beam loss monitoring – detectors photon detection and silicon photomultiplier technology in...
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Beam Loss Monitoring – Detectors
Photon Detection and Silicon Photomultiplier Technology in accelerator and particle physics
Sergey Vinogradov
QUASAR group
Department of Physics, University of Liverpool, UK
Cockcroft Institute of Accelerator Science and Technology, UK
P.N. Lebedev Physical Institute of the Russian Academy of Sciences, Russia
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Content
◙ 1. Introduction: the best photodetectors
◙ 2. Silicon Photomultipliers (SiPM) as new photon number resolving detectors
◙ 3. Benefits, drawbacks, and typical applications of SiPM
◙ 4. Evaluation studies of SiPMs for Beam Loss Monitoring
◙ 5. Modelling and analysis of comparative performance: SiPM vs PMT and APD
◙ 6. Trends and prospects of SiPM technology for BLM and accelerator applications
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 2
Introduction
◙ 1. Introduction: the best photodetectors your choice?
◙ 2. Silicon Photomultipliers (SiPM) as new photon number resolving detectors
◙ 3. Benefits, drawbacks, and typical applications of SiPM
◙ 4. Evaluation studies of SiPMs for Beam Loss Monitoring
◙ 5. Modelling and analysis of comparative performance: SiPM vs PMT and APD
◙ 6. Trends and prospects of SiPM technology for BLM and accelerator applications
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 3
Photodetector #1 *
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 4
Adaptive focusing & trichromatic / monochromatic vision High sensitivity due to 100 million rod cells (10-40 photons)High resolution & double dynamic range due to 5 million cone cellsHigh readout rate of 30 frame/sInternal signal processing (100M cells to 1M nerves @30fps)540 million years old design
(*) Yu. Musienko, NDIP 2011
CCD/CMOS approach – toward to #1
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 5
Trichromatic / monochromatic vision Number of pixels up to ~ 50 M Sensitivity from ~ 10 -100 photonsDynamic range up to ~ 50KReadout up to ~ 1000 frame/s40 years old design
SiPM approach – toward to ideal low photon detection
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 6
R 50
h
pixels
Ubias 50V
Al
DepletionRegion2 m
substrate
Resistor ~1 MOhm
20m
42m
R 50
h
pixels
Ubias 50V
Al
DepletionRegion2 m
substrate
Resistor ~1 MOhm
20m
42m
20th Anniversary ~ now!
Silicon Photomultipliers (SiPM) as new photon number resolving detectors
◙ 1. Introduction: the best photodetectors
◙ 2. Silicon Photomultipliers (SiPM) as new photon number resolving detectors
◙ 3. Benefits, drawbacks, and typical applications of SiPM
◙ 4. Evaluation studies of SiPMs for Beam Loss Monitoring
◙ 5. Modelling and analysis of comparative performance: SiPM vs PMT and APD
◙ 6. Trends and prospects of SiPM technology for BLM and accelerator applications
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 7
Concept of ideal detector:first step to SiPM
◙ Ideal detector: conversion of any input signal starting from single photon to recognizable output without noise and distortion in amplitude and timing of the signal
W. Farr, SPIE LEOS 2009
Ideal photon detector
Real photon detector
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Single photon detectionin 1 GHz BW with electronic noise 104 e
5 104 0 5 104 1 105
Single photon outputExternal noise
Photodiode
Output, electrons
Pro
babi
lity
dis
trib
utio
n
5 104 0 5 104 1 105
Single photon outputExternal noise
APD
Output, electrons
Pro
babi
lity
dis
trib
utio
n1 105 9.5 105 2 106
Single photon outputExternal noise
PMT
Output, electrons
Pro
babi
lity
dis
trib
utio
n
y 700000 1100000 2000000
1 105 9.5 105 2 106
Single photon outputExternal noise
SiPM
Output, electrons
Pro
babi
lity
dis
trib
utio
n
FactorNoiseExcessN
NENF
N
NResolution
out
out
out
noiseout
2
2
2
22
)(1
)(
σ(Nout)
σnoise
Gain =1ENF ~ 1
Gain ~ 100ENF ~ 3…10
Gain ~ 1 MENF ~ 1.2 Gain ~ 1 M
ENF ~ 1.01
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Avalanche with negative feedback: main step to SiPM
Strong negative feedback = fast quenching & small charge fluctuations
0 100 200 3000
1 104
2 104
3 104
