Correlation of HO signal with DT

29
1 Correlation of HO signal with DT Gobinda Majumder T.I.F.R. Reconstruction of muon tracks and extrapolation to HO HO signals in different time slices Signal and cross talks Conclusion

description

Gobinda Majumder T.I.F.R. Correlation of HO signal with DT. Reconstruction of muon tracks and extrapolation to HO HO signals in different time slices Signal and cross talks Conclusion. Drift Chamber information. Do not have data base for all runs - PowerPoint PPT Presentation

Transcript of Correlation of HO signal with DT

Page 1: Correlation of HO signal with DT

1

Correlation of HO signal with DT

Gobinda MajumderT.I.F.R.

• Reconstruction of muon tracks and extrapolation to HO

• HO signals in different time slices

• Signal and cross talks

• Conclusion

Page 2: Correlation of HO signal with DT

2

Drift Chamber information• Do not have data base for all runs

• Only databases from Run# 2377 (Bon) and Run#2255 (no field for MTCC-I)

• Reconstruct DTRechit → DTRecSegment2D→DTRecsegment4D

• 3.8T field (Run # 2559-2618): Use StandaloneMuon reconstruction code (modified for MTCC, but field map is for 4 Tesla) and then extrapolate to HO (only 30 cm away)– Extrapolation without any information of database

• No field case (Run # 2476-2552): Use low uniform magnetic field (200 Gauss) to reconstruct muon track.

• MTCC-II : 4412-4438 (4T) and 4446-4457 (ZERO) field : Only Ring2 timing are useful. 3986-4020 (3.8T), but many variation of timings and connections.

Page 3: Correlation of HO signal with DT

3

Cosmic ray muon spectrum in MTCC-I

• Muon trigger is only in sector 10 (Vertically downward)• Momentum has to scale down by a factor 3.8/4• Known problem : Ratio of μ+ and μ– are not 1.3• Use muon with P>4 GeV and |θ–π/2|<0.5, |φ+π/2|<0.5, ndof>30

P (GeV) θ (rad)

Page 4: Correlation of HO signal with DT

4

Pixel configuration of Ring1&Ring2

• No difference in Ring1 and Ring2

• Look for signal in nearby six pixel (if there and also readout)

Page 5: Correlation of HO signal with DT

5

Time profile of Sector10, examples

• Variation of timing within few time period

Phase-I YB1

Phase-II YB2 (3.8T)

Phase-II YB1 (3.8T)

Phase-I YB2

Page 6: Correlation of HO signal with DT

6

HO signals and cross talk

• Signals only in Sector-10, φ=270o

• Use only time slice 2-5 for MTCC-I

• MTCC-II : 3-6 for Ring-I and 4-7 for Ring-2

• Pedestal is obtained from a single run, e.g., run# 3986 for data at 3.8T in phase-II

• Signal to the extrapolated HO towers as well as nearest towers (pixel and physical position of tower)

• To check random noise use same pixel in Ring-1(2), when extrapolated muon on Ring-2(1)

• To have better accuracy of extrapolation, events are selected where muon hits inside 10cm of an edge of HO tile

Page 7: Correlation of HO signal with DT

7

Stability of pedestals

• Pedestal values are stable over MTCC run period

Pedestal of all HO pixels for run# 3334-3338

Variation of pedestal for different runs (two of them)

Run # Run #

Page 8: Correlation of HO signal with DT

8

Signal in geometrically nearby tower

η=–1 Φ=–1

η=0 Φ=–1

η=+1 Φ=–1

η=0 Φ=0

η=+1 Φ=0

η=–1 Φ=0

η=–1 Φ=+1

η=0 Φ=+1

η=+1 Φ=+1

• There are some +ve signals in geometrycally nearby towers, due to extrapolation or pixel cross talk or both ?

-10 (fC) 20

-10 (fC) 20

-10 (fC) 20

-10 (fC) 20

-10 (fC) 20

-10 (fC) 20

-10 (fC) 20

-10 (fC) 20

-10 (fC) 20

Page 9: Correlation of HO signal with DT

9

Signal in geometrically nearby tower,but in different RM (ZERO field)

• Projection is not perfect, Muon reco/Extrapolation ?

Projected φ=55

Signal in Φ=56

Projected φ=56

Signal in Φ=55

∆η=–1 ∆η=0 ∆η=+1

fC

fC fC

fCfC

fC

Page 10: Correlation of HO signal with DT

10

Signal in geometrically nearby tower,but in different RM (3.8T field)

• Projection is not perfect, Muon reco/Extrapolation ?

