sd – silicon detector em calorimetry

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28 June 2002 Santa Cruz LC Retreat M. Breidenba ch 1 SD – Silicon Detector EM Calorimetry

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SD – Silicon Detector EM Calorimetry. SD (Silicon Detector). Conceived as a high performance detector for NLC Reasonably uncompromised performance But Constrained & Rational cost - PowerPoint PPT Presentation

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Page 1: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 1

SD – Silicon Detector EM Calorimetry

Page 2: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 2

SD (Silicon Detector)

• Conceived as a high performance detector for NLC

• Reasonably uncompromised performance• But• Constrained & Rational cost

• We accept the notion that excellent energy flow calorimetry is required, and explore optimization of a Tungsten-Silicon EMCal…

Page 3: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 3

Silicon DetectorEM Calorimetry

Quadrant View

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0.000 2.000 4.000 6.000 8.000

m

m

Beam Pipe

Trkr

Ecal

Hcal

Coil

MT

Endcap

Endcap_Hcal

Endcap_Ecal

VXD

Endcap_Trkr

Page 4: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 4

Scale of EMCal & Vertex Detector

Page 5: SD – Silicon Detector EM Calorimetry

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Silicon Tungsten EMCal

• Figure of merit something like BR2/ where is the rms sum of Moliere radius of the calorimeter and the pixel size. – Maintain the great Moliere radius of tungsten

(9 mm) by minimizing the gaps between ~2.5 mm tungsten plates. Dilution is (1+Rgap/Rw)

– Could a layer of silicon/support/readout etc fit in a 2.5 mm gap? Even less?? 1.5 mm goal??

• Requires aggressive electronic-mechanical integration!

Page 6: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 6

EMCal, continued• Diode pixels between 5 – 10 mm square on largest

hexagon fitting in largest available wafer. (6” available now – 300 mm when??) Consider tracking as well as E flow in picking pixel dimension.

• Develop readout electronics of preamplification through digitization, zero suppression and IO on bump bonded chip. Upgrade would be full integration of readout on detector wafer. (R&D opportunity!)

• Optimize shaping time for small diode capacitance. Probably too long for significant bunch localization within train. But some detector element needs good time resolution!!!

Page 7: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 7

Channel Counts [Forget Them!!]

• We are used to pixel counts in CCD’s …– 3x108 last time, 1x109 this time, no problem

• Silicon Strip Tracker ~5x106 strips (channels??)

• EMCal ~5x107 pixels (channels??)• Don’t even think about multiplying channels

by O($10)……

• Must solve the cluster technology challenges.

Page 8: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 8

Structure

Page 9: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 9

Pixels on 6” Wafer

Page 10: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 10

Zoom to Readout Chip

Page 11: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 11

Gross System ArchitectureSilicon Diode Array

Readout Chip

Network Interconnect

Page 12: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 12

Cross Section

Page 13: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 13

Signal Collection from m2 board

Page 14: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 14

Preamplifier Architecture

• Charge amplifier and shaper followed by two amplifiers with gains G1,G2 and sample & holds.

• Comparator logic to select appropriate range

• Mux and 12 bit ADC

Shaper

G2

G1

MUX

12 bit ADC

Page 15: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 15

Noise and Muons

• Assume 300 (400-500 possible) effective e- collection at 80 e-/. signal ~ 24000 e-.

• Assuming diode capacitance of 0.3 pf/mm2, and amplifier noise of 20e-/pf+200e- – noise ~400 e-. S/N ~60, plenty good!

• Pick S/N of 7 (Figure) for minimum performance.

Noise & Muon Distributions

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0.4

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1

1.2

1.4

1.6

1.8

2

0 2 4 6 8 10 12Amplitude, SD Units

Pro

b

Noise

Noise,cum

Mu Signal

Signal, cum

Noise+Sig

Page 16: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 16

Plausible Resolution Criteria

• Spread the 0.6% muon into several bins, with enough range for MIP counting to a few.

• Preliminary Monte Carlo indicates peak ionizing track density from a high energy shower to be 2200 µ equivalent. (5 x 107 e- = 8 pC.)

• Do not degrade resolution of calorimeter! Energy resolution of a sampling calorimeter with 2/3 X0 plates will not exceed 12%/√E. Say this peak should be spread over 5 bins, and take no credit for multiple sampling.

• Relaxation of these requirements now being studied with EGS.

Page 17: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 17

Required Resolution

• High Res Bin Width=1000 e-, Emax=37 GeV,Mips=170• Low Res Bin Width=13200 e-,Emax=512

GeV,Mips=2325

Resolution vs Requirements

0.0E+00

1.0E+04

2.0E+04

3.0E+04

4.0E+04

5.0E+04

6.0E+04

0 100 200 300 400 500 600

Energy, (GeV)

Bin

Wid

th,

elec

tro

ns

12%*sqrt(E) *5 *105600

Low Gain

High Gain

Page 18: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 18

Technical Issues• Assuming integrator full scale voltage of

around 1 V, feedback (and calibration) capacitors need to be ~10 pF. This is large for an integrated capacitor, but doable with substantial real estate.

• Plus is that this makes the bump bond pitch easy!

Page 19: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 19

Thermal Management

• Cooling is a fundamental problem: GLAST system is ~2 mW/channel. Assume 1000 pixels/wafer and power pulsing duty factor for NLC of 10-3 (10 µsec @120 Hz), for 2 mW average power.

• Assume fixed temperature heat sink (water cooling) at outer edge of an octant, and conduction through a thick (6 oz) copper ground plane in the G10 motherboard.

• ΔT~10C.• This is fine, but it sure doesn’t work without power

pulsing!!! Holding the power down while maintaining the noise/resolution is a serious engineering challenge.

Page 20: SD – Silicon Detector EM Calorimetry

28 June 2002 Santa Cruz LC Retreat M. Breidenbach 20

Plans

• We (Oregon and SLAC) plan to develop this design in more detail and build prototype wafers and chips.

• Test detectors in 5 Tesla field.• If successful, develop board level chip.

• Build 1 wafer wide by about 25 X0 deep calorimeter for test beam.