fabio sauli photon detection and imaging with gaseous...
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
PHOTON ABSORPTION 1
I = I0 e-
x
l = I0 e-mc
I0 I
x
l =1
Ns
N = N0
r
A
I0 : incoming flux
I : outgoing flux
E E - EK
E
EC
Ee
C
e
E e+
e-
PHOTOELECTRIC:
COMPTON SCATTER:
PAIR PRODUCTION
l: absorption length (cm)
m: mass absorption coefficient (cm2g-1)
r: density (g cm-3)
N: atoms (molecules) cm-3
s: absorption cross section (cm2)
A: Avogadro number
EK-EL
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
PHOTON ABSORPTION CROSS SECTION 2
Photoionization Threshold
Xe: 12.1 eV
1 Mbarn=10-18 cm2
http://xdb.lbl.gov/
http://henke.lbl.gov/optical_constants/
http://www.nist.gov/pml/data/xraycoef/
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
UV PHOTONS ABSORPTION 3
NOBLE GASES: PHOTOIONIZATION THRESHOLD
MOLECULAR GASES:
TOTAL AND IONIZATION CROSS SECTIONS
H. S. W. Massey, Electronic and Ionic impact Phenomena
(Oxford Press 1969)
G. Marr, Photoionization Processes in Gases
(Academic Press NY 1967)
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
A CURIOUS OBSERVATION: INFRARED SENSITIVITY? 4
STUDY OF GLOW DISCHARGES IN MWPCs
Rutherford Lab (1979)
J.B. Marsh, K.H. Souten and B. O’Hagan
RL-79-038 (1979)
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
LOW THRESHOLD PHOTOIONIZING VAPORS 5
TOT
QE
Triethylamine (TEA) (C2H5)3N
Ei = 7.5 eV Tetrakis-dimethilamino-ethylene (TMAE)
C[(CH3)2N]4
Ei = 5.3 eV
R. Holroyd et al, Nucl. Instr. and Meth.A261(1987)440
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
VISIBLE PHOTOCATHODES WITH GASEOUS COUNTERS 6
D. Mörmann et al, Nucl. Instr. and Meth. A504(2003)93
GAS ELECTRON MULTIPLIER (GEM)
WITH SEMI-TRANSPARENT
PHOTOCATHODE
PROBLEMS OF ION BACKFLOW:
- GAIN DIVERGENCY DUE TO PHOTON FEEDBACK
- PHOTOCATHODE DAMAGE DUE TO ION
BOMBARDMENT
NEW STRUCTURES:
COBRA, MICRO-HOLES AND STRIPS, PACEM….
R. Chechik, A. Breskin, Nucl. Instr. and Meth. A595(2008)116
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
CAESIUM IODIDE PHOTOCATHODES 7
A. Breskin et al, Nucl. Instrum. and Meth. A483(2001)670
CsI QUANTUM EFFICIENCY FIELD DEPENDENCE OF THE
PHOTOELECTRON EXTRACTION EFFICIENCY
J. Seguinot et al, Nucl. Instr. and Meth. 297(1990)133
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
UV WINDOWS TRANSPARENCY 8
UV GLASS AND FLUORIDE CRYSTALS:
THIN POLYMER FOILS:
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
PHOTOELECTRIC CROSS SECTION: SOFT X-RAYS 9
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SOFT X-RAYS: ABSORPTION LENGTH AND DETECTION EFFICIENCY 10
GASES AT STANDARD TEMPERATURE AND PRESSURE (STP: 00C, 1 atm):
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SOFT X-RAYS WINDOWS TRANSPARENCY 11
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SOFT X-RAYS: PHOTOELECTRIC 12
K SHELL FLUORESCENCE:
L-SHELL:
