AIT-WATCHMAN A Remote Reactor Monitor and Advanced Instrumentation - - PowerPoint PPT Presentation

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AIT-WATCHMAN A Remote Reactor Monitor and Advanced Instrumentation - - PowerPoint PPT Presentation

AIT-WATCHMAN A Remote Reactor Monitor and Advanced Instrumentation Testbed Christopher Grant On behalf of the WATCHMAN Collaboration The link between nuclear reactors and nuclear weapons 235 U 85 Kr A source of fissionable material, ! such as


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SLIDE 1

AIT-WATCHMAN

A Remote Reactor Monitor and Advanced Instrumentation Testbed

Christopher Grant

On behalf of the WATCHMAN Collaboration

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SLIDE 2

The link between nuclear reactors and nuclear weapons

September 11, 2019 TAUP 2019 - Toyama, Japan 1

!

235U 85Kr 141Ba Energy

! ! !

235U 235U

A source of fissionable material, such as 235U, is required to manufacture nuclear weapons However, 235U is not ideal due to its rare isotopic abundance (0.7%) and the challenge of achieving over 90% enrichment needed for a weapon

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SLIDE 3

September 11, 2019 TAUP 2019 - Toyama, Japan 2

The link between nuclear reactors and nuclear weapons

!

238U

An alternative method, and one that was used by many countries, involves the production of 239Pu via the transmutation of natural Uranium inside a nuclear reactor

239U

"

#/%~ 23 min

' ()

239Np

"

#/%~ 2.4 days

239Pu

"

#/%~ 24,000 years

' () ̅ + ̅ + Plutonium can be easily separated from Uranium with chemistry

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SLIDE 4

Reactors are operating all over the world

September 11, 2019 TAUP 2019 - Toyama, Japan 3

  • S. M. Usman, G. R. Jocher, S. T. Dye, W. F. McDonough, and J. G. Learned, Scientific Reports 5, Article number: 13945 (2015)
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SLIDE 5

Non-Proliferation Treaty (NPT) – an attempt to mitigate the risk

September 11, 2019 TAUP 2019 - Toyama, Japan 4

Nuclear Weapon State Ratifiers Nuclear Weapon State Acceders Other Ratifiers Other Acceders or Succeeders Withdrawn Non-signatory Unrecognized State, abiding by acceders

These agreements are supported by physical measurements and monitoring systems overseen the International Atomic Energy Agency (IAEA) and the Comprehensive Nuclear-Test-Ban Treaty Organization (CTBTO)

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SLIDE 6

Can neutrinos be used to monitor distant reactors?

September 11, 2019 TAUP 2019 - Toyama, Japan 5

Roughly 6 ̅ "# released per fission and ~1021 fissions per second in a typical 3 GWt power reactor, means that you have ~1022 ̅ "# per second isotropic emission

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SLIDE 7

Can neutrinos be used to monitor distant reactors?

September 11, 2019 TAUP 2019 - Toyama, Japan 6

25 km stand-off

Water Cherenkov Detector

Inverse Beta Decay (IBD):

̅ "# + % → '( + )

Roughly 6 ̅ "# released per fission and ~1021 fissions per second in a typical 3 GWt power reactor, means that you have ~1022 ̅ "# per second isotropic emission

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SLIDE 8

Can neutrinos be used to monitor distant reactors?

September 11, 2019 TAUP 2019 - Toyama, Japan 7

25 km stand-off

! " ~ 10&'( cm( "+

(

Water Cherenkov Detector

Inverse Beta Decay (IBD):

̅

  • . + 0 → 23 + 4

Can expect “several” interactions per kiloton of water per day at 25 km distance Roughly 6 ̅

  • . released per fission and ~1021

fissions per second in a typical 3 GWt power reactor, means that you have ~1022 ̅

  • . per

second isotropic emission

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SLIDE 9

Can neutrinos be used to monitor distant reactors?

