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KLOE data collection pb -1 machine and detector studies pb -1 (7.5x10 7 ) published results pb -1 (5.7x10 8 ) analysis in progress pb -1 (9.0x10 8 ) analysis in progress
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European Physical SocietyInternational Europhysics Conference on High Energy Physics
EPS July 17th-23rd 2003 Aachen, Germany
Camilla Di Donato INFN Napolifor the KLOE Collaboration
Rare decays at KLOE
KLOE @ DANE DANE is an e+e- Collider at resonance s =1020 MeV;
DEAR
E.m. calorimeter:/E = 5.7% /(E(GeV)) t = 54 ps/(E(GeV))50ps 98% of 4
Drift chamber:p/p < 0.4%xy150 m ; z2 mm
Quadrupol Calorimeter:
Magnetic field: 0.5 T
KLOE data collection
1999 2.5 pb-1 machine and detector studies2000 25 pb-1 (7.5x107 ) published results
2001 190 pb-1 (5.7x108 ) analysis in progress
2002 300 pb-1 (9.0x108 ) analysis in progress
Radiative decays
• The analysis of 16 pb-1 from 2000 runs has produced the following publications:
Phys. Lett. B541 (2002), 45 Phys. Lett. B537 (2002), 21 Phys. Lett. B536 (2002),
209
• The analysis of full statistic (2001/2002) is in progress
Radiative decays
Radiative decays: Pand S
• Pseudoscalar mesons (JPC= 0-+)
(547) (I=0) (958) (I=0)
• Scalar mesons (JPC= 0++)
f0(980) (I=0) a0(980) (I=1)
Pseudoscalar mesons• The mass eigenstates , are related to SU(3) octet-
singlet 8, 1 through the mixing angle P
• Recent studies based on PT and phenomenological analyses
suggested a two mixing angle scenario
• In the quark flavour basis the two mixing angles are almost equal mixing is described by only one parameter (P)- - -
cosP 1 |uu+dd - sinP |ss 2 - - -sinP 1 |uu+dd + cosP |ss 2
Pseudoscalar mesons P can be extracted from the ratio: (Bramon et al., Eur.Phys.J.C7(1999))
• Br() can probe the gluonic content of
- - - X 1 |uu+dd + Y |ss + Z |glue 2
Br()Br()
ms tg V
m sin 2P
p
p
ms
mR= = cotg2P 1-
2 3
; = 1.45
Br()/Br()
N() = 120125 tot() = 23% N() = 50210220 tot () = 37% R = (4.70 ± 0.47 ± 0.31) x10-3
• Using PDG value for Br():
Br() =(6.100.610.43)10-
5
• Pseudoscalar mixing angle: P = (41.8 1.7) (flavor) P = (-12.9 1.7) (octet-singlet)
F =0.95 (interference with e+e-( )
M (MeV)
Phys. Lett. B 541 (2002), 45
R =NBr Br( )NBr Br( )
F
Gluonic content of a consistency check
• If we allow for a gluonic content
Z = 0 |Y| = cosP
other constraints on X and Y from:
(1) /(0
(2) /(0
X + Y = 0.94 (1)
(2)
+0.06-0.09 2 2
- - - X 1 |uu+dd + Y |ss + Z |glue 2
2001 runs: 100 pb-1
M (MeV)
preliminary
7
2000 data: Br() = (7.05±0.50 )x10-5
(first observation)
200020012002
E++E- (MeV)
dN/d
E
E++E- (MeV)
Ks
Kl
Ks Kl
2000
preliminary+0.53
-0.46
Scalar mesonsThe structure of f0 (980) a0 (980) is not well defined; both BR( S) and scalar mass spectra are sensitive to mesons’ natureSeveral hypothesis has been proposed:•qq states •qqqq states (Jaffe 1977) •kk molecule (Weinstein and Isgur 1990) •meson-meson scattering resonances in a chiral unitary approach (E.Oset)
Models BR( f0) BR( a0) qq 5x10-5 2x10-5
qqqq 3x10-4 2x10-4
kk 10-5 10-5
fa
Decays with 5 final statef0 ; f000
a0 ; a00
Decays with +- 5 final statea0 ; a00 +-0
Decays with +- final statef0 ; f0+-
first observation
340pb-1 2001/2
00 - M spectrum
00 3102 events; <>= 40%
estimated backgr. at level ~20%
Br(00)=(1.09 0.03 0.05) 10-4
SND: (1.220.10 0.06) 10-4 ; CMD-2: (1.080.170.09) 10-4
0 - M spectrum
0 with 916 events; <>=32% estimated backgr. at level ~30%
Br(0)=(8.510.510.57)10-5
SND: (8.8 1.40.9) 10 –5; CMD-2: (9.0 2.41.0) 10 –5
0 with +-0
197 events; <>= 19%estimated backgr. 44 events
Br(0)=(7.960.600.47)10-5
M(MeV)
Fit to the M, M spectra
Kaon loop Kaon loop (VMD) sigma(500) (VMD) sigma(500)
0
0
0
0k+
k-
a0
0k+
k- 0
f0
The structure of f0, a0 states can be investigated by comparing the M, M spectra to theoretical models. As a first step we have tried to fit our data with the kaon-loop model used for the CMD-2/SND data.
Model : f0, a0 dominated by kaon loop f0 , a0 propagator with finite width corrections (Achasov-Ivanchenko, Nucl.Phys.B315(1989))
+ interference term parametrizations (Achasov-Gubin, Phys.Rev.D63(2001))
(500) : B-W with M=478 MeV and =324 MeV (Fermilab E791-Phys.Rev.Lett.86(2001)770)point-like coupling of (500) to (Gokalp,Yilmaz,Phys.Rev.D64(2001))
+-5
5
Kaon loop model : fit results
contribution negligible • adding the (500)
improves the fit (Large f0- destructive interference at M<700 MeV)
• gf0kk, gf0 is compatible with 4q hypothesis
Simultaneous fit to both channels
Ma0=984.8 MeV (PDG) fixed
contribution negligible
• Br(a00)=(7.40.7)10-5
• ga0kk, ga0 is not
A first look at 2001 and 2002 data
• Much more statistics (x25) w.r.t. 2000• Good agreement between the three data sets (2000/2001/2002)
M (MeV)
2001+2002 data2000 data
A first look at 2001/2002 data:
• Re-analysis of 2001+2002 data: new approach• The large statistics allows now to perform a Dalitz plot fit
A first look at : soft
• We also looked for the charged decay f0(980)
• Huge background due to ISR e+e- • Interference with FSR• photon detected at large angles (45°< <135°)
Fitting the spectrum with: - Signal f0 (980) - Background (ISR, FSR) - Interference with FSR Best results for destructive interference
340pb-1
2001+2002 data
M(MeV)
Conclusions and Outlooks• First KLOE papers on radiative decays
published using data collected in 2000:
Measurement of Br() and of P ,- mixing angle in the quark flavor basis
Measurement of Br(00) and Br(0)
• Analysis in progress on 2001+2002 events
16pb-1 (2000) 500pb-1:more statistics, complete analysis of Dalitz plot content