Post on 18-Jan-2016
description
1
First results on electric field distribution First results on electric field distribution in irradiated epi-Si detectorsin irradiated epi-Si detectors
E. Verbitskaya, V. Eremin, Ioffe Physico-Technical Institute of Russian Academy of Sciences
St. Petersburg, Russia
A. MacchioloMax-Planck-Institut fuer Physik, Munich
11 RD50 Collaboration WorkshopCERN, Geneva, Nov 12-14, 2007
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1. Background: E(x) distribution in heavily irradiated detectors
2. Approach for simulation of detector Double Peak response and E(x) profile reconstruction with a consideration of electric field
in the “neutral” base
3. Experimental current pulse response in epi-Si SMART detectors irradiated by 1 MeV neutrons and 26 MeV protons and E(x) profiles
4. E(x) profiles in epi-Si detectors reconstructed from current pulse response
Conclusions
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
OutlineOutline
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Electric field distribution in heavily irradiated Si detectors
Heavily irradiated detector: Double Junction (DJ) structure:
Z. Li, H. W. Kraner, IEEE TNS 39 (1992) 577
Two depleted regions and a neutral base in-between
D. Menichelli, M. Bruzzi, Z. Li, V. Eremin, NIM A 426 (1999) 135
Two depleted regions and a base in-between with electric field due to potential drop over high resistivity bulk
E. Verbitskaya et al. NIM A 557 (2006) 528-539; “Concept of Double Peak electric field distribution in the development of radiation hard silicon detectors; pres. RESMDD’6, NIM A (in press)
Experimental verification:
A. Castaldini, A. Cavallini, L. Polenta, F. Nava, C. Canali, NIM A476 (2002) 550
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
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Approach for simulation of detector Double Peak response and E(x) profile reconstruction
with a consideration of electric field in the “neutral” base
Transient current:
Ntr = f(F)
trto ed
EQti /
p+ n+
E1
Eb
E2
W1 Wb W2
h
trthtr Nv
1
Three regions of heavily irradiated detector structure are considered Reverse current flow creates potential difference and electric field in
the neutral base
1) E. Verbitskaya et al. NIM A 557 (2006) 528;2) E. Verbitskaya, Concept of Double Peak electric field distribution in the development of radiation hard silicon detectors; pres. RESMDD’6, NIM A (in press)
Initiated by PTI, developed in:
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
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i ~ exp(-t/eff)
p+ n+ Signal due to carrier drift in W1 is independent on the properties of Wb and W2
i = i1 ~ exp(-t/tr)
W1, Neff1, E1
tcol
tcol: depends on Eb and Wb Eb, Wb
Charge collected inside W2
QW2
QW2 = Qo(d – W1 –Wn)/d Wb, W2, E2, Neff2
Edx = V
Simulation of detector Double Peak response and E(x) profile reconstruction
with a consideration of electric field in the “neutral” base
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
6
New development of E(x) profile reconstruction with a consideration of electric field in the “neutral” base
Current pulse response is considered as drift current
i(t) = enE(x)
Correction for carrier trapping is done
trcorr ttiti /exp)()(
r is parameter dependent on fluence
Edx = V at x = d
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
Special algorithm and software are developed which give direct calculation of the electric field distribution
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Current pulse response in irradiated epi-Si SMART detectors
Detectors: SMART, p+ - n-epi Si - n+ wafer
Experimental Technique: TCT setup at Ioffe Institute TCT setup response 0.8 ns Temperature range 77 – 373K Laser wavelength 830 m
All experiments: Laser at p+ side: electron collection
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
Epi-layer thickness: 150 m
# irradiation equiv. fluence (cm-2)T time (min)
W12 SMG22 26 MeV protons 7.00E+14 80C 60
W13 SMG 15 1 Mev Neutrons 8.50E+14
W12 SMG 15 1 Mev Neutrons 8.50E+14 80C 60
annealing
no annealing
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Current pulse response in proton irradiated epi-Si SMART detectors
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