September 11, 2019 TAUP 2019 - Toyama, Japan 8

25 km stand-off

! " ~ 10&'( cm( "+

(

Water Cherenkov Detector

Inverse Beta Decay (IBD):

̅

  • . + 0 → 23 + 4

Can expect “several” interactions per kiloton of water per day at 25 km distance

Monitoring capability with antineutrinos studied in great detail in the following reference:

  • A. Bernstein, et al., Science & Global Security, 18:127–192, 2010

Roughly 6 ̅

  • . released per fission and ~1021

fissions per second in a typical 3 GWt power reactor, means that you have ~1022 ̅

  • . per

second isotropic emission

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SLIDE 10

AIT-WATCHMAN

September 11, 2019 TAUP 2019 - Toyama, Japan 9

(Advanced Instrumentation Testbed – WATer CHerenkov Monitor of ANtineutrinos)

NNSA’s Office of Defense Nuclear Nonproliferation has funded WATCHMAN R&D since 2012. Mission need: demonstrate and evaluate the viability and scalability

  • f antineutrino-based technologies for remote reactor discovery and monitoring.
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SLIDE 11

AIT-WATCHMAN

September 11, 2019 TAUP 2019 - Toyama, Japan 10

(Advanced Instrumentation Testbed – WATer CHerenkov Monitor of ANtineutrinos)

Primary Goals:

  • Confirm existence of an operating reactor (ie. determine unknown reactor is
  • perating in presence of another known reactor)
  • Determine power plant operational status with and without prior knowledge
  • Demonstrate Gd-loaded water as a scalable detector medium
  • Enable future technology upgrades:

Water-based liquid scintillator WbLS, Large-Area Picosecond Photodetectors (LAPPDs), techniques for Cherenkov and scintillation light separation, etc. NNSA’s Office of Defense Nuclear Nonproliferation has funded WATCHMAN R&D since 2012. Mission need: demonstrate and evaluate the viability and scalability

  • f antineutrino-based technologies for remote reactor discovery and monitoring.
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SLIDE 12

AIT-WATCHMAN

September 11, 2019 TAUP 2019 - Toyama, Japan 11

Hartlepool Reactor AIT-WATCHMAN at Boulby Underground Lab

(Advanced Instrumentation Testbed – WATer CHerenkov Monitor of ANtineutrinos)

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SLIDE 13

AIT-WATCHMAN

September 11, 2019 TAUP 2019 - Toyama, Japan 12

Hartlepool Reactor AIT-WATCHMAN at Boulby Underground Lab

25 km

(Advanced Instrumentation Testbed – WATer CHerenkov Monitor of ANtineutrinos)

Hartlepool Reactor has two cores, each operates at a power of 1.5 GWt for a total of just over 3 GWt

WATCHMAN

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SLIDE 14

Baseline WATCHMAN Detector Design

September 11, 2019 TAUP 2019 - Toyama, Japan 13

  • Gd-doped (0.1%) water Cherenkov detector
  • ~1 kiloton fiducial volume
  • ~3600 high quantum efficiency, low radioactivity,

10” PMTs (~20% photocathode coverage)

  • Active outer veto
  • Multiple calibration system access ports and large

central access plug for future instrumentation Gd-loaded water was chosen because of it’s scalability over other media - it’s the most viable path to a 100 kt – 1 Mt scale detector

Cutaway view

~20 m ~20 m

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SLIDE 15

Advantages of gadolinium loading

September 11, 2019 TAUP 2019 - Toyama, Japan 14

̅ "# $ %

Gd

& & &

Prompt signal Delayed signal (~8 MeV gamma cascade)

'(

Gd provides roughly 70% neutron detection efficiency in WATCHMAN

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SLIDE 16

Gd-loading demonstrator

September 11, 2019 TAUP 2019 - Toyama, Japan 15

The Gd-loading and water purification system is based on EGADS (Evaluating Gadolinium’s Action on Detector Systems). This was built to test Super-K detector materials in contact with Gd-doped water. System is essentially lossless – it extracts Gd, purifies the water, and adds the Gd back in. Water transparency remained within the SK ultra-pure range for over two years.

