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Rl
A
R fb
Cfb
Cac
+Bias
A
R fb
Cfb
A
R bf
Cfb
v0
v1v2
V0,out
V1,outV2,out
A simple detector model to describecrosstalk in segmented detectors
Bart Bruyneel, IKP Köln 2006
AGATA:
Cac = 1000pF
Cfb = 1.2pF
A (Core) = 80000
A (Seg) = 10000
(Rl = Rfb = 1G)
Small signal equivalent scheme
Z00 i0
Z22
i2
Z 11
i 1
Z02 Z 0
1
Z12
v1v2
v0 Seg–to –ground impedances Zii
Seg–to –Seg capacities: Zi,j = (sCij)-1 ; i≠j
Currents to electrodes:
Potentials at electrodes:
Small crosstalk if:
are small compared to
Segment-to-ground impedance Zii
and Core-to-gound impedance Z00
Z00 i0
Z22
i2
Z 11
i 1
Z02 Z 0
1
Z12
A
R fb
Cfb
vi
Vi,out
ACfb
V0,out
Rfb
A
AVi
ii
Miller EquivalentMiller Equivalent
Zii ~ (sACfb)-1
ACfb
V0,out
Rfb
A
AV0
i0
Cac
Cac~ 1nF
ACfb ~ 10nF
Z00 ~ (sCac)-1
ImpedanceImpedanceIn realityIn reality
A
R fb
Cfb
V0,outCac
v0
Seg
men
tsS
egm
ents
Co
reC
ore
SummaryRl
+Bias
v0
v1v2
ACfb
V0,out
Rfb
A
AVi
ii
ACfb
V0,out
Rfb
A
V0
i0
CacA
i
ACCCC
ACCCC
ACCACC
sCfbac
fbac
fbfb
fbout
1
1
1
1
v
1202
1201
0201
Core-to-Seg Segment-to-Segment
Segment-to-Core
Since Cac << ACfb, Core-to-Segment
crosstalk dominates
C0-X4 = 1.19 pF
C0-X5 = 1.16 pF
C0-X6 = 0.98 pF
C0-X1 = 0.943 pF
C0-X2 = 0.666 pFC0-X3 = 0.980 pF
Agata Agata measured capacities:measured capacities:
Core and Segment crosstalk
T020102012,
T2
T0201011,
T1
1202
1201
0201
1)1(1 v
11 :doubles
11 v
011 :singles
1
1
1
1
v
acacfbout
acacfbout
fbac
fbac
fbfb
fbout
CCxCCxACCxxC
xxi
CCCCACC
i
i
ACCCC
ACCCC
ACCACC
sC
Core normalization
Seg. normaliz.
Observed shift in segments
acac CCCC 0201 1sumSegment
-0.002
-0.0015
-0.001
-0.0005
0
0 10 20 30
CrosstalkMatrixSegments
0 10 20 300
10
20
30
Experiment
Segment sum shifts in 2-folds vs. hit pattern
Theory
Segment 1
Seg
men
t 2
Experiment
Segment 1
Seg
men
t 2
Column averages
Seg 1
Re
lativ
e s
hift
s theoryExp.
D3: problem“R
ing
2”
Ring toneighbor
Cac
1000pF800pF600pF
Core shifts in singles (experimental)R
ela
tive
sh
ifts
-5.00E-04
-4.00E-04
-3.00E-04
-2.00E-04
-1.00E-04
0.00E+00
1.00E-04
2.00E-04
0 5 10 15 20 25 30 35
Segment Number