0
2 105
4 105
6 105
Avalanch current (high)Avalanch current (low)Electric field (high)Electric field (low)
Avalanche breakdown with negative feedback
Time, ps
Ava
lanc
he c
urre
nt, e
/ps
Inte
rnal
ele
ctri
c fi
eld,
V/c
m
Higher Field
+Current filament
avalanche layer
Accumulatedminority carriers(inversion layer)
feedback layer (wide-bandsemiconductor)
depleted andquasineutral
layers
metallic electrode Initialphotoelectron
p-Si
V. Shubin, D. Shushakov, Avalanche Photodetectors, 2003
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Multi-pixel design & feedback resistor:final step to SiPM
Fig. 1-4: Sadygov, NDIP 2005 Fig. 5-7: B. Dolgoshein et al., 2001-2005
R 50
h
pixels
Ubias 50V
Al
DepletionRegion2 m
substrate
Resistor ~1 MOhm
20m
42m
R 50
h
pixels
Ubias 50V
Al
DepletionRegion2 m
substrate
Resistor ~1 MOhm
20m
42m
SiPM – 1996 / 2000sMRS APD – 1990s
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
SiPM: photon number resolution
B. Kardinal et al., Nat. Photonics, 2008
R. Mirzoyan et al., NDIP, 2008
A. Barlow and J. Schilz, SiPM matching event, CERN, 2011
APD (self-differencing mode) VLPC SiPM (MEPhI/Pulsar)
SiPM (Excelitas)PMT (Hamamatsu R5600)
I. Chirikov-Zorin et al, NIMA 2001
MPPC (Hamamatsu)
S. Vinogradov, SPIE 2011
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Sergey Vinogradov Seminars on SiPM at the Cockcroft Institute 2 December 2013 13G. Collazuol, PhotoDet, 2012
Benefits, drawbacks, and typical applications of SiPM
◙ 1. Introduction: the best photodetectors
◙ 2. Silicon Photomultipliers (SiPM) as new photon number resolving detectors
◙ 3. Benefits, drawbacks, and typical applications of SiPM
◙ 4. Evaluation studies of SiPMs for Beam Loss Monitoring
◙ 5. Modelling and analysis of comparative performance: SiPM vs PMT and APD
◙ 6. Trends and prospects of SiPM technology for BLM and accelerator applications
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 14
SiPM: photon number resolution
◙ SiPM looks like ~ ideal detectorNear-ideal amplification:
― Gain > 105, ENF < 1.01
Room temperature
Low bias (<100 V)
Large area (6x6 mm2)
Good timing (jitter < 200 ps)
Fast response (rise <1 ns, fall~20 ns)
◙ In fact, not a photon spectrumPhotoelectrons
Dark electrons
Crosstalk & Afterpulses
◙ In fact, non-Poissonian distributionWhy?
How much?
Distribution?
Resolution? P. Finocchiaro et al., IEEE TNS, 2009
A. Barlow and J. Schilz, SiPM matching event, CERN, 2011
SiPM (Excelitas)
2
][1][
X
XVarXENF
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
SiPM drawbacks: crosstalk
◙ Crosstalk: hot carrier photon emission + detection = false event
A. Lacaita et al., IEEE TED, 1993
R. Mirzoyan, NDIP, 2008
Yu. Musienko, NDIP, 2005
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
SiPM drawbacks: afterpulsing
◙ Afterpulsing: trapping + detrapping + detection = false event
primary avalanche
afterpulses
Δ time
Output
G. Collazuol, PhotoDet, 2012 C. Piemonte et al., Perugia, 2007
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
SiPM drawbacks: nonlinearity
◙ Limited number of pixels = losses of photons◙ Dead time of pixels during recovery = losses of photons
Plot details:
Npixel=100
PDE=100%
No Noise (DCR, CT, AP)
0
20
40
60
80
100
0 50 100 150 200 250 300
Number of photons, Nph
Nu
mb
er o
f fi
red
pix
els,
Ns
Ideal response<Ns>=<Nph>
Nonlinear response<Ns>=f(<Nph>)
Output SignalDistribution
Equivalent SignalDistribution
Incident PhotonDistribution
( )
1eq Nph Ns d Ns
d Nph
Ideal 100 pixel SSPM
Idea
l pho
ton
dete
ctor
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Application types
◙ Binary detection of light pulses – “events” (bit error rate) - NA
◙ Photon number resolution (noise-to-signal ratio, σn/μn) - Calorimetry
◙ Time-of-flight detection (transit time spread, σt) – TOF PET
◙ Detection of arbitrary signals starting from photon counting - Iph(t)
- Beam Loss Monitoring
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
SiPM application examples
◙ CalorimetrySiPM (MEPhI) small HCAL (MINICAL), DESY, 2003
MPPC (Hamamatsu), T2K, 2005-2009
MPPC at LHC CMS HCAL
RICH for ALICE (LHC)
FermiLab, Jefferson Lab calorimeter upgrade projects
◙ AstrophysicsSiPM cosmic ray detection in space (MEPhI, 2005)
