that for ordinary charmonium
Horn & Mandula PRD 17, 898 (1977)
Banner et al, PRD 56, 7039 (1997); Mei & Luo, IJMPA 18, 15713 (2003)
Isgur, Koloski & Paton PRL 54, 869 (1985)
McNeile, Michael & Pennanen PRD 65, 094505 (2002)
Close & Page NP B443, 233 (1995)
Y(4260) s
eems t
o matc
h all
of these
!!!
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DD** thresholds in & “Y(4260)”
4.28-mD
D** spectrum
M(J/) GeV
No obviousdistortions
D1D
D2D
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BaBar’s ’ peak at 4325MeV
Nbkg = 3.1 1.0
Nevt = 68 (<5.7 GeV/c2)
2-prob < 5.7 GeV/c2
Y(4260) 6.5 10-3
(4415) 1.2 10-13
Y(4320) 29%
e+e-ISR ’
M=4324 24 MeV
= 172 33 MeV
above all D**D thresholds
S.W.Ye QWG-2006 June 2006
Not Compatible with the Y(4260)
D1D
D2D
298 fb-1 (BaBar) hep-ex/0610057
BaBar PRL 98 252001 (2007)
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4325 MeV ’ peak in Belle (new)
M=4324 24 MeV
= 172 33 MeV
548 fb-1
X.L. Wang et al (Belle) arXiv:0707.3699PRL 99, 142002 (2007)
Two peaks!
M=4664 11 ±5 MeV
= 48 15 ±3 MeV
M=4361 9 ±9 MeV
= 74 15 ±10 MeV
BaBar values
(both relatively narrow)(& both above D**D thresh)
(& neither consistent with 4260)
4260
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Recent Newsele
ctric
ally
charg
ed!!
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M(±’) from BK ±’
M2(K) GeV2
M2(’)
GeV
2
S.-K. Choi et al (Belle) arXiv:0708.1790PRL 100 this Friday!
K*KK2*K Veto Veto
M(’) GeV
6.5
M = 4433 ±4 ±1 MeV
tot = 45 +17 +30 MeV
Nsig =124 ± 31evts-13 -11
![Page 51: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/51.jpg)
Could this be a reflectionfrom the K channel?
![Page 52: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/52.jpg)
Cos vs M2(’)
16 GeV2
22 GeV2
M2(
’)
+1.0
-1.0
cos
M (’) & cosare tightly correlated;a peak in cos peak in M(’)
(4.43)2GeV2 0.25
’
K
![Page 53: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/53.jpg)
Can interference between K partial waves produce a peak?
Only S-, P- and D-waves seen in data
inte
rfere
Add incoherently
![Page 54: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/54.jpg)
Can we make a peak at cos≈0.25
with only S-, P- & D-waves?
Not without introducing other, even more dramatic
features at other cos (&,, other M’) values.
![Page 55: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/55.jpg)
Comments on the Z+(4430)
Not a reflection from the K system~
No significant signal in B KJ/
It has non-zero charge not cc or hybrid
Mass, width & decay pattern similar to Y(4360) & Y(4660)
![Page 56: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/56.jpg)
comments• There seems to be a new hadron spectroscopy in the M=3.5~5
GeV region– Maybe more than one– Bodes well for BESIII, Super-B factories & PANDA
• Some states are narrow even though they are far above decay thresholds
– e.g. Y(4660)’ & Z+(4430)’ have large Q but ≈50 MeV
• characterized by large partial widths (Bfs) to hadrons+J/(or ’)
– Br(X(3872)J/) > 4.3% (Isospin=1)– (Y(3940)J/) > 7 MeV – (Y(4260)J/) > 1.6 MeV
• States that decay to ’ not seen decaying to J/ (and vice-versa) – Bf(Y(4660)’) >> Bf(y(4660)J/) same for Y(4360) & Z(4430’– Y(4260) not seen in Y(4260)’
• The new 1-- states are not apparent in the e+e-D(*)D(*) cross sections
• There are no evident changes at the D**D mass threshold
(mine)
![Page 57: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/57.jpg)
New 1-- states J/
J/
’
C.-Z. Yuan et al (Belle) PRD 77, 011105® (2008)
![Page 58: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/58.jpg)
some of the states are near thresholds,but this is not a universal feature
DSDS thresholdsDD thresholds
![Page 59: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/59.jpg)
D*D*
DD*
DD
tot
Y(4
660)
Y(4
360)
Y(4
260)
Y(4
008) The 1-- states
do not match wellto peaks in hadr.
cross-sections
Pakhlova (Belle) PRL 98, 092001 (2007)
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Are there XYZ counterparts
for the ss- & bb- systems?
