kloe results on hadron physics

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KLOE results on hadron physics Cesare Bini Università “La Sapienza” and INFN Roma on behalf of the KLOE collaboration Hadron07, Frascati 09/10/200 Outline: 1. The KLOE experiment 2. Results on pseudoscalar mesons 3. Results on scalar mesons 4. Prospects

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Hadron07, Frascati 09/10/2007. KLOE results on hadron physics. Cesare Bini Università “La Sapienza” and INFN Roma on behalf of the KLOE collaboration. Outline: The KLOE experiment Results on pseudoscalar mesons Results on scalar mesons Prospects. 1. The KLOE experiment at DA  NE. - PowerPoint PPT Presentation

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Page 1: KLOE results on hadron physics

KLOE results on hadron physicsCesare Bini

Università “La Sapienza” and INFN Romaon behalf of the KLOE collaboration

Hadron07, Frascati 09/10/2007

Outline:1. The KLOE experiment2. Results on pseudoscalar mesons3. Results on scalar mesons4. Prospects

Page 2: KLOE results on hadron physics

1. The KLOE experiment at DANEDAFNE @ Frascati

Laboratories• e+e- collider with 2 separate

rings:

s = M= 1019.4 MeV

• Luminosity up to 1.5×1032 cm-2s-1

• 2 interaction regions

1. KLOE 2700

pb-1

2. DEAR (kaonic atoms) 100

pb-1 FINUDA

(hypernuclei) 1100 pb-1

KLOE STATUS:

March 2006: end of KLOE data

taking

2500 pb-1 on-peak 8 × 109

decays

200 pb-1 off-peak (energy scan+1

GeV run)

Dafne test in progress

Page 3: KLOE results on hadron physics

The KLOE physics program: Kaon physics: CP and CPT violation, CKM unitarity, rare decays, ChPT tests Hadron physics: lowest mass pseudoscalar, scalar and vector mesons Hadronic cross-section below 1 GeV: hadronic corrections to g-2

List of the decays: branching ratios and number of events “on tape”B.R. Nev KLOE (2.5 fb-1)

K+K- 0.49 3.7 109

K0K0 KSKL 0.33 2.5 109

0.15 1.1 109 1.3 10-2 9.7 107

1.2 10-3 9.0 106

’ 6.2 10-5 4.6 105

(f0(980), ) 3 10-4 2.5 106

(a0(980)) 7 10-5 4.6 105

KK(f0(980), a0(980)) ? ?

Initial State Radiation e+e-

Page 4: KLOE results on hadron physics

The KLOE detector: A large drift chamber A hermetic calorimeter A solenoidal superconducting coil

Drift Chamber (He-IsoBut. 2m × 3m)

E.M. Calorimeter (lead-scintillating fibres)

Magnetic field (SuperConducting Coil)

= 0.52 T (solenoid)

)(%4.5

GeVEEE

psGeVEps

t 130)(

55

%4.0)(

p

p

Page 5: KLOE results on hadron physics

Results presented here:2.1 Precision measurement of the mass2.2 Improved measurement of the - ’ mixing

(also 0)2.3 Dynamics of 3 decays 2.4 Measurement of KS 2.5 Preliminary measurement of B.R.(-e+e-)2.6 A flash on 0

2. Results on pseudoscalar mesons.

Talks by: F.Ambrosino, A.De Santis, B.Di Micco, R.Versaci (Light Meson Spectroscopy I) M.Martini (Low energy QCD)

Page 6: KLOE results on hadron physics

2.1 Precision measurement of the mass

Motivated by the discrepancy between the two best measurements:NA48 (2002)M() = 547.843 ± 0.030 ± 0.041 MeVGEM (2005) M() = 547.311 ± 0.028 ± 0.032 MeV

( >10 , PDG average gives a scale factor of 5.8 !)Recently a new measurement has been published by CLEO:

CLEO (2007) M() = 547.785 ± 0.017 ± 0.057 MeV

KLOE method: analysis of fully neutral 3 events with with

3 clusters in the calorimeter only.Kinematic fit with 4 constraints ==> energies by cluster positions Discrimination between and very easy from Dalitz plot.Absolute energy scale from the e+e- center of mass energy s(kinematic fit input) - calibrated comparing M() obtained by the energy scan to the PDG value (dominated by CMD-2)