E
E-EL
EL-EM
E E-EK
EK-EL EL-EM
E E-EK
ESCAPE
NON-RADIATIVE (AUGER)
E
~ E
E
LINEAR ATTENUATION COEFFICIENT (STP):
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SOFT X-RAYS: FLUORESCENCE YIELD AND ESCAPE PEAKS 13
5.9 keV
~ 3 keV
5.9 keV 55Fe SOURCE IN ARGON:
22-25 keV 109Cd SOURCE IN XENON:
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
FLUORESCENCE YIELD 14
FY=FLUORESCENCE/TOTAL
Ar
FY~10%
Xe
FY~90%
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
ANGULAR DISTRIBUTION AND RANGE OF PHOTOELECTRONS 15
q
e
E 5.9 keV
RANGE:
ANGLE:
200 µm
Ee=E-EK= 2.7 keV in Ar
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
POSITION RESOLUTION LIMITS 16
42 keV PHOTONS ON XENON
600 µm
2 mm
POSITION RESOLUTION FOR A
POINT-LIKE COLLIMATED BEAM:
J.E. Bateman et al, RL-75-140
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
X-RAYS DETECTION EFFICIENCY 17
1 cm, STP
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
HARD X AND GAMMA RAYS: CONVERTERS 18
DETECTION EFFICIENCY:
e =1- e-
s
l
s: converter thickness
l: absorption length
e
e
CONVERTER
GAS DETECTOR
s
USEFUL CONVERTER THICKNESS ~ ELECTRON RANGE
100 µm converter --> e ~ 1%
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
HARD X AND GAMMA RAYS: INTERNAL CONVERTERS 19
HEAVY DRIFT CHAMBER
A. Jeavons et al, IEEE Trans. Nucl. Sci. NS-23 (1978)41
MWPC
HV
e
EFFICIENCY VS CONVERTER ATOMIC NUMBER:
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
HARD X AND GAMMA RAYS: INTERNAL CONVERTERS 20
GAS ELECTRON MULTIPLIER (GEM) Au-COATED
DETECTION EFFICIENCY
T. Koike et al,
Nucl. Instr. and Meth. A648(2011)180
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
HARD X AND GAMMA RAYS: INTERNAL CONVERTERS 21
D. Watts et al, J.Rad.Res. 54 (2013)i136
DETECTION OF 511 keV FOR PET
MULTI-GAP RESISTIVE PLATE CHAMBER
+HV
- HV
400 µm HIGH RESISTIVITY GLASS PLATES
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
ELECTRONS DRIFT IN UNIFORM FIELD 22
DRIFT VELOCITY DIFFUSION
http://rjd.web.cern.ch/rjd/cgi-bin/cross
COMPUTED WITH MAGBOLTZ:
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
AVALANCHE CHARGE MULTIPLICATION 23
CHARGE MULTIPLICATION IN UNIFORM FIELD
l E
x Ions
Electrons
Multiplication factor or Gain:
dn= na dx
Incremental increase of the number of electrons in
the avalanche:
M(x) =n
n0
= ea x
Maximum avalanche size before discharge
(Raether limit): QMAX ≈ 107 e
H. Raether, Electron Avalanches and
Breakdown in Gases (Butterworth 1964)
a
P= f
E
P
æ
è ç
ö
ø ÷
Mean free path for ionization:
l =1
NsN: molecules/cm3
Townsend coefficient:
Ionizing collisions/cm
a =1
l
S.C. Brown, Basic Data of Plasma Physics (MIT Press, 1959)
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
ELECTRON AVALANCHE: FURRY STATISTICS 24
SINGLE ELECTRON
AVALANCHE SIZE DISTRIBUTION N ELECTRONS:
P(n, N) =1
n
n
n
æ
èç
ö
ø÷
N-1e
-n
n
(N -1)!