SMART W12 SMG22, epi-Si, 26 MeV protons, Fp = 7e14 cm-2, p+ side
-0.002
0
0.002
0.004
0.006
0.008
0.01
0.012
0.0E+00 2.0E-09 4.0E-09 6.0E-09 8.0E-09 1.0E-08 1.2E-08 1.4E-08 1.6E-08
time (s)
sig
na
l (V
olt
)7.1 V
7.9 V
9.6 V
11.9 V
14.4 V
16.9 V
21 V
25.4 V
29.9 V
36.5 V
44.1 V
53.8 V
64.5 V
78.2 V
93 V
111.7 V
133.3 V
158.9 V
189.5 V
Room temperature
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Current pulse response in proton irradiated epi-Si SMART detectorsSMART W12 SMG22 epi-Si, 26 MeV protons, Fp = 7e14 cm-2, p+ side
0.008
0.0085
0.009
0.0095
0.01
0.0E+00 2.0E-09 4.0E-09 6.0E-09 8.0E-09 1.0E-08 1.2E-08 1.4E-08 1.6E-08time (s)
sig
na
l (V
olt
)19 V
30 V
40 V
51 V
61 V
71.8 V
81.8 V
92.8 V
103.9 V
113.8 V
124.8 V
134.9 V
145.8 V
155.8 V
166.8 V
176.8 V
187.7 V
198.7 V
-10 C
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
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Current pulse response in proton irradiated epi-Si SMART detectors
Full depletion at -10C occurs at higher V
W12 SMG22, 26 MeV, Fp = 7e14 cm-2, RT
-0.001
0
0.001
0.002
0.003
0.004
0.005
0.006
0.007
0.008
0 2 4 6 8 10 12 14 16
time (ns)
sig
na
l (V
)
29.9 V
36.5 V
44.1 V
53.8 V
78.2 V
W12 SMG22, 26 MeV, Fp = 7e14 cm-2, -10C
0.008
0.0085
0.009
0.0095
0 2 4 6 8 10 12 14 16time (ns)
sig
nal
(V
)
71.8 V
81.8 V
92.8 V
103.9 V
113.8 V
26 MeV protons, Fp = 7e14 cm-2
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
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E(x) and Neff(x) profiles in proton irradiated epi-Si detectors
Neff(x), W12 SMG22
-8E+12
-6E+12
-4E+12
-2E+12
0
2E+12
4E+12
6E+12
8E+12
0 0.005 0.01 0.015
x (cm)
Nef
f (c
m-3
)
29.9 V36.6 V44.1 V53.8 V78.2 V
E(x), W12 SMG22
0
2000
4000
6000
8000
10000
0 0.005 0.01 0.015x (cm)
E (
V/c
m)
29.9 V
36.6 V
44.1 V
53.8 V
78.2 V
Room temperature
RTE (x) epi-Si W12 SMG22. T = -10C
0
2000
4000
6000
8000
10000
12000
14000
0 0.005 0.01 0.015x (cm)
E (
V/c
m)
71.8 V
81.8 V
92.8 V
103.9 V
113.8 V
T = -10C
Neff(x)
-1.5E+13
-1E+13
-5E+12
0
5E+12
1E+13
1.5E+13
0 0.005 0.01 0.015
x (cm)
Nef
f (c
m-3
)
71.8 V
81.8 V
92.8 V
103.9 V
113.8 V
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
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E(x) and Neff(x) profiles: comparison at different temperatures
E(x), W12 SMG22
0
2000
4000
6000
8000
10000
0 0.005 0.01 0.015x (cm)
E (
V/c
m)
RT, 78 V
-10C, 82 V
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
E(x), W12 SMG22
-1.5E+13
-1E+13
-5E+12
0
5E+12
1E+13
1.5E+13
0 0.005 0.01 0.015
x (cm)
Ne
ff (
cm
-3)
RT, 78 V
-10 C, 82 V
Base region exists near the p+ contact:
RT: V≤40 V -10C: V≤80 V
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Current pulse response in neutron irradiated epi-Si SMART detectors
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
W13 SMG15
-0.0005
0
0.0005
0.001
0.0015
0.002
0.0025
0.003
0.0035
0.004
2 4 6 8 10 12 14
time (ns)
sig
na
l (V
)
18.1 V
21.1 V
38.7 V
56.7 V
74 V
92.2 V
110 V
126.5 V
143.3 V
159.4 V
173.3 V
186.3 V
197.3 V
214.2 V
203.3 V
196.1 V
181.3 V
166 V
152 V
as-irradiated
Reverse current is significant at V>200 V
W13 SMG15, Fn = 8.51014 cm-2, as-irradiated
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Current pulse response in neutron irradiated epi-Si SMART detectors
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
W12 SMG15
0
0.001
0.002
0.003
0.004
0.005
0.006
0.007
2 4 6 8 10 12 14
time (ns)
sig
nal
(V
)
6.8 V
24.3 V
44.1 V
64.6 V
84.5 V
105.6 V
126.8 V
147 V
168.4 V
189.9 V
211 V
232.4 V
253.3 V
274.6 V
294.7 V
315.7 V
334.5 V
355.2 V
376.6 V
annealing 80C, 60 min
W12 SMG15, Fn = 8.51014 cm-2, annealed 80C, 60 min
15
Current pulse response in neutron irradiated epi-Si detectors
0.00E+00
1.00E-03
2.00E-03
3.00E-03
4.00E-03
5.00E-03
6.00E-03
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15
84.5 V
105.6 V
126.8 V
147.1 V
189.9 V
W12 SMG 15annealing 80C, 60 min
SMART W13 SMG15 epi-Si, 1 MeV neutrons, Fn = 8.5e14 cm-2
-0.001
0
0.001
0.002
0.003
0.004
0 2 4 6 8 10 12 14 16
time (ns)
sig
nal
(V
)
21.1 V
38.7 V
74 V
92.2 V
143.3 V
173.3 V
186.3 V
I-V characteristics
0
200
400
600
800
1000
1200
0 50 100 150 200 250 300 350 400
bias voltage (V)
reve
rse
curr
ent
(uA
)
W13 SMG15, as-irradiated
W12 SMG15, 80C, 60min
Annealing results in significant reduction of current.
