Difference between revisions of "SiPM Radiation Hardness Test"

Revision as of 17:51, 8 September 2010

Introduction

The of goal of the SiPM Radiation Hardness tests is to reasonably predict the life time of such a detector in normal Hall D GlueX production running as the readout of BCal. Since most of the damage to SiPM is expected coming from neutron, the study is focused on the neutron damage only. A series of tests have been performed with both electron beam on Pb target at Hall A and RadCon AmBe neutron source.

Probing Neutron and Its Damage to Silicon Detectors

Neutron probe

The neutron flux in both Hall A and RadCon neutron source is measured by portable neutron survey meter (BF₃) [1]. What this probe measures is equivalent dose [2] in the unit of rem, which is a measure of the radiation dose to tissue where an attempt has been made to allow for the different relative biological effects of different types of ionizing radiation.

The conversion coefficients are plotted here according to ICRP 74 [3]

Damage to silicon detector

Numerous observations have led to the result that damage effects by energetic particles in the bulk of any material can be described as being proportional to the so called displacement damage cross section. This quantity is equivalent to the Non Ionizing Energy Loss (NIEL) and hence the proportionality between the NIEL-value and the resulting damage effects is referred to as the NIEL-scaling hypothesis. The NIEL-value can also be referred to as the displacement-KERMA, i.e. the Kinetic Energy Released to MAtter (in this case silicon)

As recommended for the LHC silicon detector study, the equivalent neutron radiation damage to silicon detector normalized to 1 MeV neutron is plotted here [4].

Conversion from rem to 1MeV neutron fluence

With the previous two kinds of conversion factors and neutron energy spectrum, one can convert the measured neutron flux to 1 MeV neutron fluence.

Irradiation in Hall A

Test setup

• The test was performed in Hall A during P-Rex experiment [5]
• Electron beam energy: 1 GeV
• Target: 0.5 mm Pb
• Location of SiPM: 135 degrees backward, 20 meters away from target
• More details can be found in Test Plan and Setup in Hall A

Simulation

Dr. Pavel Degtiarenko did a simulation using GEANT3 for the neutron background in Hall A. The result of neutron energy spectrum is shown [6]

Conversion factor for Hall A

• Dose to fluence: 1 rem → 2.4 × 10⁷ n_eq/cm²

Rate estimation

• Estimated dose rate: 3.1 rem/H
  • The dose rate estimation with 0.5 mm Pb target and 50 μA is 7.64 rem/H.
  • In reality, the Pb target thickness was gradually reduced due to the beam damage, the effective thickness of the target during the SiPM irradiation was found to be 40% using the relative change of the neutron neutron dose rate measured by the neutron probe:
    • 03/28/2010 11:00: 950 mrem/H@22.8 μA → 2.12 rem/H@50 μA (Pb#3 first time in beam)
    • 04/06/2010 07:00: 1.53 rem/H@44.2 μA → 1.73 rem/H@50 μA (Pb#3 last time w/o collimator)
    • 04/16/2010 02:00: 0.99 rem/H@18.0 μA → 2.75 rem/H@50 μA (Pb#3 first time w/ collimator)
    • 04/20/2010 22:00: 1.41 rem/H@49.7 μA → 1.42 rem/H@50 μA (Start of SiPM test)
    • 04/22/2010 09:00: 1.30 rem/H@49.5 μA → 1.31 rem/H@50 μA (End of SiPM test)

• Measured dose rate: 5.3 rem/H
  • 1.3 rem/H from raw reading.
  • The neutron probe underestimates the actual Hall A dose rate by a factor 4.1 due to lack of sensitivity to high energy neutrons (>20 MeV). Such a factor was calculated by comparing to the damage results with AmBe source (calibration of neutron probe).
  • Very good agreement to the simulation.

• 1 MeV equivalent neutron fluence (simulation): 21000 n_eq/s/cm²

3×3 mm² SiPM test in Hall A

• Time of irradiation: 04/20/2010 21:00 - 04/22/2010 07:00
• Final dose: 174 rem (measured & corrected)
• Temperature: 21.3°C
• Initial dark current: 8.2 μA for Hamamatsu and 125 μA for SensL

Immediate damage results

• Dark current linearly increases as a function of 1MeV neutron fluence.
• Whether or not power the SiPM will not change the damage effect (the power was turned off on purpose during the big blank period).

