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Jan Balewski, MIT FGT Project Review Detector requirements Disk layout e+/e- separation e/h discrimination Simu GEM response Strip layout, occupancy To-do- list Summary 1 2 3 4 5 6 FGT disks =1.0 =1.5 =2.0 FGT Layout Simulation Results e+ shower E T =40 GeV

FGT Layout Simulation Results

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 =1.0.  =1.5.  =2.0. 1 2 3 4 5 6  FGT disks. FGT Layout Simulation Results. Detector requirements Disk layout e+/e- separation e/h discrimination Simu GEM response Strip layout, occupancy To-do- list Summary. Jan Balewski, MIT FGT Project Review - PowerPoint PPT Presentation

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Page 1: FGT Layout   Simulation Results

Jan Balewski, MITFGT Project ReviewJanuary 7-8, 2008

• Detector requirements• Disk layout• e+/e- separation• e/h discrimination• Simu GEM response• Strip layout, occupancy• To-do- list• Summary

1 2 3 4 5 6 FGT disks

=1.0

=1.5

=2.0

FGT Layout Simulation Results

e+ shower ET=40 GeV

Page 2: FGT Layout   Simulation Results

2FGT Layout and SimulationsJan Balewski, MIT

FGT Requirements

1. Reconstruct charge of e+, e- from W decay for PT up to 40 GeV/c

2. Discriminate electrons against hadrons

• Allow for uniform performance for z-vertex spread over [-30,+30] cm• Fit in geometrical space free up by the West Forward TPC (FTPC)• Benefit from limited coverage of other trackers: IST, SSD• Relay on vertex reconstruction and Endcap shower-max hit• Relay on Endcap towers for energy reconstruction• Minimize amount of material on the path of tracks• Align FGT segmentation with TPC sector boundaries and Endcap halves• Assure relative alignment vs. TPC is double with real particles

Page 3: FGT Layout   Simulation Results

3FGT Layout and SimulationsJan Balewski, MIT

Optimization of FGT Disks Location in Z

Used TPC volumenHits>=5

SSDIST1,2beam

Zvertex=+30cm

Zvertex=0cm

1 2 3 4 5 6 R-‘unconstrained’ FGT disks

1 2 3 4 5 6 1 2 3 4 5 6

a)

b) c)Zvertex=-30cm

=1.0

=1.5

=2.0

En

dca

pE

MC

Barrel EMC

• 5 hits required for helix reco

• FGT sustains tracking if TPC provides below 5 hits

• use TPC, SSD,IST for Zvertex <~0 and <~1.3

• allow Zvertex[-30,+30]cm

FGT disks geometry: Rin=7.5cm, Rout=41cm, Z1…Z6=60…150cm, Z=18cm

Page 4: FGT Layout   Simulation Results

4FGT Layout and SimulationsJan Balewski, MIT

Optimization of FGT Disk Radii (Z Vertex = 0 cm )

Rxy – Z representation

TPCIf nHit>5 EndcapSMD

IST1,2

SSD

FGT 1 2 3 4 5 6

vertex

=1.

7

Rxy – representation

Used TPC volume

nHits>=5

=1.

0=

1.5

=2.0

En

dca

p

Zver=0cm

1 2 3 4 5 6 FGT

trac

k = 1

.7

Optimization Criteria

•Each track must cross the vertex and Endcap EMC

•6 FGT disk are needed to provide enough hits for tracks at all and all z-vertex

•Single track crosses less than 6 FGT disks

Page 5: FGT Layout   Simulation Results

5FGT Layout and SimulationsJan Balewski, MIT

Optimization of FGT Disk Radii (& location)

TPCIf nHit>5 EndcapSMD

IST1,2

SSD

FGT 1 2 3 4 5 6

vertex

a) Z Vertex = - 30 cm b) Z Vertex = 0 cm c) Z Vertex = + 30 cm

R-’unco

nstrained’

