recent progress with the rpwell detector · s. bressler et al. 2013 jinst 8 p07017 • and more......
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![Page 1: Recent progress with the RPWELL detector · S. Bressler et al. 2013 JINST 8 P07017 • And more... S. Bressler. Random order • Simple • Robust • Cost-effective • Production](https://reader034.vdocument.in/reader034/viewer/2022051604/5ffbf60eb7f87804a443b36f/html5/thumbnails/1.jpg)
Recent progress with the RPWELL detector
S. Bressler on behalf of the WIS/Coimbra/Aveiro groups
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Random order• Simple• Robust • Cost-effective
• Production• Operation (etc. gas mixtures)
• Large-area • Efficient • Resolution: spatial, time, energy• Broad dynamic range• Rate capabilities• Discharge free• Industrially produced
2
THGEM-based detectorsWish list Applications
Random order• RICH devices
M. Alexeev et al. 2012 JINST 7 C02014
• Cryogenic detectors for TPC in neutrino physics and rare-event searchesM. Resnati et al. 2011 J. Phys.: Conf. Ser. 308 012016A. Bondar et al. 2011 JINST 6 P07008
• GPM for dark matter searchesL. Arazi et al. Expected online publication in JINST: November 2015
• Medical imagingS. Duval et al. 2011 JINST 6 P04007
• Neutron/Gamma imaging in cargo inspection systemsA. Breskin et al. 2012 JINST 7 C06008I. Israelashvili et al. 2015 JINST 10 P03030
• Thin sampling elements for DHCALS. Bressler et al. 2013 JINST 8 P07017
• And more...
S. Bressler
![Page 3: Recent progress with the RPWELL detector · S. Bressler et al. 2013 JINST 8 P07017 • And more... S. Bressler. Random order • Simple • Robust • Cost-effective • Production](https://reader034.vdocument.in/reader034/viewer/2022051604/5ffbf60eb7f87804a443b36f/html5/thumbnails/3.jpg)
Random order• Simple• Robust • Cost-effective
• Production• Operation (etc. gas mixtures)
• Large-area • Efficient • Resolution: spatial, time, energy• Broad dynamic range• Rate capabilities• Discharge free• Industrially produced
3
THGEM-based detectorsWish list Applications
Random order• RICH devices
M. Alexeev et al. 2012 JINST 7 C02014
• Cryogenic detectors for TPC in neutrino physics and rare-event searchesM. Resnati et al. 2011 J. Phys.: Conf. Ser. 308 012016A. Bondar et al. 2011 JINST 6 P07008
• GPM for dark matter searchesL. Arazi et al. Expected online publication in JINST: November 2015
• Medical imagingS. Duval et al. 2011 JINST 6 P04007
• Neutron/Gamma imaging in cargo inspection systemsA. Breskin et al. 2012 JINST 7 C06008I. Israelashvili et al. 2015 JINST 10 P03030
• Thin sampling elements for DHCALS. Bressler et al. 2013 JINST 8 P07017
• And more...