Projected φ=55

Signal in Φ=56

Projected φ=56

Signal in Φ=55

∆η=–1 ∆η=0 ∆η=+1

fC

fCfCfC

fCfC

Page 11: Correlation of HO signal with DT

11

Uncorrelated noise level (muon in YB1,signal in YB2)

• In YB+1 case, we see some noise in presence of magnetic field

B=0 YB=1

B=0 YB=2

B=3.8TYB=2B=3.8T

YB=1

fC

fCfC

fC

Page 12: Correlation of HO signal with DT

12

Signals in towers of nearest pixel, Ring1 without any field (H,15)

• Little signal in nearby pixel

Up left

Up right

ProjectedRight

Left

Bot Left Bot

rightAll six

QADC (fC)

Page 13: Correlation of HO signal with DT

13

Signals in towers of nearest pixel, Ring1 with B=3.8T (H,15)

• Not much cross-talk, but signal height gone down

Up left

Up right

ProjectedRight

Left

Bot Left Bot

rightAll six

QADC (fC)

Page 14: Correlation of HO signal with DT

14

Signals in towers of nearest pixel, Ring2 with 3.8T (H,15)

• Little signal in up-right pixel

Up left

Up right

ProjectedRight

Left

Bot Left Bot

rightAll six

QADC (fC)

Page 15: Correlation of HO signal with DT

15

• Statistical error ~1-3%. Total cross talk is 5-10%.

Phase I data : Sector 10 @ZERO field

Page 16: Correlation of HO signal with DT

16

Phase I data : Sector 10 @3.8T field

• Cross talk increase to ~15% for ring 1

Page 17: Correlation of HO signal with DT

17

Phase II data : Sector 10 @ZERO field

Page 18: Correlation of HO signal with DT

18

Phase II data : Sector 10 @4.0T field

• No visible change in signal and cross-talk

Page 19: Correlation of HO signal with DT

19

Comparison of means with and without B-field

• There is no effect in ring-2, but ring-1 signal has gone down by a factor ~2, whereas cross talk is only about 10-25%

Page 20: Correlation of HO signal with DT

20

Comparison of HO signal and pedestal width in TB2006 & MTCC-I (no filed)

• Signal distribution is fitted with a (Gaussian (for ped)+Gaussian convoluted Landau (signal) in TB2006, for MTCC signal is fitted with only Gaussian convoluted Landau function

TB2006 MTCC

fC

fC

fC

fC

Pedestal Pedestal

Signal Signal

Page 21: Correlation of HO signal with DT

21

• qw

HO signal and pedestal width in TB2006

Sigma peak/sigma

Page 22: Correlation of HO signal with DT

22

HO signal and pedestal width in MTCC(zero field)

• Signal@ZERO field is comparable to TB2006 signal. Though signals are not consistent (in TB06 muons cover more path in the scintillator)

Page 23: Correlation of HO signal with DT

23

Conclusion

• There is negligible cross-talk in Ring-2 pixel (~0.2T)

• Ring-1 pixel shows increase in cross-talk of the level ~10% (0.3T)

• Similarly uncorrelated noise is very low ~4×10–4

• Irrespective of cross-talk, total signal has gone down with magnetic field.

Page 24: Correlation of HO signal with DT

24

• Many test on time slice, half of RM were not connected etc.

Page 25: Correlation of HO signal with DT

25

HO signal and pedestal width in MTCC(3.8T field)

Page 26: Correlation of HO signal with DT

26

Page 27: Correlation of HO signal with DT

27

Angle between Bz/By vs z, important to eliminate HPD xtalk

Page 28: Correlation of HO signal with DT

28

2000, 2003 preditions vs 2006 Hall probe, By

Field value also changes !

Field less than0.2T (2kG) needed to have no discharges in HO

Page 29: Correlation of HO signal with DT

29

Bfield measurements with moving Hall probes (vladimir epshteyn, slava)

YB/1

-0.5-0.4-0.3-0.2-0.1

00.1

0 500 1000 1500 2000

Distance, mm

B, T

Bx By Bz

YB/2

-0.8

-0.6

-0.4

-0.2

0

0.2

-2500 -2000 -1500 -1000 -500 0

Distance, mmB,

T

Bx, T By, T Bz, T

Hall probes installed during mtcc1/mtcc2 shutdowndata taken at 3.8T (Wednesday morning, oct-25-2006)And at 4.0T (Monday, oct-31-2006)

0,4T is no good,We want <0.2 T, need to displace box by ~70 cm

70cm