Page 1 1 The TORCH PMT: A close packing, multi-anode, long life MCP-PMT for Cherenkov applications...
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Transcript of Page 1 1 The TORCH PMT: A close packing, multi-anode, long life MCP-PMT for Cherenkov applications...
page 1www.photek.co.uk1
The TORCH PMT:A close packing, multi-anode, long life MCP-PMT for Cherenkov applications
James Milnes
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk2
Photek MCP-PMTs
• Photek currently manufacture
the fastest PMTs in the world in
“analogue mode”:
– Whole pulse is captured by an
oscilloscope or digitiser
– Applications often “single-shot,
high intensity”, e.g. Fusion
Research
– We have several detectors on
the diagnostics at the National
Ignition Facility
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk3
Photek MCP-PMTs
• MCP-PMTs are also the leading detector for
time-resolved photon counting
• Jitter in photon arrival measurements ~ 30
ps FWHM
– Significantly better for multi-photon events
• Excellent fit for Cherenkov-based particle
detection
• Drawbacks:
– Detector Lifetime
– Most models are round, single anode and
not close-packing
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk4
The TORCH PMT
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
• In November 2012 Photek started the 3-year development of the
TORCH (Timing Of internally Reflected CHerenkov photons) PMT
• A collaboration with CERN and the Universities of Oxford and Bristol
for the LHCb upgrade
– See talk by Maarten Van Dijk, Thursday 14.50
• Technical aims:
– A lifetime of 5 C/cm2 of accumulated anode charge or better
– A multi-anode readout of 8 x 128 pixels
– Close packing on two apposing sides with a fill factor of 88% or better
• 53 mm working width within a 60 mm envelope
www.photek.co.uk5
The TORCH PMT
• Three main aims:
1. Lifetime
2. High granularity multi-anode
3. Square
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk6
1. MCP-PMT Lifetime
• Standard MCP detectors suffer from sensitivity loss after prolonged
exposure:
– An MCP has a very large surface area
– Prolonged electron bombardment of this surface releases material that
is ionised
– These ions are drawn back to the photocathode and reduce sensitivity
• Previous solutions have involved barrier films to prevent the ions
reaching the photocathode
– Limited success
– Lowers MCP efficiency and overall sensitivity
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk7
1. MCP-PMT Lifetime• Recent technology of ALD (Atomic Layer Deposition) coating on MCP has significantly
reduced out-gassing
• Two PMT samples produced in 2011: Double-MCP 10 mm diameter working area
– One with coated MCPs, One control with standard MCPs
• Independently verified by Photek and others: Britting et al (PhotoDet 2012), Conneely et al (VCI 2013)
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk8
1. MCP-PMT Lifetime
300.0n 400.0n 500.0n 600.0n 700.0n 800.0n 900.0n0.0
10.0m
20.0m
30.0m
40.0m
50.0m
60.0m ALD Coated MCP-PMT Accumulated Anode Charge:
0 C/cm2
0.38 C/cm2
0.71 C/cm2
1.13 C/cm2
1.95 C/cm2
2.49 C/cm2
3.18 C/cm2
3.71 C/cm2
5.11 C/cm2
Pho
tocu
rren
t (A
/W)
Wavelength (m)300.0n 400.0n 500.0n 600.0n 700.0n 800.0n 900.0n
0.0
10.0m
20.0m
30.0m
40.0m
50.0m
60.0m Uncoated MCP-PMT Accumulated Anode Charge:
0 C/cm2
0.13 C/cm2
0.17 C/cm2
0.20 C/cm2
0.25 C/cm2
0.28 C/cm2
0.30 C/cm2
0.32 C/cm2
0.36 C/cm2
Pho
tocu
rren
t (A
/W)
Wavelength (m)
• ALD coating results in no detectable
sensitivity loss after > 5 C/cm2
• Some gain reduction
• 6 test devices produced, 2 successfully
life tested at Photek, 1 currently being
tested at CERN
-0.5 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.5 5.0 5.5 6.0
105
106
Gai
n
Integrated Anode Charge (C/cm2)
B5130419Volts per MCP:
600 V 550 V 500 V
G2130614Volts per MCP:
650 V 600 V 550 V
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk9
1. MCP-PMT Lifetime• 1st year objective: produce 5
long-life MCP-PMTs
– 1st build cycle produced 6
double-MCP devices plus 1
control
– ALD also gives major gain
enhancement
– A 2nd build cycle will
attempt to produce a
photon counting device
with 1 MCP800 1000 1200 1400 1600 1800 2000
102
103
104
105
106
107
Ga
in
Voltage across MCP pair (V)
G1130614 (modified scrub) G2130614 (modified scrub) G1130510 G2130510 B1130419 B4130419 (control) B5130419