Page 7: KLOE results on hadron physics

KLOE final result: M() = 547.873 ± 0.007 ± 0.031 MeVSystematic error due to: - detector uniformity; - Dalitz plot cuts. mass check: M() = 134.906 0.012 0.048(compatible at 1.5 with PDG)

3 Dalitz plot mass peak

Page 8: KLOE results on hadron physics

2.2 Measurement of the – ’ mixing

KLOE method: measurement of

R B.R.( ')B.R.( )

2002 result (Phys.Lett.B541,45) Lint= 16 pb-1 , final states2007 result (Phys.Lett.B648,267) Lint=427 pb-1 , final states

2002 2007

N() 5 107 1.4 109

N() 5 104 1.7 106

N(’) 120 3400

R (4.70 0.47 0.31) 10-3

(4.77 0.09 0.19) 10-3

BR(’) (6.10 0.61 0.43) 10-5

(6.20 0.11 0.25) 10-5

P(*) (41.8 +1.9 -1.6)o (41.4 0.3 0.9)o

Errors are now dominated by “intermediate and ’ B.R.s”:(BR(’ ) known @ 3%, BR((’ ) @ 5.7%)

(*) evaluated according to A.Bramon et al., Eur.Phys.J. C7, 271 (1999)

Page 9: KLOE results on hadron physics

KLOE analysis uses the constraints:J.L.Rosner, Phys.Rev. D27 (1983) 1101,A.Bramon et al., Phys.Lett. B503(2001) 271E.Kou, Phys.Rev.D63(2001) 54027

Y1: ’ Y2: ’ Y3: R Y4: ’A >3 effect is found:

Z2’ = 0.14 0.04

P = (39.7 0.7)o

' X ' qq Y ' ss Z ' gluons

R.Escribano, J.Nadal (JHEP 0705,006,2007) reanalyze all V P and P V decaysupdating wavefunction overlaps parameters and neglecting the Y1 constraint no evidence of gluonium content

Experimentally:improve (’), BR(’), ’,BR(0)

Constrain to the ’ gluonium content:

Page 10: KLOE results on hadron physics

e+e- 0: interference pattern between decay and continuum:fit of cross-section s dependence using 2 decays channels of the .

Cross-section parametrization:

Preliminary results:BR(0)=(5.63±0.70)×10-5

()/()=0.0934±0.0021

Using PDG values for the main decay we get: BR()=(8.40±0.19)% (error reduced to 2%, central value shifted –6%)

Page 11: KLOE results on hadron physics

2.3 Dynamics of the 3 decay'3 decay isospin violation in strong interactions mu md ms

A test of low energy effective theories of QCD

KLOE has studied with high statistics the dynamics of both channels:(a)Dalitz plot analysis: 1.34 106 events(b)”slope” analysis: 0.65 106 events

(a) Dalitz plot (submitted to Phys.Lett.B):- large statistics- negligible background- use X and Y variables

Page 12: KLOE results on hadron physics

Fit results of the Dalitz plot

Comments: 0. the odd terms (c and e) in X are compatible with 0 (no asymmetries); 1. the quadratic term in X (d) is unambiguosly different from 0; 2. the cubic term in Y (f) is needed to get an acceptable fit; 3. the b=a2/2 (current algebra rule) is largely violated.

Including systematic errorsa=-1.090 0.005 +0.008 -0.019

b= 0.124 0.006 0.010d= 0.057 0.006 +0.007 -0.016

f= 0.14 0.01 0.02

Page 13: KLOE results on hadron physics

Dalitz plot asymmetries test of C invariance

All asymmetries are compatible with 0 up to the 10-3 level

Left-Right C-invarianceQuadrant C-invariance in I=2 amplit. Sextant C-invariance in I=1 amplit. (see J.G.Layter et al.,Phys.Rev.Lett.29 (1972) 316)

KLOE results: x 5 statistics respect to best previous experiment

Page 14: KLOE results on hadron physics

(b) Fit results of the ”slope”