FGT d

isks

FGT disksfitting in available R-space

Critical FGT coverage depends on Z-vertex

FGT disks geometry: Rin=7.5cm, Rout=41cm, Z1…Z6=60…150cm, Z=18cm11.5 37.5 70

Page 6: FGT Layout   Simulation Results

6FGT Layout and SimulationsJan Balewski, MIT

1 of reco track

FGT Enables Reco of Sign of e+,e-

2mm

Sag

itta

(m

m)

100cm

Y/cm

40cm

20cm

X/mm

1.0Vertex=200m

Endcap SMDhit =1.5mm

reco track

Lim

it fo

r p T

tra

ck

3 FGT hits=70m

0

Sag

itta

(m

m)

2mm

2.0 mm

Sagitta=2mm

Wrong Q-signGood Q-sign

Page 7: FGT Layout   Simulation Results

7FGT Layout and SimulationsJan Balewski, MIT

Track & Charge Sign Reco EfficiencyFGT disks geometry: Rin=7.5cm, Rout=41cm, Z1…Z6=60…150cm, Z=18cm

N0 – thrown electrons, ET=30 GeV

N1 – reco tracks (<3 mrad) N2 – reco tracks w/ correct charge sign

•Track reco efficiency >80% for up to 2.0•Wrong charge reco <20% for above 1.5

Page 8: FGT Layout   Simulation Results

8FGT Layout and SimulationsJan Balewski, MIT

Zvert=0

Stability of Charge Reconstruction

Studied variations of efficiency (shown in proposal):- degraded FGT cluster resolution (80m 120m, OK)- reduced # of FGT planes (6 4 , bad, too few hits/track)- degraded transverse vertex accuracy (200m 500m, OK)- FGT cluster finding efficiency (100% 90%, OK , details)

- smaller FGT disk size & separation - OK

Rin=18cm, Rout=37.6cm, Z1…Z6=70…120cm, Z=10cm

Page 9: FGT Layout   Simulation Results

9FGT Layout and SimulationsJan Balewski, MIT

GeV

e/h Discrimination Capability of Endcap EMC

Projective tower

PreShowers

PostShower

ShowerMax

Shower from electron

E=30 GeV

=2.0

=1.08

Simu of Endcap response toElectrons (black) & charge pions (red) with ET of 30 GeV

Endcap+

e+

30 GeV0

+ e+

GeV

+

e+

~15 GeVE T Trigger

threshold

Page 10: FGT Layout   Simulation Results

10FGT Layout and SimulationsJan Balewski, MIT

e/h Discrimination : PYTHIA Events

Hadrons from PYTHIA M-CQCD events

e+, e- from PYTHIA M-C

W-events

Isolation & missing-PT cutssuppress hadrons by ~100

Page 11: FGT Layout   Simulation Results

11FGT Layout and SimulationsJan Balewski, MIT

Real Electrons Reconstructed in Endcap

e+, e-

M

IP

TPC P [6,8] GeV/c

e+, e-

MIP

TPC P [10,14] GeV/c

Endcap-based cuts Identified e+,e-

Page 12: FGT Layout   Simulation Results

12FGT Layout and SimulationsJan Balewski, MIT

Detailed Simulation of GEM Response (1)1. ionization and charge amplification2. spatial quantization on GEM grid3. charge collection by strip planes4. 1D cluster reconstruction

Primaryionization

Amplified signal is displaced

Hole in GEM foil amplifies charge

cloud

phi-axis strippitch=600m

R-a

xis

strip

Pitc

h=80

0m

x hit

Latice attractorsspaced 130 m

Charge from this hexagon is attracted by the hole

best

Page 13: FGT Layout   Simulation Results

13FGT Layout and SimulationsJan Balewski, MIT

Simulated FGT Response (2)

22 eV/pair

(760 eV/ track)14 prim pairs/track

32 any pairs/track

22 eV/pair 14 prim pairs/track

R=122mR*=40m

GE

M r

esp

on

se1D

Clu

ster

fin

der

res

olu

tio

n Test beam data

Page 14: FGT Layout   Simulation Results

14FGT Layout and SimulationsJan Balewski, MIT

FGT Strip Layout *)32

6 R

-str

ips

Top -layer949 -stripspitch 600m

x

y

Xz 15 deg

Endcap halves

y

x

*) close to final

Essential for PT reco

~ 50% transparency

needed for 3D track recognition, resolving ambiguities

FGT quadrant boundariesmatch to Endcap

segmentation

Bottom R-layerpitch 800m

Page 15: FGT Layout   Simulation Results

15FGT Layout and SimulationsJan Balewski, MIT

Estimation of Strip Occupancy

Track rate per strip for minB PYTHIA events @ s500 GeVBased on FGT geometry:Rin=15cm, Rout=41cm