Cherenkov light detection of air showers (CTA, 2013)
◙ Medical imaging Positron Emission Tomography:
―TOF-PET ― PET / MRI
◙ TelecommunicationQuantum cryptography
Deep space laser link (Mars exploring program)
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Evaluation studies of SiPMs for Beam Loss Monitoring
◙ 1. Introduction: the best photodetectors
◙ 2. Silicon Photomultipliers (SiPM) as new photon number resolving detectors
◙ 3. Benefits, drawbacks, and typical applications of SiPM
◙ 4. Evaluation studies of SiPMs for Beam Loss Monitoring
◙ 5. Modelling and analysis of comparative performance: SiPM vs PMT and APD
◙ 6. Trends and prospects of SiPM technology for BLM and accelerator applications
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 21
Beam Loss Monitoring (ref. E. Nebot talk 08-07-14)
Objectives:
ProtectMonitorAdjust
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
BLM: first evaluation of SiPM
D. Di Giovenale et al., NIMA, 2011SPARC accelerator, Frascati, INFN
FERMI@Elettra, Synchrotrone Trieste
MPPC, 1mm2, 400 pixels
Quartz fiber 300 μm, 100 m
Dark count noise: negligible
Electronic noise: negligible
Spectral dispersion in fiber: n( ) →∆t( ) 𝜆 𝜆 ~ 3 ns @100 m
τfall ~ 10 ns → deconvolution◙Compact low cost BLM
1m-scale resolution @100 m
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
SiPM performance metrics for BLM
◙ Loss scenarios reconstructionAmplitude → # photons → # particles per location (PNR)
Transit time to rising edge → single loss location (Time Res.)
Resolution of multiple loss locations & # particles ― Modulation transfer function (MTF) ?― Nonlinearity has to be accounted !
PNR
TTS
New metrics ?
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Challenges for SiPM in BLM:saturation, recovering, duplications
◙ Transient nonlinearity of SiPM responseLarge rectangular light pulse: Nph > Npix; Tpulse > Trec
Peak – initial avalanche events in ready-to-triggering pixels
Plateau – repetitive recovering and re-triggering of pixels
Fall – final recovering (without photons, but with afterpulses!)
4 us pulse 50 ns pulse
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
MPPC response on rectangular pulse
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Modelling and analysis of comparative performance: SiPM vs PMT and APD
◙ 1. Introduction: the best photodetectors
◙ 2. Silicon Photomultipliers (SiPM) as new photon number resolving detectors
◙ 3. Benefits, drawbacks, and typical applications of SiPM
◙ 4. Evaluation studies of SiPMs for Beam Loss Monitoring
◙ 5. Modelling and analysis of comparative performance: SiPM vs PMT and APD
◙ 6. Trends and prospects of SiPM technology for BLM and accelerator applications
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 27
Photon Number Resolution
◙ Photon Number Resolution & Excess Noise FactorBurgess variance theorem
0
20
40
60
80
100
0 50 100 150 200 250 300
Number of photons, Nph
Nu
mb
er o
f fi
red
pix
els,
Ns
Ideal response<Ns>=<Nph>
Nonlinear response<Ns>=f(<Nph>)
Output SignalDistribution
Equivalent SignalDistribution
Incident PhotonDistribution
Ideal 100 pixel SSPM
Idea
l pho
ton
dete
ctor
1
2
2
2
2
2
2
1
)()(
)(
)(
1)(
1
ENFENFPoissonianNif
ENFN
N
N
NPNR
randomNif
N
NN
N
ENF
NifN
NENF
Nin
Nin
in
out
outout
in
in
in
out
out
N
in
out
out
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Schematics of AP & CT stochastic processes
Branching Poisson
Crosstalk Process
Geometric Chain
Afterpulsing
Process
Poisson number of primaries <N>=μ
e.g. SSPM Photon Spectrum
Single primary event N≡1
e.g. SSPM Dark SpectrumDuplication
Models
Non-random (Dark) event
Primary
1st CT
2nd CT
No CT
Ran
dom
CT
eve
nts …
Random CT events
Random Photo eventsRandom primary (Photo) events
Ran
dom
CT
eve
nts
…
…
…
Non-random (Dark) event
Ran
dom
CT
eve
nts …
… …
…
…
…
Random primary (Photo) events
Ran
dom
CT
eve
nts
…
…
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Results Geometric chain process Branching Poisson process
Primary event distribution
Non-random single (N≡1)
Poisson (μ) Non-random single (N≡1)
Poisson (μ)
Total event distribution
Geometric (p) Compound
Poisson (μ, p) Borel (λ) Generalized Poisson (μ, λ)
P(X=k) pp k 11
Ref. [1]
!