![Page 61: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/61.jpg)
Belle:((5S)(nS))
2S
3S4S
(4S) (1S) +
(4S)(1S)477 fb-1 from Belle
44±
8 e
vts
“(5S)”(1S)23.6 fb-1 from Belle
(1/20 times the data &
~1/10th the crosssection)
325±
20
evts
!
8 times as many events!
Belle 0710.2577
K.F. Chen et al (Belle) PRL 100, 112001 (2008)
(2 weeks ago)
is Huge!!!
![Page 62: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/62.jpg)
Partial Widths
N.B. Resonance cross section 0.302 ± 0.015 nb at 10.87 GeV PRD 98, 052001 (2007) [Belle]
Cf (2S) (1S) ~ 6 keV (3S) 0.9 keV (4S) 1.8 keV
Assume “(5S)” = (5S)PDG value taken for (nS) properties
>100 times bigger!!
![Page 63: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/63.jpg)
It looks like there is a bbversion of the Y(4260)
lurking around the (5S)
If there are bb versions of the XYZ’s, why not ss versions as well?
W.-S. Hou PRD 74, 017504 (2007)
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1-- Ys states around 2 GeV?Y(2175)f0(980)
from BaBar (confirmed by BESII)
e+e- f0(980)@ Ecm ~10.6 GeV
confirmed by BESII
M(f0(980) GeV
M.Ablikim et al (BES)PRL 100, 102003 (2008)
3 weeks ago
![Page 65: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/65.jpg)
Luciano Maiani @ had-2007
![Page 66: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/66.jpg)
Now it looks like there may also be XYZ-like spectroscopies for the s- & b-quark sectors
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Lots of pieces
Y(4360)
Y(4
660)
Y(4260)
Y(4
050)
X(3872)
X(3940
)
X(416
0
)
Z(4430) Y(3940)
Are the
y al
l fro
m the
sam
e pu
zzle
?
![Page 68: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/68.jpg)
謝謝
![Page 69: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/69.jpg)
Inclusive BKx from BaBar
?
Fully reconstructed B- tags
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M2(’) / cos plot1.0< M(K)<1.4 GeV
Our attempts to fit theM=4.43 GeV (cos=0.25)
peak with any combination ofS-, P- & D-waves
![Page 71: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/71.jpg)
M(DD): Broad threshold enhancement
arXiv:0708.3812
Relativistic BW
D sidebands
D-reconstructed D-tag
3.8
Bg subtracted
Resonance?Thresh effect?… ?
![Page 72: The XYZ Mesons Stephen Olsen U. of Hawai’i & 高能所 北京 Nankai University 天津 April 7,2008.](https://reader036.fdocument.pub/reader036/viewer/2022081503/56649d595503460f94a396a3/html5/thumbnails/72.jpg)
BaBar looked for a charged partner of the X(3872) and excluded isospin 1: BF(B0 X- K+ ) BF(X J/ψ - 0 ) < 5.4 x 10-6
BF(B- X- K0 ) BF(X J/ψ - 0 ) < 2.2 x 10-5
c.f BF(B0 X0 K+ ) BF(X 0 J/ψ -- + ) =(1.28 0.41 ) x 10-5
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M() near 4008 & 4260 MeV
3.8 < M(J/) <4.2 GeV 4.2 < M(J/) <4.4 GeV
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Y(4660) f0(980) ’?
4.0 < M(’) <4.5 GeV 4.5 < M(’) <4.9 GeV
f0(980)?
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K+K- J/ from Belle (very new)
C.Z.Yuan et al (Belle) arXiv:0709.2565
(4415)?
M=4875 132 MeV
= 630 126 MeV M=4430 +38 MeV
= 254 +55 MeV
4260
-43
-46
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M(K+K-)