The RPWELL - boosts the items on the wish list
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Resistive Plate WELL:• WELL coupled to materials with large
bulk resistivity • The charge is induced on the readout pads• The avalanche charge flows through the
plate to the anode
4
Material Dimensions[mm]
Bulk resistivity[Ωcm]
VERTEC 400 glass 36×31×0.4 8×1012
HPL Bakelite 29×29×2 2×1010
Semitron ESD 225 30×30×2 2×109
Tested materials
The RPWELL detector
A. Rubin et. al, JINST 8 P11004 2013
S. Bressler
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5
Lab. studies
0
50
100
150
200
250
300
0 200 400 600 800
Coun
ts [A
U]
Charge [fC]
Semitron 2mm~109 Ohm cmRate: 3x102Hz/mm2
W E L L$
gain$
T o t a l$
gain$
RPWELL 109 Ωcm - 2 mm layer
• Same pulse shape as standard well
• ~20% Energy resolution• Gain saturation at high
irradiation rate• < 50% gain drop over 4
orders of rate magnitudes• No discharges at high
rate of HIPs
Arb
itrar
y U
nits
Cou
nts
Gai
n
Gai
n
Rel
ativ
e G
ain
micro-sec
Rate [Hz/mm2] Injector gain
A. Rubin et. al, JINST 8 P11004 2013
Characterization in Ne\(5%)CH4
Focus on thin Semitron ESD 225 layers
A. Rubin et. al, JINST 8 P11004 2013
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Improved performance with thinner (0.4 & 0.6 mm) layers
Higher gain for the same voltage• Smaller anode-cathode gap
Gain drops slower with rate• Lower resistivity
Stable with HIPs• Observe gain saturation
3 x 3 cm2 3 x 3 cm2 3 x 3 cm2
Focus on thin Semitron ESD 225 layers
Lab. studies Characterization in Ne\(5%)CH4
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7
Lab. studies Operation in different gas mixtures
1000#
10000#
100000#
1000000#
10000000#
800# 1000# 1200# 1400# 1600# 1800# 2000# 2200# 2400# 2600# 2800#
Gain%[Log]%
V[V]%
Ne/CH4%mixtures%
3 x 3 cm2
95/5 90/10
80/20
50/50UV UV
UV
X-ray
UV
X-rayX-ray
X-ray
• Very high gains > 106 • Also with X-ray
• High gain with high CH4 concentration• Potential advantage in photo-
electron extraction efficiency ΔVRPWELL
Gain
Ne/CH4
UV & X-ray
S. Bressler
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Beam studies 10×10 cm2 detector - Ne/(5%CH4)150 GeV µ & π beams
Discharge-free operation also at high rate π-beam
µ-beam• Efficiency ≥ 99%• Pad multiplicity ≤ 1.2
π-beam• Efficiency ≥ 98%• Pad multiplicity ≤ 1.25
• Small difference attributed to secondary particles emitted in π interactions
Global detector response
S. Bressler et. al, arxiv:1510.03116
Gas gain ~104; effective gain ~103
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9
Beam studies
Discharge-free operation also at high rate π-beam
Local performance• Uniform efficiency• Larger multiplicity close to
pad boundaries
Stability in time• µ-beam: RMS 0.2 fC (5%)• π-beam: RMS 0.1 fC (2%)
10×10 cm2 detector - Ne/(5%CH4)150 GeV µ & π beams Local detector response
S. Bressler et. al, arxiv:1510.03116Gas gain ~104; effective gain ~103
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10
Beam studies
Discharge-free operation also at high rate π-beam
• ~20% gain drop over 2 orders of rate magnitudes
⇒
• ~5% efficiency loss• Can be avoided with
slightly higher nominal operation voltage (still in discharge-free) mode
10×10 cm2 detector - Ne/(5%CH4)150 GeV µ & π beams Rate capabilities
S. Bressler et. al, arxiv:1510.03116
S. Bressler et. al, arxiv:1510.03116
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11
Beam studies
Present detector• Discharges from the holes in
the resistive sheet ⇒ direct link between the RPWELL electrode and the cathode
30×30 cm2 detector 150 GeV µ & π beams
S. Bressler
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12
Beam studies
Present detector• Discharges from the holes in
the resistive sheet ⇒ direct link between the RPWELL electrode and the cathode
• Improves with additional isolation around the holes
30×30 cm2 detector 150 GeV µ & π beams
S. Bressler
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13
Beam studies
Present detector• Discharges from the holes in
the resistive sheet ⇒ direct link between the RPWELL electrode and the cathode
• Improves with additional isolation around the holes
Future detector (design is in progress)
• Large area built from smaller tiles
• Single uniform resistive sheet• No holes• Snake-shaped support also
