Analysis on TB0904 Data Jianchun Wang Syracuse University
Jan 14, 2016
Analysis on TB0904 Data
Jianchun Wang
Syracuse University
09/08/09 Jianchun Wang 2
The Telescope
PixelVELO
Pixel
YX YX
120 GeV proton beam
Pixel
Y
Scint
RR(
X
Z
Y
Pixel & VELO use independent DAQ systems, sharing trigger signals from the same source.
VELO events and pixel events are matched offline. Pixel stations / modules are aligned within its own system and generate tracks. Velo sensors are aligned with respect to the pixel tracks. Pixel track event, corresponding Velo event ID and Velo alignment parameters are
saved in tracking data files. Pixel tracking data are fed to Vetra. Real VELO studies of R/ and irradiated RR sensors.
Just
a re
mind
er
09/08/09 Jianchun Wang 3
Introduction
Track is reconstructed from pixel hits and fit to straight line. Pixel hit resolutions. Track fit probability issue. Track projection error and multiple scattering effect. Alignment precision (not estimated yet).
Analysis of R/data. Cluster size vs pitch and track angles. Eta curve of charge sharing. Velo R resolution.
Analysis of irradiated RR sensors ( ongoing, not included).
09/08/09 Jianchun Wang 4
Residual On the 5th Station
Measurement – Track Projection (mm)
Num
ber
of E
ntrie
s (A
rb.
Uni
t)
Ncol > 1
Nrow > 1
Ncol = 1
Nrow = 1
DifferentScale
Resolution (m)
ResidualRemove
track
Ncol > 1 7.6 5.8
Ncol = 1 120.0 119.8
Nrow > 1 8.3 6.6
Nrow = 1 12.7 11.7
Binary readout5 pixel stations
Simulated through iterations track proj. error ~ 4.9 m
09/08/09 Jianchun Wang 5
Track Probability Issue
Simulation
parameters
N Row N Col
1 >1 1 >1
Probability 0.759 0.241 0.978 0.022
Resol (m) 11.7 6.6 119.8 5.8
Type Z (mm) X (10-3 X0)
X-pixel -450 9.5
Y-pixel -444 9.5
VELO 0 6.4
Y-pixel 317 12.5
X-pixel 514 9.5
Y-pixel 520 9.5
Non-gaussian
Prob (2, ndof)
Tra
cks
(arb
. U
nit)
Exclude Ncol = 1
With multiple scattering
Prob (2, ndof)
Tra
cks
(arb
. U
nit)
Expect
Seen Uniform dist for Ncol=1Gaussian for the rest
09/08/09 Jianchun Wang 6
Tracking Error
Multiple scatt.
Include Ncol=1
Residual (m)
x y
5 station
s
No No 7.47 6.32
No Yes 7.42 6.30
Yes No 7.73 6.53
Yes Yes 7.69 6.51
Multi-ccatt. only 2.07 1.74
4 station
s
Yes No 7.71 7.72
Yes Yes 7.68 7.68
Multi-scatt. only 1.85 1.85
5 pixel stations
Tracking Error from Pixel (m)
Y
X
Log
( nu
mbe
r of
tra
cks
)
Calculated without multiple scattering
Multiple scattering contributes 1.7-2.1m to track projection error.
One can select events of better tracking error.
Measurements of Ncol=1 improve track projection precision, although distort the track probability distribution.
09/08/09 Jianchun Wang 7
Look at R/Data
X ( mm)Y
( m
m)
Effective Track Angle (degree)
Signal (ADC)
Matched Hits
We took data at nominal 0, 4, 8, 12 degrees rotated around horizontal axis.
The effective angle is smaller due to concentric strips.
Pixel coverage
09/08/09 Jianchun Wang 8
Effective Track Angle (Degree)
Per
cent
age
of H
itsCharge Sharing (I)
Cluster Size
All pitches & track angle
Seed threshold = 6 ADC ~ 9.6 Ke
Side threshold = 3 ADC ~ 4.8 Ke
Strip pitch (40, 50) mNstrip = 1 Nstrip = 2
Nstrip = 3
R sensor of R/pair
Range: angle0.5
09/08/09 Jianchun Wang 9
Charge Sharing (II)
Pitch ( m)
40 – 5050 – 6060 – 7070 – 8080 – 90
90 – 100
Effective Track Angle (Degree)
(Nst
rip >
1)
/ N
tota
l (%
)
R/ data is split into 1 of angle & 10 m of pitch sub-samples.
Sub-samples of 0, 3, 7 and 11 are with reasonable large statistics.
