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Home > Documents > 1 HFT Technology and Mechanical Design Wieman RNC LBNL TAC Review Wed. 11:30 – 12:05 15-Mar-2006.

1 HFT Technology and Mechanical Design Wieman RNC LBNL TAC Review Wed. 11:30 – 12:05 15-Mar-2006.

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1 HFT Technology and Mechanical Design Wieman RNC LBNL TAC Review Wed. 11:30 – 12:05 15-Mar-2006
Transcript

1

HFT Technology and Mechanical Design

Wieman RNCLBNL

TAC ReviewWed. 11:30 – 12:05 15-Mar-2006

2

Topics

Requirements and features CMOS APS Detector Technology

APS Introduction Basis for Technology Choice Development history Efficiency vs Accidentals based on electron beam measurements R&D plan, a 4 ms chip followed by a 0.2 ms chip Detector Verification in STAR Environment

Mechanical Concept Minimum mass ladders Single end support

Stable reproducible spatial alignment Rapid insertion and removal

Thin beam pipe system Conclude with summary of R&D issues

3

Requirement

Detect low momentum D’s in the environment of high multiplicity heavy ion collisions and high luminosity at RHIC in the most effective manner consistent with available resources

4

Some HFT features

Pointing resolution (13 12GeV/pc) m

Layers Layer 1 at 1.5 cm radiusLayer 2 at 5 cm radius

Hit resolution 8.7 m

Position stability 10 m

Radiation thickness per layer

X/X0 = 0.28%

Beam pipe radiation thickness

X/X0 = 0.14%

Number of pixels 98 M

Raw data rate 31 GBytes/sec

Stored data rate after sparcification

90 MBytes/sec

Integration time (affects pileup)

R&D phase 4 msFinal detector 0.2 ms

Rapid installation and replacement

Reproducible positioning

5

6

MIMOSTAR APS uses forward biased diode

Pixel signal read every 4 msCorrelated double sample (CDS) – the difference between each sample

Decay time is long compared to sample period ~100 ms

7

Basis for CMOS APS Technology Choice

Hybrid technology (silicon pixels bump bonded to ASIC readout) Advantages:

Very fast, short integration time, no pileup Potential for trigger generation Rad hard Well established technology, ATLAS etc

Disadvantages: Too thick for optimum pointing accuracy required for low momentum D

meson reconstruction Additional mass required for cooling Requires establishing complicated partnerships for production and

testing (can’t just buy units)

8

Basis for CMOS APS Technology Choice

CCD technology Advantage:

Successfully used in high precision vertex detector, VXD3 of SLD Disadvantages:

Limited radiation tolerance Sufficient readout speed pushes technology boundaries Limited industry access

DEPFET technology Advantages:

Excellent signal to noise Sophisticated thin ladder structures High speed Probably RAD hard

Disadvantages: Single foundry Highly specialized one of a kind technology No currently installed systems

9

Basis for CMOS Technology Choice

CMOS APS technology Advantages:

Relatively RAD hard Available through multiple standard CMOS foundries Inexpensive commercial thinning Good success rate making working detectors by many institutions Excellent position resolution and fine granularity Partnered with the leading institution, IReS (now IPHC) in Strasburg Young technology, can expect considerable growth in capability

Disadvantages: Young technology for vertex detectors, currently no installed systems Limited signal to noise Current designs have relatively long integration times, i.e. potential

pileup at highest luminosities

10

Si Pixel Developments in Strasbourg

Mimosa – 1 4k array of 20 m

pixels with thick epi layer

Mimosa – 4 Introduce Forward

Biased Diode Mimosa – 5

1M array of pixels, 17 m pixels using AMS 0.6 process

Used at LBNL for ladder development

Mimosa – 8 Fast parallel column

readout with internal data sparsification

MimoSTAR – 1 128x128 pixels using TSMC 0.25 MimoSTAR – 2 128x128 pixels using AMS 0.35

– Duct tape these to the STAR Beam Pipe for 07 run

MimoSTAR – 3 320x640 pixels using AMS 0.35 MimoSTAR – 4 640x640 pixels production run

Ultra – 1 Ultra – 2

11

IReS MIMOSTAR chips

MIMOSTAR1 (0.25 m TSMC) Reduced size prototype but

sophisticated chip with complete functions for operation in a real detector system

Everything operating except pixel signal because of 0.25 m TSMC feature: Unexpected short signal decay time compared to theory and AMS experience.

MIMOSTAR2(0.35 m AMS optical process) Tested in beam 700-800 e most probable for Min-I 10-12 e-rms, noise. Signal decay time 100 ms

12

MIMOSTAR2, features

Parallel voltage out - for readout chip (abandoned)

Serial current loop out – for off ladder ADC up to 80 MHz

128 X 128 ½ Standard forward bias design ½ Rad Hard forward bias design, reduced

oxide Leakage Current 3-5 fA at room

temperature, shot noise adds 4 e-rms for 4 ms integration (total noise 16 e-rms)