force uniform gas flow across the detector (a la ATLAS TGC)
30×30 cm2 detector 150 GeV µ & π beams
Top cover + Cathode
Gas inlet
Gas outlet
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2 detectors setup + telescope installed in SPS/H4 beam area: 30 x 30 cm2 configuration with induction gap 10 x 10 cm2 RPWELL 0.4 mm Semitron layer
Beam studies Ne/(5%CH4) - Ar/(5%CH4) - Ar/(20%CO2)
150 GeV µ & π beams 10×10 cm2 & 30×30 cm2
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15
Beam studies
10×10 cm2 - Discharge-free operation also at high rate π-beam
• Similar efficiency for10×10 cm2 & 30×30 cm2 detectors• Small difference in the
electrode thickness• Analysis not final
• High efficiency with all gas mixtures
Ne/(5%CH4) - Ar/(5%CH4) - Ar/(7%CO2)
150 GeV µ & π beams Efficiency
Ar/(5%CH4) Ar/(7%CO2)
Ne/(5%CH4)
Gas gain ~104; effective gain ~103
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16
Beam studies
10×10 cm2 - Discharge-free operation also at high rate π-beam
• Higher multiplicity for 30×30 cm2 compared to that of 10×10 cm2 detectors• Analysis not final
• Also related to the naive production used• Misalignment between the
readout pads and painted pads on the resistive sheet
• Will be done more carefully in the new detector
Ne/(5%CH4) - Ar/(5%CH4) - Ar/(7%CO2)
150 GeV µ & π beams Efficiency & Multiplicity
Ne/(5%CH4)
Ar/(5%CH4) Ar/(7%CO2)
Gas gain ~104; effective gain ~103
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17
Beam studies
10×10 cm2 - Discharge-free operation also at high rate π-beam
• Similar rate dependence for both 10×10 cm2 & 30×30 cm2 detectors
• ~5% efficiency loss over 3 orders of rate magnitudes• Can be avoided by defining
higher nominal operation voltage
• Still maintain discharge-free operation
Ne/(5%CH4) - Ar/(5%CH4) - Ar/(7%CO2)
150 GeV µ & π beams Rate capabilities
Ar/(5%CH4)
Ar/(7%CO2)
Ne/(5%CH4)ΔVRPWELL=880 V
ΔVRPWELL=1700 V ΔVRPWELL=1710 V
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18
Beam studies
10×10 cm2 - Discharge-free operation also at high rate π-beam
• The current increases with the rate
• ‘Ohmic’ behavior is observed
Ne/(5%CH4) - Ar/(5%CH4) - Ar/(7%CO2)
150 GeV µ & π beams Rate capabilities
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19
Summary
S. Bressler
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Random order• Simple• Robust • Cost-effective
• Production• Operation (etc. gas mixtures)
• Large-area • Efficient • Resolution: spatial, time, energy• Broad dynamic range• Rate capabilities• Discharge free• Industrially produced
20
The RPWELLWish list
S. Bressler
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Random order• Simple• Robust • Cost-effective
• Production• Operation (etc. gas mixtures)
• Large-area • Efficient • Resolution: spatial, time, energy• Broad dynamic range• Rate capabilities• Discharge free• Industrially produced
• New design of large detector is ongoing• Additional characterization is on-going
21
The RPWELLWish list
![Page 22: Recent progress with the RPWELL detector · S. Bressler et al. 2013 JINST 8 P07017 • And more... S. Bressler. Random order • Simple • Robust • Cost-effective • Production](https://reader034.vdocument.in/reader034/viewer/2022051604/5ffbf60eb7f87804a443b36f/html5/thumbnails/22.jpg)
Random order• Simple• Robust • Cost-effective
• Production• Operation (etc. gas mixtures)
• Large-area • Efficient • Resolution: spatial, time, energy• Broad dynamic range• Rate capabilities• Discharge free• Industrially produced
• New design of large detector is ongoing• Additional characterization is on-going
22
The RPWELLWish list Applications
Random order• RICH devices
M. Alexeev et al. 2012 JINST 7 C02014
• Cryogenic detectors for TPC in neutrino physics and rare-event searchesM. Resnati et al. 2011 J. Phys.: Conf. Ser. 308 012016A. Bondar et al. 2011 JINST 6 P07008
• GPM for dark matter searchesL. Arazi et al. Expected online publication in JINST: November 2015
• Medical imagingS. Duval et al. 2011 JINST 6 P04007
• Neutron/Gamma imaging in cargo inspection systemsA. Breskin et al. 2012 JINST 7 C06008I. Israelashvili et al. 2015 JINST 10 P03030
• Thin sampling elements for DHCALS. Bressler et al. 2013 JINST 8 P07017
• And more...