The slope is evaluated by comparing the z distribution of the data with a Montecarlo simulation with =0 (pure phase space) High sensitivity to the M() value (Dalitz plot contour)

MC with M()=547.3 MC with M()=547.822

New (preliminary) result: = -0.027 0.004 +0.004 -0.006

in agreement with Crystal Ball (=-0.0310.004);

Page 15: KLOE results on hadron physics

2.4 Measurement of the decay KS BR estimated by ChPT @ order p4 (G.D’Ambrosio, D.Espriu, Phys.Lett.B175 (1986)27)

KLOE method: KSKL

- KS tagging provided by KL interacting in the calorimeter:

- Large background from KS decay (105 times more frequent)

Red= MC signalBlue= MC backgroundPoints=data

BR(KS )=(2.27 0.12(stat) 0.05(syst))10-6

Result compared to other experiments and theory

Page 16: KLOE results on hadron physics

KLOE preliminary result based on 622 pb-1 (1/4 of full data sample)Event selection:

4 tracks events + 1 photon (363 MeV );Kinematic Fit-e recognition (kinematic and calo PiD (in progress))

Backgrounds:other decays (mainly and with conversion)charged kaon decays +

2.5 Preliminary measurement of BR(-e+e-)

-Up to now poorly measured (4 events CMD-2, 16 events CELSIUS-WASA);(WASA@COSY program)

-BR predicted by ChPT and VMD models (2.63.6 × 10-4);-Plane asymmetry “unconventional” CP violation ;(D.Gao, Mod.Phys.Lett.A17 (2002) 1583)

Page 17: KLOE results on hadron physics

Fit of Minv(ee) with signal + background 733±62 signal events (×36 with respect to previous experiments)

Total efficiency = 11.7%Systematic uncertainty still under evaluation

BR(-e+e-)=(2.4 ±0.2stat± 0.4syst) × 10-4

() data pointssignalother decaysother bckg (mainly K±)

In progress: asymmetry Few % level sensitivity

Page 18: KLOE results on hadron physics

ChPT “golden mode” KLOE has presented a 3 signal (only 1/5 of full statistics)

The signal is confirmed in the full data sample. B.R. updated result with the full sample will have ~15% error

2.6 A flash on 0

4 mass spectrum of selected events(1.5 fb-1 2005 data).Yellow = expected bck.Points = data

CB@MAMI-B: BR=(22.4±4.6±1.7) ×10-5

Page 19: KLOE results on hadron physics

3. Results on scalar mesons.KLOE contribution to the understanding of the lowest mass scalars:

f0(980), a0(980), (500) through radiative decays in pairs of pseudoscalars

(1020)

Mass (GeV/c2)

a0(980)

I=0 I=1/2 I=1

f0(980)

(500)

(800)

0

1

Motivations: 1. |ss> scalar quark composition

of f0(980), a0(980) 2. Search for evidence of (500)

Results presented here: 3.1 KLOE results on f0(980) 3.2 High statistics study of 3.3 Search for the decay K0K0

Talks by: S.Fiore, F.Nguyen (Light Meson Spectroscopy II)

Page 20: KLOE results on hadron physics

Large “unreducible” backgrounds for both channels:0 and 0 for ;ISR, FSR and for

Extraction of the scalar amplitude fit of the spectrum parametrization of signal and background

KLOE observed the decay f0(980) in and 00 channels: : Phys.Lett.B634 (2006) 148;

: Phys.Lett.B537 (2002) 21; Eur. Phys.J. C49 (2006) 433;

3.1 Update of KLOE results on f0(980)

f0(980)Dalitz plot

mass spectrum

Page 21: KLOE results on hadron physics

Comments:1.The Kaon-Loop well describes the mass spectra;2.The f0(980) is strongly coupled to the s quark: gf0KK > gf0+-

3.The scalar amplitude has a large low mass tail (m<600 MeV) that can beinterpreted as due to the (600);In progress: combined fit with improved background amplitudes

Attempt to describe both spectra with a unique scalar amplitude.[Achasov and Kiselev, Phys.Rev.D73 (2006) 054029]:Scalar amplitude = f0(980) + (600) + interference.

