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PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

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Page 1: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

PANDA electromagnetic calorimeters

Pavel Semenov IHEP, Protvinoon behalf of the IHEP PANDA group

INSTR08 28 Feb - 05 Mar 2008

Page 2: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 2

Outline

• PANDA detector setup

• Target Spectrometer EMC– PANDA gamma irradiation facility at IHEP

– Light output at -20°C

– Radiation hardness measurements at -20°C

• Forward Spectrometer EMC– EMC prototype module parameters

– Prototype testbeam results for energy and position resolution

– MC studies to find optimal parameters

Page 3: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 3

PANDA EM Calorimeters placement

FS EMCTS EMC

Page 4: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 4

Target spectrometer EMC

• Requirements – Geometrical coverage close to 4π– Compact size– Fast signal, good time resolution– Low energy threshold (10 MeV) of photon detection– Excellent position and energy resolutions

• PbWO4 (PWO) crystal as a good candidate for the TS EMC– 21 mm x 21 mm x 20 cm barrel cell size (front), 25 mm x 25 mm x 20

cm endcap cell cize – ~17000 crystals (96 % of 4 π)

• Improved light output is needed to reach excellent resolution and low threshold– Calorimeter operates at low temperature (about -200C, factor of 3 increase

of light output) – PWO-II: enhanced light output PWO (~20 phe/MeV)

• PWO radiation hardness at room temperature is not a problem for PANDA (dose rates not more then a few rad/hour). But there were no data for PWO radiation hardness properties at -20 0C

Page 5: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 5

PANDA-IF at IHEP features

• Crystal holder (Cu plate with heat-exchanging system) for 5 crystals

• Cryothermostat (LAUDA RC6CP) capable of temperature stabilization in the region of -35 °C --- +200 °C

• LED system to monitor PMT gain and crystals transparency in blue and red part of the visible spectrum

• Cs137 gamma source gives irradiation dose rate 100 rad/h and below

• Monitoring of temperature sensors ( Pt100 and Pt1000 class A ) at 6 points (2 on crystals)

Page 6: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 6

PANDA-IF picture

Cryothermostat

Crystal box

Page 7: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 7

PWO properties studies at low temperatures

Crystal # S(-19.4) / S(+18.5)

b4 2.83

b16 2.80

b17 2.75

b24 2.78

b30 2.84

Light output change before the irradiation with temperature change from +18.5 0C to -19.4 0C

Radiation hardness studies of PWO-II at PANDA dose rates (max 2 rad/hour) and -20 0C showed 20%-35% drop of DC output signal after 300-400 hours of irradiation

Page 8: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 8

PWO light transmittance recovery at -200C

Published at NIM A Vol 582/2 pp 575-580

Paper:First study of radiation hardness of lead tungstate crystals at low

temperatures

Page 9: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 9

Radiation hardness studies of PWO-II (high dose rate)

Still factor 1.4 enhancement of light output

Page 10: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 10

Forward Spectrometer EMC

• 7 meters from the interaction point

• Covers 3 m2

• Fine segmented sampling calorimeter with light collection by optical WLS fibers passing through holes in the scintillator and lead layers (shashlyk type)

• Not in magnetic field (PMT as photodetector)

• Working energy range 10 MeV – 10 GeV

Page 11: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 11

Testbeam setup

DC1M14 DC2DC3

DC4ECAL prototype Beam

• Spectrometer consisted of 4 drift chamber stations and a magnet to measure beam particle momentum precisely

• Calorimeter prototype installed on a movable platform

Page 12: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 12

Shashlyk prototype module parameters

9 modules assembled in matrix 3x3• 380 layers of 0.3-mm lead and 1.5-mm scintillator,

total length 680 mm• Transverse size 110x110 mm2

• Effective Moliere radius: RM=59 mm

• Effective radiation length: X0=34 mm

• Total radiation length: 20X0

• Light collection: 144 (1212) fibers BCF-91A (1.2 mm)

