studies of the branching ratio for η µ + µ - decay

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Studies of the Branching Ratio for ηµ + µ - decay rascati, Phi Decay Meeting .02.2008 Jarosław Zdebik

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Studies of the Branching Ratio for η  µ + µ - decay. Frascati, Phi Decay Meeting 5.02.2008. Jarosław Zdebik. PLAN. Physics motivation, previous experiments and results. Simulation studies for the signal and background with Geanfi. Physic motivation. - PowerPoint PPT Presentation

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Page 1: Studies of the Branching Ratio for  η  µ + µ -  decay

Studies of the Branching Ratio for ηµ+µ- decay

Frascati, Phi Decay Meeting 5.02.2008 Jarosław Zdebik

Page 2: Studies of the Branching Ratio for  η  µ + µ -  decay

PLAN

1. Physics motivation, previous experiments and results.

2. Simulation studies for the signal and background with Geanfi.

Page 3: Studies of the Branching Ratio for  η  µ + µ -  decay

Physic motivation

1. The dilepton pair production decays can serve to study the structure of decaying hadrons (Form Factor shape)

2. These decays gives a chance to study the physics beyond the Standard Model (searching a candidate for the dark matter particle)

3. Recent BR value measured by SATURNE is equal to 1.3±0.2 (~20% ,~100 events) times the unitarity bound (4.3*10-6) [calculated with VDM]

4. Rare decay - BR= 5.8 * 10-6

Page 4: Studies of the Branching Ratio for  η  µ + µ -  decay

Previous measurements of the BR(ηµ+µ- )

1968 – BROOKHAVEN

upper bound for ..%901020 6 LC

1969 – CERN The first observation of this decay.

anythingnp

B

610923

1980 (published) – SERPUKHOV [Institute for High Energy Physics, USSR]

6101.25.6 BMeasured result is:

Phys. Rev. Lett. V70, N7

Phys. Lett. B V. 97, Pages 471-472

np 27±8 events

ηµ+µ-

Page 5: Studies of the Branching Ratio for  η  µ + µ -  decay

Previous measurements of the BR(ηµ+µ- ) (2)

66.07.0 10.5.0.6.5

syststatB

1993 (published) - SATURNE

Measured 100 events of and 8 events of background

1994 (published) – SATURNE IIPhys. Rev. D 50, 92-103

Measured 114 events of and 14 events of background

67.07.0 10.5.0.7.5

syststatB

3Hepd

3Hepd

Page 6: Studies of the Branching Ratio for  η  µ + µ -  decay

How many events for we expect?

KLOE data = 100 000 000 η mesons (L=2.5 fb-1)

BR(ηµ+µ-) = 5.8 * 10-6 PDG(2008)

If reconstruction efficiency=100%

Number of reactions = 100 000 000 * 5.8 * 10-6 = 580 events (reactions) (5 x Saturne events)

Need to perform efficiency studies in order to estimate how many events we should see.

Very important background rejection (especially from e+e-u+u-)

Page 7: Studies of the Branching Ratio for  η  µ + µ -  decay

The value in PDG 2008, Was calculated as the

average forSerpukhov and Saturne II

results

Page 8: Studies of the Branching Ratio for  η  µ + µ -  decay

SERPUKHOV [Institute for High Energy

Physics, USSR] near Moscov

CEA at Saclay, near Paris, SATURNE synchrotron

Page 9: Studies of the Branching Ratio for  η  µ + µ -  decay

Reaction mechanism

η

l+

l-

γ*

γ*

Dominant mechanism within the Standard Model: second order electromagnetic process,

F(q12,q2

2)arXiv:0711.3531v3

F(q12,q2

2)

C parity: +1 -1

η γ

Page 10: Studies of the Branching Ratio for  η  µ + µ -  decay

Expected background channels for

ϕ ηγ 1.304% ηµ+µ- 5.8 *10-

6 e+e-µ+µ-γ e+e-µ+µ- e+e- ??

e+e-e+e- e+e- γ ??e+e-π+π-γ e+e-π+π- π0 π+π-γ γ e+e- e+e-γ ??

phi decays:

collision:

eta decays: ηπ+π- π0π+π-γ γ 22.73%

ηπ+π-γ 4.6% ηe+e-γ 6.8

*10-3ηµ+µ-γ 3.1 *10-4

η π+π- 1.3 *10-5

ϕe+e- 2.97 *10-4 ??ϕµ+µ- 2.86 *10-4

ϕ π+π- 7.3 *10-5

Signature of signal:One neutral cluster in calorimeter,

Two charged tracks in Drift Chamber

ϕ π+π- γ 4.1 *10-5

ϕµ+µ- γ 1.4 *10-5

Page 11: Studies of the Branching Ratio for  η  µ + µ -  decay

Simulations

Signal:simulated with the standard GEANFI package,

(stand alone simulation)

Background :

GEANFI + phokara generator

Reconstruction and production prod2ntu.hbook was performed

using standard kloe „datarec.exe” program

(e+e-µ+µ-γ)

Page 12: Studies of the Branching Ratio for  η  µ + µ -  decay

Geanfi studies [NTMC - KINE]

Cut:541.0 < Inv mass µ+µ- < 554.0

50 000 events

ηµ+µ-e+e-µ+µ-γ

Page 13: Studies of the Branching Ratio for  η  µ + µ -  decay

ηµ+µ-

e+e-µ+µ-γ

GeanFi studies [NTV – tracks connected with vertex]

50 000 eventsCut:

541.0 < Inv mass µ+µ- < 554.0 eV

Page 14: Studies of the Branching Ratio for  η  µ + µ -  decay

σ(e+e-µ+µ-γ) ~ 30.7 [nb]

σ(e+e- ϕ η γ µ+µ- γ) ~ 3.1 *10-6 * 1.304 *10-2 * 5.8 *10-6

= 2.3 *10-4 [nb]

Ratio S/B~10-5 before any cut.