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk10
1. MCP-PMT Lifetime• In other respects, coated MCPs behave
as normal
• Jitter measurement made with 40 ps
laser source
105 106 107 108
Voltages: 200 600 600 1000 200 650 650 1000 200 700 700 1000 200 750 750 1000
PMT225 G1130510PHD
Co
un
ts (
no
rma
lise
d)
Gain
0.0 2.0n 4.0n 6.0n 8.0n 10.0n
-0.7
-0.6
-0.5
-0.4
-0.3
-0.2
-0.1
0.0
PMT225 G1130510200 750 750 1000LPG-1 @ 10 KHz6 dB AttenuatorAveraged 16 times
Vo
ltag
e (
V)
Time (s)
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk11
1. MCP-PMT Lifetime• At the RICH conference in Japan 2013 Albert Lehmann observed
substantial gain non-uniformity with ALD coated MCPs
• We tried to repeat this observation but could not detect anything
significant
This region is due to an artefact in our scanning software
This region shows the gain suppression after the life test
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk12
2. High granularity multi-anode• Traditional multi-anode manufacturing uses multiple
pins brazed through a solid ceramic
• Prone to leaking, also unrealistic for a 128 x 8 array!
• Our aim is to use multilayer
ceramic with filled vias
• Much smaller pad size allows
for finer pitch
• The pads on this design are
0.75 mm wide on a 0.88 mm
pitch
Vacuum side Air side
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk13
2. High granularity multi-anode
• Contact made to anodes by
Anisotropic Conductive Film
(ACF)
– ACF are filled with conductive
particles which provides electrical
interconnection between pads
through the film thickness (z-
direction)
– The conductive particles are
distributed far apart thus not
electrically conductive in the
plane direction (x & y) of the film
– PCB could contain front-end
electronics and/or connectors
Detector
ACF
PCB
x
yz
ACF is insulating in x and y but conducting in z
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk14
2. High granularity multi-anode - readout• NINO ASIC
• 32 channel differential amplifier
/discriminator developed at CERN
• 10 ps RMS jitter on the leading
edge
• >>10 MHz maximum rate
• The time-over-threshold technique
uses the discriminator output pulse
width to determine the event
charge
• High Performance Time-to-Digital
Convertor (HPTDC)
• A programmable TDC developed for
ALICE time-of-flight RPCs at the LHC
• Two modes of 100 ps LSB resolution
with 32 channels, or 24.4 ps LSB
resolution with 8 channels
• Default maximum rate is 2.5 MHz per
channel, can be increased beyond 10
MHz using higher logic clock
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk15
2. High granularity multi-anode• Using a method of charge
sharing between pads, we can
reduce the channel count and
the required granularity of the
multi-anode structure
• The plot shows the simulated
position resolution of a parallel
readout, charge sharing
detector (using the NINO and
HPTDC as readout electronics)
in the fine direction of the
required 8 × 64 pad layout but
aiming for 8 × 128 resolution
• The position resolution strongly
depends on the NINO threshold
and detector gain, with this plot
showing a gain of 1 × 106 or
greater being required to
achieve the desired resolution
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk16
3. Square Tube Development
• Square tube manufacturing is new to Photek
• Currently developing methods of
– Square body brazing
– Square MCP locating
– Square photocathode sealing
– Square anode sealing
• Current status:
– Producing leak-tight square test cells
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk17
3. Square Tube Development – Anode Seal
• Traditional method of sealing
anode – welding – is unusable
due to close packing
requirements
• We are experimenting with
– Indium seal
– Brazing
– Fritting
2 inch square body with solid ceramic anode indium sealed
Indium seal
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk18
Summary
• TORCH PMT in development at Photek
• 3 year development aims to finish in November 2015
• 1st year task complete: To produce long-life demonstrators
• 2nd year task on-going: To produce high-granularity multi-anode
demonstrator
• Final year task: Fully functioning detector
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014
www.photek.co.uk19
Thank you for listening
Workshop on picosecond photon sensors for physics and medical applications, Clermont Ferrand 12th March 2014