Min-I cluster signal 700-800 e Successful radiation test, 20 Krad OK

13

Ultimate (fast APS detector) - good for high luminosity at RHIC

Submitted requirements list to IReS. In discussion

Technology MIMOSA8

Ladder active area 2cm 20cm

Pixel size 30m 30m

~Pixel mapping on the ladder 640 6400

Minimum operating distance from beam 1.5 cm

Power 100 mW/cm2

Operating temperature 30 C

Integration time[1] 0.2 ms

Mean silicon thickness 100m

Readout time 1 ms

Efficiency (min I)[2] 98%

Accidental cluster density 50/cm2

Binary readout, number of threshold bits[3]

2

Radiation tolerance [4] 124 kRad

Number of conductors supporting the ladder (10 chips/ladder)[5]

140

Triggered readout, maximum trigger delay[6]

2 s

14

Ultimate Chip

640X640 30 m pixels 200 sec integration time, a

factor 20 improvement, will work at the highest luminosities

Digital readout, 3 bit ADCs, i.e. CDS plus two threshold levels

4 parallel LVDS lines 1 ms readout and dead time Feasibility of this concept

proven with MIMOSA8 Multiple analogue storage on

the pixel for reduced dead time? Not clear that this option is possible.

4ch LVDS

640

640

15

Efficiency vs Accidentals

A critical issue with thin APS CMOS detectors Can data sparcification be achieved without loss of efficiency? Following study shows that planned simple high speed

algorithm will work

16

Accidental vs Efficiency Test based on Measured charge spectrum

APS measured signal spectrum in ALS electron beam agrees with Bichsel theory

To find efficiency add large measured signals scaled to distribution to empty APS noise frames and apply filter algorithm

Find accidental rate by using filter algorithm on empty noise frames

noise contribution

17

Test of two threshold algorithm

Require > 98% efficiency # of accidentals

Limit set by outer layer background rate

< 5 hits/cm2

Data shows stable region of good efficiency and low noise

18

Event size and data rate, data reduction crucial

Some numbers:

Itemnumber

bits/address 18

inner ladders 6

outer ladders 18

half chips per ladder 20

ave hits/half chip, inner, L = 1027 200

ave hits/half chip, outer, L = 1027 40

Only the hit addresses generate significant data volume. The totals are:

Itemnumber

Event Size 90 kBytes

Data Rate at 1 KHz event rate 90 Mbytes/sec

The HFT event size is significantly smaller than the TPC which has an event size of 2 MBytes for central Au+Au

Raw data rate: 31 GBytes/sec

Reduction 1/340,000

19

R&D Plans, Scope change

R&D phase for technology verification using MIMOSTAR2 (4 ms integration) technology Install n 4 ladder modules Verify mechanical insertion technology and stability control Verify DAQ and data reduction technology

Final phase MIMOSTAR-Ultimate (200 s integration) Full 24 ladder, 2, installation Multiple backup copies for rapid repair The full luminosity solution

20

Main R&D effort this year

Build two ladders with two MIMOSTAR2 chips each ( each chip 4 mm x 4 mm)

Install chip to chip (for coincidence) at an intersection region, preferably STAR

Operate with DAQ 1000 ALTERA/NIOS/SIU-RORC based system and STAR trigger interface

Gain operating experience and obtain track density numbers at small radius

21

Mechanical

Mechanical support Beam pipe

22

HFT Mechanical requirements

Full self consistent spatial mapping prior to installation

Installation and removal does not disturb mapping

Rapid replacement

10 Micron stability

(mapping of BarBar with visual coordinate machine)

23

Conceptual mechanical design

24

25

26

Kinematic mounts

27

Beam pipe

Meetings and discussions with Wolfram FisherDick HseuhRobert PakDan Weiss

•Our beam radius OK for accelerator, but we are a limiting aperture•Accelerator can live with 10-5 (we expect 10-9, but what can we live with?)•PHENIX has adopted our 1.5 cm radius, 0.5mm wall.•Preferred bake out 200-250 C to activate NEG coating

28

Important R&D Issues - Electronics

Question Solution status

Chip thinning Thin and test (APTEK) Done with earlier chips, MIMOSTAR needs testing

Off chip digitization and data sparcification

ADC/FPGA/SRAM daughter board

On going

Analog signal path buffer/FLEXcable/Drivers/twisted pair/ADC

In design

Latchup and recover BNL SEU test facility/PS control

Planning

STAR particle background at small radius

Measure with test ladders Planning

DAQ and Trigger interfaces Build prototype ladders and readout

In progress

Full size chip and readout in STAR environment

Part of 4 ms system To do

Scaling chip design mm to cm and to production quantities (4 ms design)

Prototype and Engineering runs with testing

On going

Scaling chip design mm to cm and to production quantities (0.2 ms design)

Prototype and Engineering runs with testing

On going

29

Important R&D Issues - Mechanical

Question Solution status

Maintain 10 micron stability and reproducibility

Design Ladders and do vibration tests

In progress

Ladder thermal distortion tests

In progress

Design support arms and test

To do

Design Kinematic couplers and test

To do

Design Transfer mechanics and test

To do

Design Metrology tools and test

To do

Measure and Analyze STAR thermal and vibrational environment

Initial test done, more to do

Maintain highly regulated temperature control

Analyze and Design cooling systems

To do

Interface to IST Analyze and Design To do

Small beam pipe issues Design and insert To do

30

Conclusion


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