P(n) =e-n n
nn = eax s n = n
n _
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
25
P(N ) =N (1 + q)
N
é
ë ê
ù
û ú
q
e-
N (1 +q )
N
sA
A
æ
è ç
ö
ø ÷
2
=1
A +
1
1-q@
1
1-q
H. Sclumbohm, Zeit. Physik 151(1958)563
SINGLE ELECTRON AVALANCHE: POLYA STATISTICS
H. Schindler, S.F. Biagi, R. Veenhof,
Calculation of gas gain fluctuations in uniform fields
Nucl. Instr. and Meth. A624(2010)78
AVALANCHE DISTRIBUTION AT INCREASING GAINS (FIELDS)
POLYA DISTRIBUTION EXPERIMENTAL:
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SINGLE ELECTRON AVALANCHE IN MPGDs 26
GAS ELECTRON MULTIPLIER (GEM)
F. Sauli, Nucl. Instr. and Meth. A553(2005)18
TRIPLE-GEM
CsI Photocathode
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SINGLE ELECTRON AVALANCHE IN MPGD 27
MICROMEGAS
Ne-iC4H10 95-5
M=6.104
Polya: q=2.3
T. Zerguerras et al, Nucl. Instr. and Meth. A608(2009)397
MICROMEGAS
WINDOW
PHOTOCATHODE
e-
UV PHOTON
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SINGLE ELECTRON AVALANCHE 28
J. Melai et al, Nucl. Instr. and Meth, A628(2011)133
CsI-COATED MICROMEGAS WITH TIMEPIX READOUT
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SOFT X-RAYS: ENERGY RESOLUTION 29
sE
E
æ
è ç
ö
ø ÷
2
=sN
N
æ
è ç
ö
ø ÷
2
+s M
M
æ
è ç
ö
ø ÷
2
M =1
NAi = A
i=1
N
å Ai : single electron avalanche size Average gain:
sM
2 =1
N
æ
è ç
ö
ø ÷
2
sA
2
i=1
N
åGain variance:
sM
M
æ
è ç
ö
ø ÷
2
=1
N
sA
A
æ
è ç
ö
ø ÷
2
Furry statistics:
sA = A
sA
A
æ
è ç
ö
ø ÷
2
=1
sA
A
æ
è ç
ö
ø ÷
2
=1
A + b b =
1
1+ qPolya statistics:
sN
2 = F N
sE
E
æ
è ç
ö
ø ÷
2
=1
N(F + b)
b= 1 (1- q)Furry: b=1 Polya:
Ar 0.19
Xe <0.17
Ne+0.5%Ar 0.05
Ar-CH4 0.19
GAS F
Energy resolution:
Ionization Avalanche statistics
Ionization variance: F: Fano factor
FANO FACTORS
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SOFT X-RAYS ENERGY RESOLUTION 30
GAIN
RE
SO
LU
TIO
N %
NOISE IONIZATION
AVALANCHE
TOTAL
H. Sipilä and E. Kiuru, Adv. X-Ray Analysis 21(1978)
fwhm 1.3 keV
5.9 keV
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
MICROMEGAS ENERGY RESOLUTION 31
INGRID: MICROMEGAS WITH TIMEPIX READOUT
M. Chefdeville et al,
Nucl. Instr. and Meth. A591(2008)147
5.9 keV 55Fe in Ar-CH4 90-10
14% fwhm GAP INDEPENDENCE OF GAIN
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
ELECTRON COUNTING 32
A. Pansky et al, Nucl. Instr. and Meth. A330(1993)150
LOW PRESSURE (10 Torr) PROPORTIONAL
COUNTER 676 eV 110 eV
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SCINTILLATION PROPORTIONAL COUNTERS 33
PHOTON EMISSION BEFORE CHARGE MULTIPLICATION:
NO AVALANCHE DISPERSIONS
NOBLE GASES SCINTILLATION SPECTRA ~1bar
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SCINTILLATION PROPORTIONAL COUNTERS 34
SCINTILLATION COUNTERS
A. Policarpo et al, Nucl. Instr. and Meth. 102(1972)337
ENERGY RESOLUTION:
CLOSE TO STATISTICAL LIMIT
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
WIRE COUNTERS 35
SINGLE WIRE COUNTER
MULTI-WIRE PROPORTIONAL CHAMBER
E. Rutherford and H. Geiger, Proc. Royal Soc. A81 (1908)141
G. Charpak et al, Nucl. Instr. and Meth. 62(1968)262
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