Strip Pitch (m)(N
strip
> 1
) /
N to
tal (
%)
Angle ( )-0.5 – 0.52.5 – 3.56.5 – 7.5
10.5 – 11.5
09/08/09 Jianchun Wang 10
The Eta Curve
Track Hit Fraction
Center of Strip N Center of Strip N+1
Only Strip N has Charge
Clu
ster
Fra
ctio
n
Only Strip N+1 has Charge
( )
i
Cluster Fraction
ADC i N
ADC
One strip shift due to tracking precision
All pitches & angles
Nstrip = 1 removed
09/08/09 Jianchun Wang 11
The Eta Curves Of Small Pitches
Clu
ste
r F
ract
ion
Track Hit Fraction
Angle=0 Angle=3
Angle=7 Angle=11
Pitch = (40-50) m
Nstrip = 1 removed
09/08/09 Jianchun Wang 12
The Eta Curves Of Small Pitches
Clu
ste
r F
ract
ion
Track Hit Fraction
Angle=0 Angle=3
Angle=7 Angle=11
Pitch = (40-50) m
Cluster fraction=0 or1 correspond to nstrip=1, indicating how charge sharing varies with hit position.
09/08/09 Jianchun Wang 13
Velo Resolution Measurement
<Resid = 19.2 m
trk> = 8.0 m
Nevent = 175K
Rvelo – Rtrack (m)
Resid = 18.0 m
trk> = 5.1 m
Nevent = 12.5K
Rvelo – Rtrack (m)
Trk error = (pixel)1.85m (multi-scatt.)
<trk> = quadratic average over all trks
Tracking Error from Pixel (m)
Error < 6 m
To improve tracking precision one has to sacrifice statistics.
09/08/09 Jianchun Wang 14
Resolution vs Pitch
R sensor of R/pairV
elo
Hit
Res
olut
ion
(m
) Preliminary !.Angle ( )- 0.5 – 0.52.5 – 3.56.5 – 7.5
10.5 – 11.5
Strip Pitch (m)
Seed threshold = 6 ADC ~ 9.6 Ke
Side threshold = 3 ADC ~ 4.8 Ke
Tracking projection uncertainty removed from resolution.
Tracking precision is determined for each point ( ~ 4.7–5.4 m).
Error bar represents only statistic error.
Linear charge weighting, eta-correction not applied yet.
09/08/09 Jianchun Wang 15
Tracking Precision
For each track the projections on Velo and projected errors in both X and Y directions are calculated using the corresponding pixel resolutions. R and error in R is calculated from X/Y.
For each sample (point), the projection error is quadratically averaged over all tracks used.
Projection error due to multiple scattering is ~1.85 m obtained from simulation.
The alignment error is to be determined.
Angle ( )- 0.5 – 0.52.5 – 3.56.5 – 7.5
10.5 – 11.5
R E
rror
Fro
m T
rack
Pro
ject
ion
(m
)
Strip Pitch (m)
09/08/09 Jianchun Wang 16
Resolution vs Track Angle
Pitch ( m)
40 – 5050 – 6060 – 7070 – 8080 – 90
90 – 100
Effective Track Angle (Degree)
Vel
o H
it R
esol
utio
n (
m)
Effective track angle is determined in plane perpendicular to the strip.
Sub-samples of 0, 3, 7 and 11 are with reasonable large statistics.
Other angles are due to concentric strip, thus with small amount of hits.
09/08/09 Jianchun Wang 17
Summary
Pixel charge sharing is consistent with expectation.
Velo hit resolution is measured. The trend is as expected. But the value is not as good as we hoped.
RR studies are on going.
Explanation on Fanl tb09 VELO data, pixel tracks and supporting software can be found in 08/21/09 presentation. http://indico.cern.ch/getFile.py/access?contribId=5&resId=1&materialId=slides&confId=66615
Velo data, pixel data and pixel tracks (pixel track files will be updated with better alignment) are in /castor/cern.ch/lhcb/testbeam/lhcbvelo/fnaltb09
Track tool and a small example code ( Example.cpp, PixelTracks.cpp, PixelTracks.h, IPixelTracks.h ) can be found at http://phy.syr.edu/~jwang/projects/tb09/
09/08/09 Jianchun Wang 18
Data Sets
Detector Angle HV Setting Stations ADC
90 Lars90 Kazu
90, 20, 40 Chris P2V1 20.15 - 20.18 9ChrisLarsChrisLarsChrisLars
500 Lars500 + scan Chris500 + scan Kazu
8 500 + scan Kazu 5 P3V1 24.07 - 24.18 514 500 + scan Kazu 4.5+thin P4V1 26.06 - 26.15 630 500 + scan Kazu P5V1 26.19 - 27.09 77
500 + scan Kazu500 Chris
4 500 Kazu P5V3 27.20 - 27.22 99KazuChris
23
26
88
106
First
1
16
20
21.16 - 21.18
22.07 - 23.14
27.11 - 27.18
28.09 - 28.22
Time Range (date.hour )
21.08 - 21.10
21.12 - 21.14
19.13 - 20.11
VELO Pixel
0
8Rbottom
4
0RR
bottom
4
12
500
5
2-bit
binary
90
90
90
8RR top
RR middle
0
Geom Config
P2V2
P2V3
P1V1
P2V4
P2V5
P5V2
P5V4