1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting...

27
1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI

Transcript of 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting...

Page 1: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

1

Lead glass simulations

Eliane Epple, TU MunichKirill Lapidus, INR Moscow

Collaboration Meeting XXI

March 2010GSI

Page 2: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

2

1. Cherenkov light tracing

2. Lookup table

3. Physical application

Outline

Page 3: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

3

HADES EMC

Hardware:

Cherenkov light EM calorimeter

142 * 6 lead glass blocks

Physics:

e/h separation at high momentum

π0, η reconstruction

Sesimbra meeting status:

EMC is implemented in HGeant

First simulations were started

Page 4: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

4

The challenge

Realistic studies require simulation of the electron/gamma and

hadron response Hadron response is complex and can’t be simulated simply via

energy deposit in the module Need for proper Cherenkov light tracing Previously obtained results are not satisfactory:

8.7% / sqrt(E)~5% / sqrt(E)

γ in simulation: γ in reality:

old simulationsOpal results

Page 5: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

5

The solution

Use the Light Transport code written by Mikhail Prokudin, ITEP

(CBM ECal)

Standalone program outside HGeant

Tuning of the parameters

Light attenuation length in the lead glass

PMT geometry and quantum efficiency

Reflective properties of the lead glass wrapping

Page 6: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

6

Tuning results

γ 580 MeV cosmics

Experimental reference for the tuning

Energy resolution for γ

Same response shown by γ 580 MeV and cosmics

Page 7: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

7

Single lead glass module response to different particle species

eγπpn

Cherenkov

thresholds

Pπ = 98 MeV/c

Pp = 700 MeV/c

Page 8: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

8

e/pi separation

at 95% electron efficiency

Page 9: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

9

Making things faster:Lookup table instead of the light tracing

• Light tracing is very slow: 1.2 s/event for 1 GeV γ

• Prepare a lookup table for the probability of the p. e. production

• 4D lookup table: t = (x2 + y2)1/2, z, θ, energy

• Make use of THnSparse class as a container

• Binning: 30 * 30 * 180 * 30 = 5·106, populated by 3·109 trial photons

• 2D projections: (z, t) and (energy, z)

glass pmt

Page 10: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

10

Testing the approach: Full tracing vs Lookup table

Tracing

Lookup table

pion, p = 0.3 GeV/c neutron, p = 2 GeV/c

gamma, p = 0.1 GeV/c gamma, p = 1 GeV/c

Page 11: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

11

Testing the approach: Full tracing vs Lookup table

Tracing

Lookup table

gamma, p = 0.1 GeV/c gamma, p = 1 GeV/c

In general Lookup table works well

A bit more effort is needed for correct gamma width

Increase the bin numbers/statistics in the table

4%

4.5%

Page 12: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

12

What is the profit from the Lookup table?

γ 1 GeV CC 8 AGeV AuAu 1.25 AGeV

no EMC — 0.2 0.7

Tracing 1.2 4.9 10.2

Lookup < 0.1 0.6 1.7

Computational time, seconds per event

Page 13: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

13

Application:light system at high energies

Pluto cocktail for C + C at 8 AGeV

Mp = Mn = 8.9

Mπ+ = Mπ– = Mπ0 = 1.86

Mη = 0.093

Full HADES geometry in front of EMC

Simple reconstruction software was written

Digitization Clustering Pair makingRPC matching

Page 14: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

14

Diphoton invariant mass in CC at 8 AGeV

Employ only calorimeter data

Overwhelming background

from hadron misidentification

CC 8 AGeV

Page 15: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

15

Diphoton invariant mass in CC at 8 AGeV

Cluster matching with RPC hits to reject charged hadrons

Significant background suppression

Clear π0-peak

η is not visible, more statistics is mandatory

CC 8 AGeV

Page 16: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

16

Diphoton invariant mass in CC at 8 AGeV

Cluster matching with RPC hits to reject charged hadrons

Significant background suppression

Clear π0-peak

η is not visible, more statistics is mandatory

CC 8 AGeV

Page 17: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

17

Summary

1. New approach to Cherenkov light tracing

2. Reasonable response both to gamma and hadrons

3. Working Lookup table

4. Simulation software is complete

5. First realistic diphoton spectra for the light system

at high energies (π0 reconstruction is shown)

Outlook:

— Further development of the reconstruction software

— η reconstruction

— Attack heavy systems

Page 18: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

18

Additional slides

Page 19: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

19

Integral Lookup table test

TracingLookup table

Reconstructed diphoton invariant mass for

CC 8 AGeV 10k events

Page 20: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

20

Calibrations and corrections for the simulation(to be done)

Page 21: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

21

Correlation of energy deposition and Cherenkov photon yield

N_pe = 1785 * (E/GeV)

OPAL paper NIM A290 76-94N_pe = 1800 * (E/GeV)

~ 10K Cherenkov photons tracked in each module

Limited energy range was investigated due to extreme hit multiplicities

Dep

osi

ted

en

erg

y in

mo

du

le, M

eV

Page 22: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

22

Study of response to single photons:energy deposition in EMC

— whole EMC— 3x3 cluster

▼ whole EMC▼ 3x3 cluster

Deposited energy for 1 GeV photon Energy dependence

Page 23: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

23

EMI 9903B quantum efficiency

Page 24: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

24

Lead glassinteraction lengths

Lead glass

Quantity Value Units Value Units

<Z/A> 0.42101

Density 6.22 g cm-3

Nuclear collision length 95.9 g cm-2 15.42 cm

Nuclear interaction length 158.0 g cm-2 25.40 cm

Pion collision length 122.2 g cm-2 19.64 cm

Pion interaction length 190.0 g cm-2 30.55 cm

Radiation length 7.87 g cm-2 1.265 cm

Page 25: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

25

EMC geometry

Top view of one sector

142 identical modules

Technical drawing by Polish group

Page 26: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

26

Position as present Shower

phi (0, 2pi) theta (18, 45)L = 240 cm

d x d = 9.2 x 9.2 cm2

sigma_theta = d/L/sqrt(12)sigma_phi = sigma_theta

sigma_E/E = 5% / sqrt(E/GeV)

EMC geometry

C+C @ 8 AGeV10M events

Pluto

Multiplicities (min. bias)M_pi0 = 1.86M_eta = 0.093

Diphoton decays only

Simple simulation:geometry and Pluto input

Page 27: 1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.

27

S/B = 10%S/B = 11%

sigma_eta = 25 MeVsigma_eta = 25 MeV

pγ > 300 MeV pγ > 500 MeV

Diphoton invariant mass

EMC acceptance spatial & energy smearing of photon

M, GeV M, GeV