COUNTER GAIN: PROPORTIONAL TO STREAMER 36
STREAMER TRANSITION
N. Koori et al, Jap. J. Appl. Phys. 25(1986)986
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
RAETHER LIMIT 37
MINIMUM IONIZING
PARTICLES
Q= 100 x104=106
n ~ MeV p
Q ~ 104 x 104 = 108
p
Field emission
~ 104 x 104 = 108
TOTAL CHARGE Q > 107----> DISCHARGE
N. Koori et al, Jap. J. Appl. Phys. 25(1986)986
103
104
DISCHARGES IN MICROSTRIP CHAMBERS
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
SPARK DAMAGES IN THE MICROSTRIP COUNTER 38
EFFECTS OF DISCHARGES IN MSGCs
Fabio’s Museum of Horrors
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
MICRO-PATTERN GAS DETECTORS (MPGD) 39
R. Bellazzini et al,
Nucl. Instr. Meth. A424(1998)444
A. Ochi et al,
Nucl. Instr. and Meth. A478(2002)196
P. Rehak et al
IEEE TNS-47(2000)1426
MICRO-PIN ARRAY
F. Bartol et al
J. Phys.III France 6(1996)337
COMPTEUR A
TROUS
MICRO-PIXEL CHAMBER
MICRO-GROOVE CHAMBER
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
MICRO-MESH GASEOUS STRUCTURE (MICROMEGAS)
40
Y. Giomataris et al, Nucl. Instr. and Meth. A 376(1996)29
HIGH/LOW FIELD REGIONS
SEPARATED BY A MESH
~ 200 V cm-1
~ 40 kV cm-1
GAP UNIFORMITY:
SPACERS OR PILLARS
Ioannis Giomataris (1996)
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
MICROMEGAS FOR THE COMPASS EXPERIMENT AT CERN 41
C. Bernet et al, Nucl. Instr. and Meth. A536(2005)61
9 ns rms
SPACE RESOLUTION:
TIME RESOLUTION:
12 planes in 3 stations X,Y, U, V
40x40 cm2 active
350 µm strips with digital readout 70 µm rms
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
LARGE SIZE MICROMEGAS 42
ATLAS FORWARD MUON UPGRADE:
1024 mm
J. Wotschack, RD51 Meeting (CERN 2013)
J. Wotschack, JINST 7, C02021 (2012)
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
GAS ELECTRON MULTIPLIER (GEM) 43
F. Sauli, Nucl. Instr. and Meth. A386(1997)531
THIN (50 µm) METAL-COATED POLYMER
FOIL WITH HIGH DENSITY OF HOLES:
STANDARD GEM:70 µm Ø at 140 µm PITCH Fabio Sauli (1997)
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
TRIPLE GEM DETECTOR FOR COMPASS 44
31x31 cm2 active Total thickness in active area ~ 0.7% X0
2-D readout board: 400 µm pitch strips
Honeycomb
plates
GEM foils
Readout
board
80 µm
350 µm
C. Altumbas et al,
Nucl. Instr. and Meth. A490(2002)177
22 DETECTORS, OPERATIONAL 2002-2012
B. Ketzer et al, Nucl. Instr. and Meth. A535(2004)314
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
LARGE SIZE GEM DETECTORS 45
99 cm
D. Abbaneo et al, JINST 9(2014)C01053
M. Tytgat, MPGD 2013
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
MICROMEGAS DISCHARGES 46
SPARK PROBABILITY IN HADRON BEAM
FOR A GAIN OF 5.103 , 106 PARTICLES s-1:
~ ONE DISCHARGE PER SECOND
A. Delbart et al,
Nucl. Instr. and Meth. A478(2002)205
10-6
5 103
RESISTIVE MICROMEGAS
J. Galán et al, Nucl. Instr. and Meth. A732(2013)229
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
GEM DISCHARGES 47
C. Büttner et al,
Nucl. Instr. and Meth. A409(1998)79
HIGHER GAIN, LOWER VOLTAGE ON EACH GEM TRIPLE-GEM:
CASCADED ELECTRODES DISCHARGE RATE ON ~ 5 MeV a (105 e)
Q~107
Q~108
Q~109
WHAT ABOUT THE RAETHER LIMIT?