exp1
k
kk k
!
exp1
k
kk k
E[X] p1
1
p1
1
1
1
Var[X] 2)1( p
p
2)1(
)1(
p
p
31
31
ENF p1 )...(2
31
1
1 32 ppp
Analytical results for CT & AP statisticsCT & AP model results
[1] S. Vinogradov et al., NSS/MIC 2009 λ is a mean number of successors in one branch generation
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
1.0E+01
1.0E+02
1.0E+03
1.0E+04
1.0E+05
1.0E+06
1.0E+07
0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18
Threshould [fired pixels]
Dar
k C
ou
nt
Rat
e [H
z]
Experiment
Borel
Geometric
A few photon detection spectrum of Hamamatsu MPPC
(S. Vinogradov, SPIE 2012)
Dark event complimentary cumulative distribution – DCR vs. threshold
(S. Vinogradov, NDIP 2011; experiment B. Dolgoshein et al., NDIP 2008)
Pct=40%
Pct=10%
P. Finocchiaro et al., IEEE TNS, 2009
0
0.005
0.01
0.015
0.02
0.025
0.03
0.035
-1 0 1 2 3 4 5 6 7 8 9 10 11 12 13
Number of fired pixels
Pro
bab
ility
de
nsity
fun
ctio
n
Experiment
Generalized Poisson
A.N. Otte, JINST 2007
Crosstalk models and experiments
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
<Ns>=f(<Nph>)
0 50 100
Number of photons, Nph
SSPM
sign
al, fi
red
pixe
ls Ns
0
50
Photon signaldistributionSSPM equivalentphoton distributionCalibration
SSPM signaldistribution
NphdNsdNsNph
1
cell
ph
N
PDEN
N
PDEN
N
PDEN
cellNN
PDEN
cellfired
N
PDENe
ENF
eeNeNN
cell
ph
cell
ph
cell
ph
fired
cell
ph
1
11 2
SiPM binomial nonlinearity
Intrinsic Resolution in σ units; Npix=506
Photons per pulse, Nph
B. Dolgoshein et al., 2002Ou
tpu
t si
gn
al, N
s
E.B. Johnson, NSS/MIC 2008
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
SiPM recovery nonlinearity
1 10 100 1 103 1 104 1 1050.01
0.1
1
Tpulse=20TresetTpulse=2TresetTpulse<<Treset
Dead-time non-linear Resolution
Number of photons per pulse
1
0.01
R Nph 5 10 9 R Nph 50 10 9 R Nph 500 10 9
1 1051 Nph
Plot details:
PDE=100%
Npixel=500
Tpulse=100 ns
32
)1(
1
dead
Ns
dead
Ns
t
t
Nonparalizible dead time modelProbability distribution (~ Gaussian)
W. Feller, An Introduction to Probability Theory and Its Applications, Vol. 2, Ch. XI, John Willey & Sons, Inc., 1968
( ) ( ) 1eq Nph deadENF
Recovery non-linearity → ENFS. Vinogradov et al., IEEE NSS/MIC 2009
pulse recT T
2) Exponential recovery of Gain m(t) accounting for Pdet(m)S. Vinogradov, SPIE DSS, 2012
3
( ) det
1( ) ( )
12
receq Nph
rec
ENF if P m const
M.Grodzicka, NSS 2011
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Performance metrics: ENF and DQE
Noise source Key parameter Typical values for
SiPM ENF expression
SiPM ENF
PMT ENF
Fluctuation of multiplication
Mean gain and standard deviation of gain
μ(gain) ~ 106
σ(gain) ~ 105 )(
)(1
2
2
gain
gainFm
1.01 1.2
Crosstalk Probability of crosstalk
event Pct 5% – 40%
1
1 ln(1 )Fct
Pct
1.05 – 2 1
Afterpulsing Probability of afterpulse