• PMT Hamamtsu R5800 as photodetectors

Page 13: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 13

Shashlyk modules production

Page 14: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 14

Shashlyk prototype pictures

3x3 matrix of shashlyk modules and PMT attached to the modules

Page 15: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 15

Minimum ionizing particle peak

Page 16: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 16

Energy Resolution dependence on energy

Page 17: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 17

Energy Resolution parameterization

σE /E = a/E b/√E c [%], E in GeV

Experiment data fit: MC data fit:

a = 3.5 ± 0.3 a = 0.0

b = 2.8 ± 0.2 b = 3.0 ± 0.3

c = 1.3 ± 0.04 c = 1.1 ± 0.7

Good agreement with MC without noise term.

Good agreement with previous studies of similar sampling modules at lower energies (2.9%/ √E at 220-370 MeV: Test beam study of the KOPIO shashlyk calorimeter prototype, G.Atoian, S.Dhawan,V.Issakov et al. CALOR-2004 Proceedings )

Page 18: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 18

Measured S-curve at 19 GeV

Real Position, cm

Xcog,au

Page 19: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 19

Position resolution (center) dependence on energy

Page 20: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 20

Position resolution parameterization

σx = a/√E b [mm], E in GeV

Experiment data fit: MC data fit:

a = 17.6 ± 0.9 a = 14.2 ± 0.6

b = 4.6 ± 0.9 b = 5.5 ± 0.9

Worst case – resolution at the module center.

Resolution near the module edge is 3 times better

Page 21: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 21

Shashlyk 8x8 cells prototype

• We plan to have another shashlyk testbeam run in 2008 with prototype of 8x8 cells

• Now prototype with 55mm x 55mm module sizes is under construction

• Testbeam studies includes prototype energy and position resolution as well as test of π0 reconstruction capabilities in the energy range up to 15 GeV

Page 22: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 22

Conclusions

• PWO-II radiation hardness at -200C studies showed deep light transmission drop (20%-35% at 2rad/hour) and low light transmission recovery rate

• Testbeam studies of energy and position resolution of shashlyk prototype (110x110mm cell) results:

– Energy σE /E = 3.5/E 2.8/√E 1.3 [%] – Position (at the cell center) σx = 17.6/√E 4.6 [mm] – Good agreement with MC results

• Further improvement of shashlyk parameters includes prototype with 55x55 mm cell size testbeam study

Page 23: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 23

Backup slides

Page 24: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 24

Radiation hardness temperature dependence

Page 25: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 25

MC shashlyk parameters

• Shashlyk module geometry including holes

• Tile att. length 70 cm

• Fiber att length 400 cm

• Reflection from tile edges diffusive

• Tot. internal reflection 0.97

• Tile light output 100 eV/photon

• Reemission probability in fiber 0.1

• Refraction in tiles and fibers 1.59

Page 26: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 26

S-curve MC (0.5 – 10 GeV)

Page 27: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 27

PANDA-IF electronics

• Based on i7k (ICP DAS) modules with RS485 interface

• Short connections (0.5 m) from PMT and temperature sensors to read-out electronics

• Temperature measurements with an accuracy better than 0.03 °C

• DC current measurements accuracy up to nA

• LED signals in DC mode – measurement of the mean current thru 10 kΩ generated by a bunch of pulses

• HV for PMTs: LeCroy1440 system

Page 28: PANDA electromagnetic calorimeters Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group INSTR08 28 Feb - 05 Mar 2008

3 March 2008 Pavel Semenov, INSTR08@BINP, Novosibirsk 28

PANDA-IF electronics diagram

7013PT1000

CAMAC

RS485 bus

Irradiation facilityControlroom

7017ADC

7042DO

LED generator

HV

Crystal Box

Shutter

LRS1440HV system

VME

Shutter digital control lines

RS232

DAQ computerLinux

RS485/RS232converter

LAUDA

PT1000

7 signal lines

Opt. fibers

RS232-CL

Cs137