cryogenic detector systems: recent work. · recent work. m.borri daresbury laboratory ukri-stfc...

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Cryogenic detector systems: recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR * . Nuclear physics: Prospectus. Conclusion. * not Ge sensor. See also BEGe cryostat I.Lazarus @ AGATA Week Milan, 2017.

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Page 1: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

Cryogenic detector systems:recent work.

M.BorriDaresbury Laboratory

UKRI-STFC

Outline:

• Photon-science: XH for x-rays and mid-IR∗.

• Nuclear physics: Prospectus.

• Conclusion.∗ not Ge sensor.

See also BEGe cryostatI.Lazarus @ AGATA WeekMilan, 2017.

Page 2: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

ESRF-ID24 upgrade.

• Extremely Brilliant Source ESRF: new lattice.

• ID24 refurbished to High Power Laser Facility (HPLF).

• Coupling 100J ns-Laser to 4th Generation Synchrotron.

• Pump-probe experiments in single shot.

• Experimental technique is Energy Dispersive EXAFS(EDE).

• ... And to upgrade XH.

Page 3: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

XH system.

• Radiation Harsh Environment:1014 γ/s on Active Area;

• Cryostat Unit:Coolant is LN2;Ge Sensor @ T<-170C;Front-End Electronics;Pwr [10-14W] @ T>-40C;

• DAQ Unit:Operated in Atmosphere;FPGA + µProcessor;CTRL, CLK, DATA;

• Upgrade:New Ge Sensors;New Cryostat;

Page 4: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

Micro-strip Ge sensors.

• Size: 1024 strips.

• Strip pitch: 50 um with 25um gap.

• Strip length: 5mm.

• Sensor thickness: 1.5mm.

• Two guard-rings.

• Interleaved wire-boning pads.

• Back illuminated.

Page 5: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

X3CHIP.

• STFC designed.

• Process: AMS 0.35um.

• Channels: 128.

• Analogue front-end:Charge integration;Charge sampling;

• Analogue output:32 chs per mux;4 mux per ASIC;

Page 6: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

DAQ.

• 14bit 50MHz ADC.

• Virtex5 (FX70) FPGA.

• Embedded micro-processor 400MHz.

• 1GByte Ethernet link.

Page 7: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

Prototyping: in-beam tests.

0 2 4 6Time [s] 1e 7

0.00

0.25

0.50

0.75

1.00

[a.u

.]

Sensor T~-157C;~7.5x103( @7.5keV)/700ns

Sam

plin

g fo

r:16

bun

ch a

nd 7

/8+1

Vbias-50VVbias-55VVbias-60VVbias-65VVbias-70VVbias-75VVbias-80VVbias-85VVbias-90VVbias-95VVbias-100V

0 2 4 6Time [s] 1e 7

0.00

0.25

0.50

0.75

1.00

[a.u

.]

Sensor T~-157C;V=-100V

Sam

plin

g fo

r:16

bun

ch a

nd 7

/8+1

Vbias=-100V

=7.52e+03( @7.5keV)/700ns=5.26e+03( @7.5keV)/700ns=3.79e+03( @7.5keV)/700ns=2.15e+03( @7.5keV)/700ns=1.11e+03( @7.5keV)/700ns=5.39e+02( @7.5keV)/700ns

• Anticipate shut-down.

• Enable early testing while stilldeveloping new cryostat.

• First assembly:New sensors;Old cryostat;

• Study Q-collection time Vs fill-patern.

• In-beam tests:Q-collection time Vs Voltage;Q-collection time Vs Flux;

Page 8: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

Mid-IR system.

• STFC Central Laser Facility.

• Electronic and structural dynamics atquantum level.

• Ultrafast [s]: 10−3-10−15.

• Chemistry, physics and biology.

• Mid-IR detectors with STFC Technology.

• Sensor selection ongoing: not Ge!

Page 9: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

Starting point

• XH system: not upgraded cryostat.

• Max 4 XCHIPs to r/o up-to 512 strips.

• Sensor T: -297C (or below?).

• Mod the current design to build ademonstrator.

0.0 2.5 5.0 7.5 10.0 12.5 15.0 17.5Pwr [W]

150

100

50

0

50

T_hb

Brd

[C]

Chassis@RoomT; hdBrd; y=12.3x-154.4

200

190

180

170

160

150

140

130

120

T_cld

Plt &

T_c

ldFn

g [C

]

Chassis@RoomT; cldPlt; y=1.97x-190.2Chassis@RoomT; clFng; y=1.28x-192.8

Page 10: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

Study on head-board module.

• 4 XCHIP, pwr [W]: 5-7.

• THB > -40C.

• Increased thermal resistivity.

• Torlon spacer non-linearity becomesdominating factor.

0 1 2 3 4 5 6 7Pwr [W]

160

140

120

100

80

60

40

20

0

T [C

]

Head-board module4x16mm screws; y=15.32x-161.44x14mm screws; y=16.05x-154.63x14mm screws; y=18.05x-135.92x14mm screws; y=19.42x-125.1

Page 11: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

Low IR contribution.• Low IR contribution to T.

• No IR-shield installed.

• Heated chassis and checked effect oncomponents.

• To repeat with IR-shield.

10 20 30 40 50 60 70T_chassis [C]

200

190

180

170

160

150

140

130

120

[C]

IR contributionhd-brd; y=0.58x-163.4cld-plt; y=0.11x-191.8cld-fng; y=0.08x-193.8

Page 12: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

Prospectus.

• Compton camera.

• Nuclear medicine.

• Low dose diagnostics.

• Single Photon Emission ComputedTomography (SPECT).

• Scatterer and absorber in samecryostat.

• Cryostat characterization ongoing.-Vacuum;-Temperature;

Page 13: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

Vacuum tests.• P measured in vessel.

• Comparing P cycles.

• Base-line pressure in vessel.

• LN2 burn-rate @ 0W.

• Next:-TminVsVac;-Pump-speedVsTemp;-TempVsPwr;

0 2 4 6 8 10 12[days]

10 5

10 4

10 3

10 2

10 1

100

[mba

r] At room TNo venting between cycles

Repeated cycles

pumping cycle 0pumping cycle 1outgassing cycle 0outgassing cycle 1

0 5 10 15 20 25 30 35[days]

10 6

10 5

10 4

10 3

10 2

10 1

100

[mba

r] Big spikes during cold periodare due to LN2 refill.

Rem

oved

from

pum

p,st

art c

oolin

g.

Star

t war

m-u

p

Stability

0 2 4 6 8 10[day]

40

45

50

55

60

65

[kg]

Only IR No additional pwr

LN2 brun-rate

y=-2.0x + 61.7y=-2.1x + 61.0y=-2.1x + 60.5

Page 14: Cryogenic detector systems: recent work. · recent work. M.Borri Daresbury Laboratory UKRI-STFC Outline: Photon-science: XH for x-rays and mid-IR . Nuclear physics: Prospectus. Conclusion

Conclusion.

• Results of the XH system for X-rays.

• T optimisation for a possible demonstrator for Mid-IR.

• Characterisation of Prospectus cryostat.