Pap 5% – 20% 1Fap Pap 1.05 – 1.2 1.01
Shot noise of dark counts
Dark count rate DCR Signal events in Tpulse
105 – 107 cps 1DCR Tpulse
FdcrNph PDE
1.01 1
Noise / losses of photon detections
Photon detection efficiency PDE
15% – 40% 1
FpdePDE
2.5 – 6.6 5
Total noise in linear dynamic range
Total ENF_linear _ENF linear Fm Fct Fap Fdcr Fpde 2.8 – 16 6
Pixel number nonlinearity
Mean number of possible single pixel firings n
exp( ) 1; ; binomial distribution
Nph PDE nn ENFpix
Npix n
Recovery time nonlinearity
Mean rate of possible single pixel firings λ
; 1 ; nonparalizible modeln
ENFrec TrecTpulse
totalnlapctdcrpdemtotaltotalin
out
outout ENF
DQEFFFFFFENFNphENFNphPNRN
NPNR
1)()(
)(
)(
*
*
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Performance in DQE – various detectors
SNR performance (relative to ideal) in nanosecond light pulse detection by 1mm2 PDs
0.00%
10.00%
20.00%
30.00%
40.00%
50.00%
60.00%
70.00%
80.00%
90.00%
100.00%
1.E+0 1.E+1 1.E+2 1.E+3 1.E+4 1.E+5 1.E+6 1.E+7 1.E+8 1.E+9
Number of photons per pulse
Det
ecti
ve Q
uan
tum
Eff
icie
ncy
SSPM potential
DAPD Amplification Tech.
MPPC-50 Hamamatsu
APD
PIN - photodiode
PMT
Fm
PDE
Gain
Gain
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Time resolution
◙ Time resolution is combined as a sum of contributionsTransit time spread of photon arrival, avalanche triggering, avalanche development, and single electron response times
Jitter of signal amplitude fluctuations in a time scale
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Filtered point process approach to amplitude fluctuations & time resolution
Point Process
Marked Point Process
Filtered Output
Clastered Point Process
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Clastered filtered point process model
◙ Time resolution includes all essential factors and combines performance in time response and PNR (ENF)
2
2
sec
2
22
2
sec
2sec
secsec
sec
sec
2sec
2
22
sec222
secsec
1
)()(:
)()(
)(1)(
)(
)(
)()(
Thresh
noisetotal
phriset
sersersptrph
out
noisesci
sersptrph
sersptrphgain
pesersptrph
sersptrph
sersptrphpe
ser
noisesersptrphpescisersptrphgainpe
t
V
VENF
N
ththslowisSERandfastispulselightIf
tV
V
th
thENFENF
N
dt
thd
th
dt
thdN
KVV
thNthENFENFN
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Time resolution:scintillation model & experiment
asdasd
0 5 10 15
0.14
0.16
0.18
0.2Poisson with SER filtering (no noise)+ Gain and electronic noise+ Scintillator resolution 9%+ Crosstalk 15%+ Crosstalk 30%
Trigger threshold (SER amplitudes)
CR
T, n
s
Most popular & demanded case study: LYSO+MPPCLYSO: 0.09 ns rise, 44 ns decay; 9% resolution
MPPC: Npe=3900, ENFgain=1.015, Pct=0.14; SPTR=0.124 ns, Vnoise=0.32 mV S. Seifert et al, “A Comprehensive Mode to Predict the Timing Resolution ”, TNS, 2012.
