status of new tpc( Ⅱ ) performance study yohei nakatsugawa leps meeting in taiwan
TRANSCRIPT
Status of New TPC( )Ⅱ
Performance Study
Yohei Nakatsugawa
LEPS Meeting in Taiwan
What we have done
TEST experiment in October 2005 Ⅰ Pad Response Function
TEST experiment in December 2005 Ⅱ Position Resolution in X-Y plane
In all tests, only MWPC part was used.
Pad Response Functiones
timat
ed a
vala
nche
pos
ition
(mm
)
central pad position(mm)
estimated avalanche position(mm)
sigma= 6.99×10-2mm
mean = 0
Usually, Gaussian is used.
simulation (intrinsic)
I searched for better function …
avalanche position = 0 (fixed)
Pad Response Function
F(x)=1
(p1+p2 (x-p3)2) a
a=3.5
sigma = 4.431×10-2 mm
mean = 6.62×10-3 mm
p3 = avalanche position
Is this really better function?
Pseudo Lorentzian
better than Gaussian
TESTⅠ (October 2005)
55Fe
pulse motor
anodewire
trigger
To decide PRF,We measured the dependence of pad gain on hit position.
Source spot is on layer4.
TPC was set vertically and moved by 500μm step by pulse motor.(total: -2500~2500μm one pad width)
X-ray source (55Fe, 5.9keV) was used.collimator
One anode wire above the layer4 wasused as trigger.
layer4
32mm
3mm 16mm
x
y
z
y
pad plane 1mm
TEST set upⅠ
This is actually not a photo of TEST set up, but it was like this.Ⅰ
Analysis
Source event selection
Three pads in the source spot are hit.Other layers are not hit.
PRFmeasured(x) =∫ dx’ PRF(x’)*exp[ -{ x - x’ }2/(2*σ2) ]σ=1.106 (by Monte Carlo )
Unfolding the dispersion of X-ray
assuming Gaussian
Compare Gaussian and Pseudo Lorentzian
Analysis
measuredPseudo Lorentzian
Pseudo Lorentzian
Gaussian
χ2 Gaussian 10.5 Pseudo Lorentzian 5.2
Pseudo Lorentzian is better.
TEST ( December 2005 )Ⅱ
γ
Pd converter
magnet
e-
e+
up veto scintilator
start up start down scintilatorsolenoid
trigger condition: up start up start down
To see angle dependence of XY resolution, data were taken at0°(figure),±12.5°,±25° TPC angle.
rotation
Sector 1 & 4 could not be read out due to geometry in the hatch. (Cable length was not enough.)
~25cm
(~5cm width)
dipole
Layer9 was also read out.( new FADC)
TEST set upⅡTPC side view
e-
TEST set upⅡTPC side view
e-
TEST set upⅡTPC front view
TEST set upⅡsweep magnet
Flux is closed by iron planes.
TEST set upⅡsweep magnet
Typical Event Display
storage ring
top viewTPC angle 0°
Typical Event Display
TPC angle 12.5°
storage ring
top view
Typical Event Display
TPC angle 25°
storage ring
top view
Extra Data
γe-
e+
start up standard start counter
We just wanted to see multi-track and to read out all sectors!
trigger condition: Tag up start up STC
Typical Event Display
TPC angle 0°
storage ring
top view
Typical Event Display
TPC angle 0°
storage ring
top view
Analysis
require more than 4 layers are hit.
line fit tracking ( least square ) residual distribution
x position : estimated by PRF (PL)y position : center of layer
TPC angle : 0° sigma : 176μm
12.5°371μm
25°824μm
ADC value of pulse peak is used.
Time
peak
AD
C
Our goal …at least ~300μm too bad..Resolution is getting worse as track angle increase.
Analysis
y position in layer
Anode signal has random fluctuation. Anode which has large signal drags estimated hit position.
true positionestimated
In previous analysis,y position was fixed.(center of layer)
y position also have to be estimated. using anode information
true position
Analysis
using anode signal
y position = center of gravity of charge induced by 5 anode wires = ∑yi * wi * ADCi ( i = 1~5)
w1 = w5 = 0.1098 , w2 = w4 = 0.3776 , w3 = 0.4567
12345
not using layer1
no field cage Electric field may be distorted.
calibration of anode
using cosmic ray data ( taken after beam time ended ).
Actually, anode 1 & 27 (most outside) have lower gain in calibration data.
TPC angle : 0°sigma : 175μm
12.5°196μm
25°382μm
(176μm) (371μm) (824μm)
Analysis
Resolution is improved.
Analysis
Comparison with Gaussian PRF
175μm
196μm
382μm
192μm
197μm
383μm25°
12.5°
0°
Pseudo Lorentzian GaussianTPC angle
Pseudo Lorentzian is slightly better…
Intrinsic resolution
require 5 layers are hit
residual distribution in the middle layer.
track including and excluding the middle layer
σexc =54
σσinc =45
σ σ= σinc * σexc
0° 133μm12.5°163μm25° 331μm
intrinsic resolution
Next
X-Y position resolution was improved by using anode information,but is still over 300μm. further analysis
Study of Z-direction drift velocity, position resolution, dependence on dip angle …
We are waiting for completed new TPC !
DAQ collector has to be arranged for new FADC. ( The number of channel is different. 32ch 16ch )
Convention
1
2
3
45
6
1234567
89
x
y