Increase of electric field near the interface wafer-epi-layer due to carrier trapping from enhanced current at higher V?
E. Verbitskaya et al., 11 RD50 Workshop, CERN
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E(x) and Neff(x) profiles in neutron irradiated epi-Si detectors
E(x)
0
5000
10000
15000
20000
25000
30000
35000
0 0.002 0.004 0.006 0.008 0.01 0.012 0.014x (cm)
E (
V/c
m)
84.5 V
105.6 V
126.8 V
147.1 V
189.9 V
W12 SMG 15annealing 80C, 60 min
Neff(x)
-2.5E+13
-2E+13
-1.5E+13
-1E+13
-5E+12
0
5E+12
1E+13
1.5E+13
2E+13
2.5E+13
0 0.005 0.01 0.015
x (cm)
Ne
ff (
cm
-3)
84.5 V
105.6 V
126.8 V
147.1 V
189.9 V
W12 SMG 15annealing 80C, 60 min
W13 SMG15, E(x)
0.0E+00
5.0E+03
1.0E+04
1.5E+04
2.0E+04
2.5E+04
3.0E+04
3.5E+04
4.0E+04
0 0.005 0.01 0.015x (cm)
E (
V/c
m)
109.9 V
126.5 V
143.3 V
173.3 V
186.8 V
W13 SMG 15as-irradiated
W13 SMG15, Neff(x)
-6E+13
-4E+13
-2E+13
0
2E+13
4E+13
6E+13
8E+13
0 0.005 0.01 0.015
x (cm)
Nef
f (c
m-3
)
109.9 V
126.5 V
143.3 V
173.2 V
186.8 V
W13 SMG 15as-irradiated
W13 SMG15, as-irradiated W12 SMG15, anneal 80C, 60 min
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
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E(x) and Neff(x) profiles: comparison of as-irradiated and annealed detectors
E(x)
0.0E+00
5.0E+03
1.0E+04
1.5E+04
2.0E+04
2.5E+04
3.0E+04
3.5E+04
4.0E+04
0 0.005 0.01 0.015x (cm)
E (
V/c
m)
143 V
187 V
147 V
190 V
no anneal
80C, 60 min
Neff(x)
-5.0E+13
-4.0E+13
-3.0E+13
-2.0E+13
-1.0E+13
0.0E+00
1.0E+13
2.0E+13
3.0E+13
0 0.005 0.01 0.015
x (cm)
Ne
ff (
cm
-3)
143 V
187 V
147 V
190 V
no anneal
80C, 60 min
E(x) Neff(x)
E at n+ contact is higher in as-irradiated detector
Low field base region near p+ contact exists in both detectors, annealing doesn’t eliminate it
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
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Trapping time constants
Proton irradiated, 71014 cm-2: 1.6-1.8 ns
Neutron irradiated, 8.51014 cm-2:
1.1 ns – as-irradiated 1.4 ns - annealed
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
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Conclusions
SCSI occurs in epi-Si detectors irradiated by 26 MeV protons and 1 MeV neutrons (F = (7-8)1014 cm-
2).
DP response in epi-Si irradiated detectors is related with base region rather than with DP E(x). Electric field in the base regions arises from current flow and potential drop over the base.
Base region with rather high E (~few kV/cm) extends near the surface pf the epi-layer.
As-irradiated detector – enhanced current and increase of electric field related to trapping at the n+ contact? – needs additional study.
New method of E(x) reconstruction in irradiated Si detectors is universal and is related to minimal number of parameters.
E. Verbitskaya et al., 11 RD50 Workshop, CERN, Geneva, Nov 12-14, 2007
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Acknowledgements
This work was supported in part by:
• Grant of the President of RF SSc-5920.2006.2• INTAS-CERN project # 03-52-5744
Thank you for your attention!
Acknowledgemets to SMART team - M. Boscardin, M. Bruzzi, D. Creanza, D. Menichelli, C. Piemonte.