R-strips45 deg long

2

0

1

trac

ks

R=41cm R=15cm =0 deg =90

1 track/strip

per 1000

minB events

trac

ks

0.8

0

0.4

1

-strips 400 m pitch

• pileup from minB events dominates•1.5 minB interactions/RHIC bXing• 300nsec response of APV 3 bXings pile up

Total pileup of 5 minB events per trigger event

• 1 tracks per FGT quadrant per minB event (scaled from simu below)

• Cluster size: 1mm along , 2mm along R

• Cluster occupancy per triggered event per quadrant • -strips (span ~43cm) 1.2% occupancy• R-strips (span 25cm) 4% occupancy(uncertainty factor of 2)

minB PYTHIA event @ s=500 GeV

Page 16: FGT Layout   Simulation Results

16FGT Layout and SimulationsJan Balewski, MIT

To-do List

• completion of detailed (a.k.a. ‘slow’) simulator for GEM response

• develop 3D tracking with pattern recognition

• include pileup from 3 events in reco of physics events

• implement and optimize full array of e/h discrimination techniques

• completion of full W event simulation and comparison to full hadronic QCD events simulation

• determine background contribution from Z0 and heavy flavor processes, above pT>20 GeV/c

Page 17: FGT Layout   Simulation Results

17FGT Layout and SimulationsJan Balewski, MIT

FGT Simulation Summary

1. Will be able to reconstruct charge of e+, e- from W decay for PT up to 40

GeV/c with efficiency above 80%

2. There is enough information recorded to discriminate electrons against hadrons

• Allow for uniform performance for z-vertex spread over [-30,+30] cm, OK• Will fit in geometrical space• Will use hits from IST, SSD• Will relay on vertex reconstruction and Endcap shower-max hit & energy• FGT quadrants are aligned with TPC sector boundaries and Endcap halves• FGT disks 1 &2 overlap with TPC allowing relative calibration

Page 18: FGT Layout   Simulation Results

18FGT Layout and SimulationsJan Balewski, MIT

BACKUP

Page 19: FGT Layout   Simulation Results

19FGT Layout and SimulationsJan Balewski, MIT

Compact FGT- proof of principle

Critical FGT coverage depends on Z-vertex

Rin=18cm, Rout=37.6cm, Z1=70cm, …,Z6=120cm, Z=10 cm

Page 20: FGT Layout   Simulation Results

20FGT Layout and SimulationsJan Balewski, MIT

FGT Material budget UPGR13, maxR=45 cm

Z vert= - 30cm Z vert= 0cm Z vert= + 30cm

0

0.5

0

0.5

Page 21: FGT Layout   Simulation Results

21FGT Layout and SimulationsJan Balewski, MIT

FGT Material UPGR13 w/o SSD

Page 22: FGT Layout   Simulation Results

22FGT Layout and SimulationsJan Balewski, MIT

TPC reco with 5 points

‘regular’ tracking5-hits tracking

‘regular’ tracking5-hits tracking

Page 23: FGT Layout   Simulation Results

23FGT Layout and SimulationsJan Balewski, MIT

Alternative Snow-flake Strip Layout

As in Proposal

12-fold localCartesianref frame

Page 24: FGT Layout   Simulation Results

24FGT Layout and SimulationsJan Balewski, MIT

Track Reco Strategy1. Select EMC cluster with large energy

2. Eliminate all FGT hits outside the cone: vertex SMD hit

3. Resolve remaining ambiguities comparing R vs. charge

4. Consider shorter -strips (snow flake design)

1 2 3 4 5 6 FGT

1

2

3

4