• Compmared to the change of dark current, the changes of the signal shape (gain and the width) are very small. The colors represent the neutron dose: red (initial) -> violet (final)

Signals of Hamamatsu SiPM with radiation growing

Signals SensL SiPM with radiation growing

Signal Amplitude gradually decreases as a function of radiation dose while no change of its width observed.

• The VI responses of both SiPMs were not effected by the radiation: no change of break down voltages.

Comparison of VI curves of Hamamatsu unit before and after radiation

Comparison of VI curves of SensL unit before and after radiation

Recovery from radiation damage

• The dark current from both SiPM samples recovered by about 50% with time constant of 10 days.
• The gain was fully recovered.
• Taking the bias voltage adjustment into account, the dark current has an exponential relation to the ambient temperature:
  • I(dark) ~ exp(a*(T-T0))
  • a for Hamamatsu: 0.061±0.003/C
  • a for SensL: 0.047±0.002/C

Recovery of SiPM dark current, fit with initial point.

Recovery of SiPM dark current, fit without initial point.

Recovery of SiPM gains, fit without initial point.

Other info

• Report to GlueX meeting (2010/05/10): link to docDB
• Dark rate measurement shows a increase of noise level consistent with the increase of dark current:Carl's report
  • I_dark ~ σ_pedestal²

1×1 mm² SiPM test in Hall A

• Temperature: ~ 21.3 degree C
• SiPM Serial Number: 1260
• Irradiation time: 06/11/2010 11:20 - 06/15/2010 10:00
• Total dose: 141 Rem (34.3 rem x 4.1)

Test Result

• ADC dark spectrum before/after irradiation and two months later

• Formula used in the fit:
  • 
  • 
• Note: the pre-amplifier used in the first two tests (before and post) was from Stepan with a total gain of 105 while during the last test (anneal) the pre-amplifier from Fernando was used with a gain of 65.
• Immediate increase of dark rate: factor of 37
• Permanent increase of dark current: factor of 18: Carl's measurement
• Permanent increase of dark rate: factor of 21
• Cross-talk: 15%

Irradiation with RadCon AmBe Source

Conversion factor for AmBe neutron source

• The AmBe source has an narrow neutron energy spectrum averaged at 4 MeV [7] page82

• Dose to fluence: 1 rem → 3.3×10⁷n_eq/cm²

Test Condition

• The AmBe source in RadCon has the following dose rate:

 dose rate = [13/D2]*[1+(0.248*D)2.2375*e-0.3536*D] mrem/H

where D is the distance from the source in the unit of meter

• One 1×1 mm² and one 3×3 mm² SiPMs from Hamamatsu together with their pre-amplifiers were irradiated by this source
• The distance is 17 cm and dose rate is 0.45 rem/H
• Irradiation time: 07/12/2010 14:40 - 07/15/2010 14:25
• Total dose: 32±2 rem

Results

1x1 mm SiPM

• ADC spectra before/after irradiation and 1 month later:

• Immediate increase of dark current: factor of 6.4 Carl's Measurement
• Permanent increase of dark current: factor of 4
• Permanent increase of dark rate: factor of 3.5
• Cross talk: 13%

3x3 mm SiPM

• ADC spectra before/after irradiation and 1 month later:

• Immediate increase of dark current: factor of 7.1 Carl's Measurement
• Permanent increase of dark current: factor of 4.7
• Permanent increase of dark rate: factor of 4.1
• Cross talk: 14%

Calibration of neutron probe for Hall A measurement

• Use the increase of dark current as a bench mark
  • WIth AmBe source, it took 32 rem to permanently increase the Hamamatsu SiPM dark current by a factor of 4.4.
    • 32 rem → 1.06×10⁹ n_eq/cm²
  • In Hall A, with Pb target, it took 11 rem (measured, NOT corrected, 8.2 hours with 1.3 rem/H dose rate) to permanently increase the Hamamatsu SiPM dark current by a factor of 4.4.
    • 11 rem → 2.6×10⁸ n_eq/cm²
  • The correction factor should be: 1.06×10⁹/2.6×10⁸ = 4.1

Fluence simulation of Hall D

Pavel recently updated his simulation for the neutron flux through SiPMs with normal Hall D production condition.