Background from e+e-µ+µ-γ

Page 15: Studies of the Branching Ratio for  η  µ + µ -  decay

Inv mass studies – kine MC

B/S ~ 62.5Cut:541.0 < Inv mass < 554.0

Inv mass studies – ReconTracks connected with vertex – DC signal

Cut:541.0 < Inv mass < 554.0

B/S ~ 300

Page 16: Studies of the Branching Ratio for  η  µ + µ -  decay

Angular distributions for muons+

Page 17: Studies of the Branching Ratio for  η  µ + µ -  decay

Angular distributions for photon

Statistic: 50000events

Page 18: Studies of the Branching Ratio for  η  µ + µ -  decay

How we reconstructed „gamma quanta” (neutral) cluster ?

1. Extracted neutral cluster using TRACK to CLUSTER association BANK

2. Time window condition:

2

2

222

14.01000

057.05_

__

CLU

LIGHT

CLUCLU

CLUCLUCLUCLU

Ewindowtime

c

RTclutimedelta

BpzZBpyYBpxXR

If(time_window > 2.0) smaller_window = 2.0If(time_window < 2.0) smaller_window = time_window

if(delta_time_clu < smaller_window) calculate:

180arccos

MODUL

Z

CLU

CLUCLUi

p

p

R

XEp

Page 19: Studies of the Branching Ratio for  η  µ + µ -  decay

Energy distributions for photon

Strongly correlated with the invariant mass for eta

Page 20: Studies of the Branching Ratio for  η  µ + µ -  decay

statistic Inv mass µ+ µ-Cut: 541<inv<554

2 measured tracks

1 neutral cluster

1 neutral cluster

ECLU> 250 MeVKINE RECO

N

signal 50 000 50 000 38 401

44 225 45 847 44 276

background

50 000 357 319 41 324 43 424 6 767

Cuts efficiency studies

Page 21: Studies of the Branching Ratio for  η  µ + µ -  decay

Conclusions and futher steps

-- perform efficiency studies in the respect to estimate a realistic number of reactions

-- good cut: invariant mass of the muons (541 < Inv mass < 554)-- additional background recjection should be given by: optimizing invariant mass of the muon (m =5 MeV)and angular cuts-- perform /mu separation

Page 22: Studies of the Branching Ratio for  η  µ + µ -  decay

Thanks for attention

Page 23: Studies of the Branching Ratio for  η  µ + µ -  decay

BACKUP SLIDES

Page 24: Studies of the Branching Ratio for  η  µ + µ -  decay

TRACKS to VERTEX reconstruction

LOOP of tracks connected to the vertex, „vv”

LOOP of all reconstructed tracks, „tt”

If(trkind[tt]==trknumv[vv])

If(trtype1 == 5 mion+)If(trtype1 == 6 mion-)

Page 25: Studies of the Branching Ratio for  η  µ + µ -  decay

Why we need this BR ?

The real part of the amplitude of ηe+e- decay can be estimated using the measured value of BR(ηµ+µ-), etc.

arXiv:0711.3531v3

Page 26: Studies of the Branching Ratio for  η  µ + µ -  decay

Dark matter – cluster bullet

Evidence for existing Dark Matter in Universe.

Galactic gas (red color),Dark matter (blue color). Year: 2006

Page 27: Studies of the Branching Ratio for  η  µ + µ -  decay

Analysis goals

Present measurement:16% precision on the BR

etamu+mu-

Goal of the analysis:Measurement of the BR at 8%

precision level or better.

Enhancement on respect the predicted value of 5.11 ± 0.20 is expected from the

KTevresult on

ee0

Page 28: Studies of the Branching Ratio for  η  µ + µ -  decay

Inv mass studies – kine MC

62.5 times higher background than signal

Cut:541.0 < Inv mass < 554.0

Page 29: Studies of the Branching Ratio for  η  µ + µ -  decay

250 times higher background than signal

Cut:541.0 < Inv mass < 554.0

Inv mass studies – ntv MCTracks connected with vertex – DC signal

Page 30: Studies of the Branching Ratio for  η  µ + µ -  decay

Unitarity bound

Electromagnetic decays of light mesonsInstitute for High Energy Physics, Serpukhov, U.S.S.R

Physics Reports 128. No. 6 (1985) 301-376

2

22

2/12

2222

1

1ln

4

1

41

:

2

Y

m

m

where

YXPBRallP

llPllPBR

P

l

for unitarity bound:

Y and X are the imaginary (absorptive) and real (dispersive) components, respectively,of the normalized dimensionless amplitude

in Pl+l- decay

BR(ηµ+µ-)unit.= BR(ηγγ)*1.07*10-5=4.3*10-6