(600) parameters and /KK scattering phases fixed(10 different parameter sets, see Eur. Phys.J. C49 (2006) 433)

free parameters: Mf0, gf0KK , gf0+- Preliminary results (uncertainties under evaluation) are encouraging:

Mf0(MeV)

gf0KK

(GeV)gf0+-

(GeV)P(2)

982.1 4.0 -1.7 6.3% 983.7 4.7 -2.2 2.5%

Page 22: KLOE results on hadron physics

3.2 High statistics study of : the a0(980).

• Selection of:1. events with : fully neutral 5 events;2. events with : 2tracks and 5 events

• Background subtraction: 18% in sample 1, 13% in sample 2• Event counting: 18400 in sample 1, 3600 in sample 2

“Pure” final state, dominance of a0(980) intermediate state

Preliminary results on the branching ratioB.R.( )(1) = (6.92 0.10stat 0.20syst) 10-5

B.R.( )(2) = (7.19 0.17stat 0.24syst) 10-5

in good agreement, (part of the systematic errors are common).Error improvement: 9% (Phys.Lett.B536 (2002) 216) 3% (this result)

• M() spectra• Combined fit of the spectra with a0 production parametrizations(convoluted with efficiencies and resolutions)

Page 23: KLOE results on hadron physics

The fit parameters (preliminary). Ratio BR( )/BR( ) BR( ) contribution(KL) Kaon-Loop:(N.Achasov,A.V.Kiselev, Phys.Rev.D73(2006)054029) Ma0, couplings ga0KK ga0, phase

(NS) Breit-Wigner + polynominal “background”:(G.Isidori et al., JHEP0605 (2006) 049) Ma0, couplings ga0 ga0KK ga0

KL fit: points =datared =fitting curve (model efficiency and resolution)

Page 24: KLOE results on hadron physics

Comments:1. Good consistency between sample 1 and 2: the result is experimentally “solid”; 2. KL fit is stable, NS requires to fix some parameters; Results: 2.1 ga0KK ~ 2 GeV and ga0KK / ga0 ~ 0.8 “conflict” with qqqq hypothesis; 2.2 Large values of BR( ) and of ga0

sizeable coupling with the (as for f0(980))

Meson gM (GeV-1)

0 0.13

0.71

´ 0.75

a0(980) 1.6

f0(980) 1.2 – 2.7

Other descriptions: Unitarized Chiral Model [Palomar et al., Nucl.Phys.A729 (2003) 743] KK molecule [Kalashnikova et al., Eur.Phys.J.A24 (2005) 437] Linear Sigma Model [Bramon et al., Phys.Lett.B494 (2000) 221]

Page 25: KLOE results on hadron physics

3.3 Search for the decay KSKS

In K0K0 the K0K0 pair is:in a J=0 state = [|KSKS>-|KLKL>]/2;in a I=0,1 isospin state a0 and f0 contribute;

Very small allowed phase space: 2MK < MKK < Msmall B.R.Predictions on B.R.: from 10-13 (no scalar contribution) up to 10-7 We have used the decay chain: KSKS ()() 4 tracks+1 photon (E

max=24 MeV) Overall efficiency = 20.6% Very small bckg (ISR KSKL)

Result (preliminary): (Ldt = 1.4 fb-1)1 event found;0 expected background;

BR( KSKS)<1.810-8 90% CL

Page 26: KLOE results on hadron physics

4. Prospects. (talks by P.Moskal and D.Domenici (Future facilities))

DAFNE is testing now a new scheme to increase luminosity KLOE phase-2 could start (2009):

~10 times more statistics improved detector (inner tracker, improved calorimeter

readout, tagger, new small angle calorimeters) “enriched” physics program

Kaon, , ’ decays (high statistics) (sigma), 0 2 widthdeeply bound kaonic states (AMADEUS proposal)

Increase the center of mass energy up to 2.5 GeV is also considered (KLOE phase-3)

physics program extended tohadronic cross-section (g-2, em)baryon time-like form factors (DANTE proposal) physics (,’,f0(980),a0(980) 2 widths)

[see http://www.lnf.infn.it/lnfadmin/direzione/roadmap/roadmap.htmlF.Ambrosino et al., Eur.Phys.J. C50,729 (2007)]