Simulation Condition and Results

• Detector location: Z = 462 cm
• Rate of photon beam before collimator: 11 GHz
• Dose rates and energy spectra with Hydrogen target
• Flux in downstream SiPM area with Hydrogen target
• Flux in upstream SiPM area with Hydrogen target
• Dose rates and energy spectra with Helium target
• Flux in SiPM area with Helium target
• Flux in upstream SiPM area with Helium target

Hydrogen Target

Downstream Detector

• The energy spectrum of neutron from Hydrogen target:

• Dose to fluence: 1 rem → 2.6×10⁷ n_eq/cm²
• At 65-90 cm
  • Dose rate: 4.3-3.3 mrem/H
  • Total neutron flux: 90-76 Hz/cm² (54-43 forward, 37-33 backward)
  • Neutron flux > 10 MeV: 4.3-2.6 Hz/cm² (3.1-1.7 forward, 1.2-1.0 backward)
  • 1 MeV equivalent neutron fluence: 31-23 n_eq/s/cm²

Upstream Detector

• The energy spectrum of neutron from Hydrogen target:

• Dose to fluence: 1 rem → 2.7×10⁷ n_eq/cm²
• At 65-90 cm
  • Dose rate: 1.0-0.4 mrem/H
  • Total neutron flux: 20-16 Hz/cm² (3.5-3.2 forward, 17-13 backward)
  • Neutron flux > 10 MeV: 0.7-0.4 Hz/cm² (0.1-0.0 forward, 0.6-0.4 backward)
  • 1 MeV equivalent neutron fluence: 8-3 n_eq/s/cm²

Helium Target

Downstream

• The energy spectrum of neutron from Helium target:

• Dose to fluence: 1 rem → 2.6×10⁷ n_eq/cm²
• At 65-90 cm
  • Dose rate: 6.5-4.9 mrem/H
  • Total neutron flux: 140-108 Hz/cm² (94-67 forward, 46-41 backward)
  • Neutron flux > 10 MeV: 7.0-4.0 Hz/cm² (5.6-3.0 forward, 1.3-1.1 backward)
  • 1 MeV equivalent neutron fluence: 47-35 n_eq/s/cm²

Upstream

• The energy spectrum of neutron from Helium target:

• Dose to fluence: 1 rem → 2.4×10⁷ n_eq/cm²
• At 65-90 cm
  • Dose rate: 1.2-0.8 mrem/H
  • Total neutron flux: 35-28 Hz/cm² (4.0-3.8 forward, 31-24 backward)
  • Neutron flux > 10 MeV: 1.5-1.1 Hz/cm² (0.5-0.1 forward, 1.0-1.0 backward)
  • 1 MeV equivalent neutron fluence: 8-6 n_eq/s/cm²

Life Time of SiPMs in Hall D

• Our current calorimeter design allows a factor 5 increase of the dark noise, and the 1 MeV neutron fluence needed according to Hall A simulation: 10 hours of 50 μA beam → 31 rem → 7.4×10⁸n_eq
• At 65-90 cm (inner-outer radius of BCal), to reach same 1 MeV neutron fluence:
  • Hydrogen target: 0.8-1.0 years for downstream and 3-8 years for upstream of full-time running
  • Helium target: 0.5-0.7 years for downstream and 3-4 years for upstream of full-time running
• Factors to increase life time of SiPM
  • Running efficiency: 33%
  • Lower temperature: 20°C→5°C will reduce the dark rate by a factor of 3 (has been very verified with non-irradiated samples).
• Expected life time with high luminosity production (10⁸ γ):
  • 7 - 9 years for Hydrogen target
  • 4.5 - 6 years with Helium target

Future Test Plan with Radcon AmBe Source

Tests with previously irradiated samples

• Revisit noisy 1x1 mm² SiPM sample from Hall A (done)
  • Increase of dark rate compared to the one irradiated with AmBe source and showed a factor of 2.2 discrepancy:

20(increase in Hall A) x 32 rem(dose with AmBe) x 3.3 (conversion for AmBe)/2.8(increase with AmBe)/140 rem(dose in Hall A)/2.4(conversion for Hall A) = 2.2

• Uniformity test of the 4x4 3x3 mm² array from Hall A
• Measure permanent damage of all the irradiated samples (done)

Temperature test with AmBe source

• Purchase 12 1x1 samples from Hamamatsu product page
• Set up a DAQ test platform in F117 (done)
• Irradiate all of them with AmBe source to 30 rem (4 days), 6 at 0 degree, 6 at room temperature
• Annealing test of all the samples at three different temperatures: 0, 20 and 60 degrees for 20 days

Parasitic Test

• Re-irradiate old samples to see potential change of the damage rate
• Irradiate SiPM used in tagger hall