MPPC SER pulse shape – analytical expression (~ 1 ns rise, ~ 25 ns decay) D. Marano et al, “Silicon Photomultipliers Electrical Model: Extensive Analytical Analysis” TNS 2014
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Arbitrary signal detection:rectangular pulse response model
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 40
Trends and prospects of SiPMs for BLM and accelerator applications
◙ 1. Introduction: the best photodetectors
◙ 2. Silicon Photomultipliers (SiPM) as new photon number resolving detectors
◙ 3. Benefits, drawbacks, and typical applications of SiPM
◙ 4. Evaluation studies of SiPMs for Beam Loss Monitoring
◙ 5. Modelling and analysis of comparative performance: SiPM vs PMT and APD
◙ 6. Trends and prospects of SiPM technology for BLM and accelerator applications
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 41
SiPM trends and advances
◙ Market leadersHamamatsuKETEKSensLFBK / AdvanSiDExcelitas / Perkin ElmerPhilips (digital SiPM)
◙ Design improvements (~ in a few year time scale)Higher Photon Detection Efficiency (30% → 70%)Lower crosstalk, lower afterpulsing (30% → 3%)Lower dark count rate (1000 → 40 Kcps/mm2)Faster SER, smaller pixel size (25 → 10 um)Larger area, larger arrays (3x3→10x10mm2, 4x4 → 16x16 channels)
Latest news from 2nd SiPM Advanced Workshop and Conf . on New Development s in Photodetection, 2014
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Hamamatsu: Through Silicon Vias
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Hamamatsu: Low Crosstalk & Afterpulsing
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Performance in DQE - MPPC series
Pulse duration & detection time = 10 ns
1 103 0.01 0.1 1 10 100 1 10
3 1 104 1 10
5 1 106 1 10
70
0.1
0.2
0.3
0.4
MPPC 100 umMPPC 50 umMPPC 25 umMPPC 15 umMPPC 10 um
DQE of market MPPCs (3x3mm 100, 50, 25, 15, 10 um pixels)
Photons / pulse
DQ
E
1 103 0.01 0.1 1 10 100 1 10
3 1 104 1 10
5 1 106 1 10
70
0.1
0.2
0.3
0.4
0.5
MPPC 100 um trenchMPPC 75 um trenchMPPC 50 um trench
DQE of newest MPPCs (3x3 mm 100, 75, 50, um pixels)
Photons / pulseD
QE
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
KETEK
◙ Highest PDE @50 um pixels◙ Various geometries◙ 15 … 100 um pixels
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
SensL
◙ Fast capacitive outputFWHM < 3.2 ns @ 6x6 mm2
◙ Large arrays / modules◙ Low cost
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Philips: Digital SiPM (Modern active quenching SPAD array)
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
Summary on BLM with SiPM
◙ BLM is one of the most challenging application for SiPMBenefits
―Practical & efficient (cost, compactness, Si reliability…)―Perfect Transit Time Resolution (as is for now)―Acceptable DQE within dynamic range (may be better)
Drawbacks―Upper margin of dynamic range is low (design improvement)
– Number / density of pixels (↑ 10 times)– Pixel recovery time (↓ 10 times)
―Time response (bandwidth) (external measures)– Analog / digital SiPM output signal processing
◙ BLM with SiPM: big problem with a chance to winAnd with a lot of space for new ideas, designs, and fun
Sergey Vinogradov Seminars on SiPM at the Cockcroft Institute 3 February 2014 49
SNR performance (relative to ideal) in nanosecond light pulse detection by 1mm2 PDs
0.00%
10.00%
20.00%
30.00%
40.00%
50.00%
60.00%
70.00%
80.00%
90.00%
100.00%
1.E+0 1.E+1 1.E+2 1.E+3 1.E+4 1.E+5 1.E+6 1.E+7 1.E+8 1.E+9
Number of photons per pulse
Det
ecti
ve Q
uan
tum
Eff
icie
ncy
SSPM potential
DAPD Amplification Tech.
MPPC-50 Hamamatsu
APD
PIN - photodiode
PMT
Summary on SiPM
◙ SiPM technology: breakthrough in photon detectionPhoton number resolution at room temperature
Silicon technology / mass production / reliability / price
Highly competitive in short (< μs) pulse detection
Fast progress in improvements: DQE, Dynamic range, Timing
◙ Welcome to
SiPM applicationsScintillation
Cherenkov
Laser pulse
And much more…
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014
The end
◙ Thank you for your attention
◙ Questions?
Sergey Vinogradov oPAC Advanced School on Accelerator Optimization Royal Holloway University, London, UK, July 9th, 2014 51