IN MULTI-GEMS, THE CHARGE
SPREADS OVER MANY
INDEPENDENT HOLES!
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
UV PHOTONS DETECTION: MWPC 48
CsI-coated cathode pads
MWPC
Window
E. Albrecht et al, Nucl. Instr. and Meth. A502(2003)112
COMPASS RING IMAGING CHERENKOV COUNTER (RICH)
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
UV PHOTON DETECTION: MICRO-PATTERN CHAMBERS 49
EDRIFT ~ 0
e
CsI LAYER
D. Mormann et al,
Nucl. Instr. and Meth. A478(2002)230
GEM WITH REFLECTIVE CsI PHOTOCATHODE COATING
FURTHER AMPLIFICATION
T. Meinshad. L. Ropelewski, F. Sauli
Nucl. Instr. and Meth. A535(2004)324
POSITION ACCURACY:
TWO COLLIMATED PHOTON BEAMS AT 200 µm
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
UV PHOTON DETECTION AND LOCALIZATION 50
F. Sauli et al, IEEE NSSS 2004 Conf. Rec.Vol. 1, 12
TRIPLE GEM WITH HEXABOARD READOUT
MATRIX OF HEXAGONAL PADS
INTERCONNECTED ALONG THREE DIRECTIONS
TWO-PHOTONS EVENT:
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
GEM WITH SILICON PIXEL READOUT 51
X-RAY POLARIMETER
R. Bellazzini et al, Nucl. Instr. and Meth. A623(2010)766
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
GEM WITH SILICON PIXEL READOUT 52
R. Bellazzini et al, Nucl. Instr. and Meth. A581(2007)246
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
GEM WITH SILICON PIXEL READOUT 53
~ 4 µm
R. Bellazzini et al, Nucl. Instr. and Meth. A581(2007)246
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
THICK GEM 54
MECHANICAL DRILLING OF METAL-CLAD PC BOARD:
• SELF-SUPPORTING
• HIGH GAIN
P. Janneret, Thesis at Neuchatel University (2001)
ALSO NAMED LARGE ELECTRON MULTIPLIER (LEM)
R.Chechik et al,
Nucl. Instr. and Meth. A535(2004)303
A. Breskin et al,
Nucl. Instr. And Meth. A623(2010)132
A. Badertscher et al, Nucl. Instr. And Meth. A617(2010)188
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
UV PHOTONS DETECTION: THICK GEM 55
DEVELOPMENT FOR THE COMPASS RICH UPGRADE
LARGE RIM:
• HIGH GAIN
• CHARGING UP
GAIN
V (kV)
0
10 µm
100 µm
0.1 mm rim
No rim
RIMLESS:
• LOW GAIN
• STABLE
M. Alexeev et al, Nucl. Instr. and Meth. A695(2012)159
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
COMPASS RICH UPGRADE 56
M. Alexeev et al, Nucl. Instr. and Meth. A732(2013)264
COMPASS RICH UPGRADE PROTOTYPE
TRIPLE-THICK GEM CsI-COATED 30x30 cm2
9-PHOTONS RING
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THE END 57
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Fabio Sauli – Photon Detection and Imaging with Gaseous Detectors – NDIP14
BUY ME ACHETE-MOI COMPRAMI KAUFEN SIE MICH КУПИТЬ МНЕ 58
www.cambridge.org/9781107043015
F4GASEOUS