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SLIDE 17

Backgrounds for reactor monitoring

September 11, 2019 TAUP 2019 - Toyama, Japan 16

Gammas from radioactivity within detector materials or within the internal water volume Detector related backgrounds (random coincidences) γ γ In addition to antineutrinos from the Earth and from other nuclear reactors, the following backgrounds need to be addressed…

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SLIDE 18

Backgrounds for reactor monitoring

September 11, 2019 TAUP 2019 - Toyama, Japan 17

Gammas from radioactivity within detector materials or within the internal water volume Detector related backgrounds (random coincidences) γ γ In addition to antineutrinos from the Earth and from other nuclear reactors, the following backgrounds need to be addressed… "

#

Fast neutrons from nearby rock muons "

9Li

Long-lived radionuclides produced by spallation (9Li and 8He) that undergo $-decay with neutron emission

#

Cosmogenic related backgrounds (correlated events)

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SLIDE 19

Background Measurements

September 11, 2019 TAUP 2019 - Toyama, Japan 18

PRELIMINARY Multiplicity And Recoil Spectrometer (MARS)

Plastic scintillator + GdO2 (1%) 12 layer detectors Neutron converter

  • 3,560 lbs of lead

in a steel table Neutron energy spectrum was measured by MARS at three different depths in Kimbleton Underground Research Facility (KURF). The data was compared with an existing model and other measurements.

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SLIDE 20

Background Measurements

September 11, 2019 TAUP 2019 - Toyama, Japan 19

Neutron multiplicity 2 3 4 ]

  • 1

Rate [day

2 −

10

1 −

10 1 10

Data FLUKA Geant4

PRELIMINARY

2-ton Gd-loaded water target surrounded by pure water veto

WATCHBOY Detector

Watchboy was deployed at the same depth as

  • MARS. FLUKA simulations of neutrons in

WATCHBOY, using the MARS measured neutron energy spectrum as input, agree with the data.

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SLIDE 21

Boulby Underground Laboratory

September 11, 2019 TAUP 2019 - Toyama, Japan 20

Depth of 1.1 km (2805 mwe) Cleanliness in the underground lab will reduce the impact of dust and other environmental contamination This facility is well-established, hosting a variety of low- background particle physics experiments and other multidisciplinary projects

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SLIDE 22

Estimated sensitivity for the baseline design

September 11, 2019 TAUP 2019 - Toyama, Japan 21

Component Events/week Core-1 4.2 Core-2 4.2 World reactors 1.5 Accidentals 0.9 Fast neutrons* 0.6 Radionuclides 0.1 Total 11.3

*Fast neutron sims with FLUKA still in progress

Summary of background budget WATCHMAN simulations use combination of customized rat-pac with BONSAI for event reconstruction

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SLIDE 23

Estimated sensitivity for the baseline design

September 11, 2019 TAUP 2019 - Toyama, Japan 22

! (1) Observe any reactor ̅ ! signal over background?

25 km

unknown

~1 week of detector live time (95% C.L.)

Component Events/week Core-1 4.2 Core-2 4.2 World reactors 1.5 Accidentals 0.9 Fast neutrons* 0.6 Radionuclides 0.1 Total 11.3

*Fast neutron sims with FLUKA still in progress

Summary of background budget WATCHMAN simulations use combination of customized rat-pac with BONSAI for event reconstruction

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SLIDE 24

Estimated sensitivity for the baseline design

September 11, 2019 TAUP 2019 - Toyama, Japan 23

! (1) Observe any reactor ̅ ! signal over background?

25 km

! (2) Observe the presence of another reactor?

25 km

!

unknown known unknown

~1 week of detector live time (95% C.L.) ~1 month of detector live time (95% C.L.)

Component Events/week Core-1 4.2 Core-2 4.2 World reactors 1.5 Accidentals 0.9 Fast neutrons* 0.6 Radionuclides 0.1 Total 11.3

*Fast neutron sims with FLUKA still in progress

WATCHMAN simulations use combination of customized rat-pac with BONSAI for event reconstruction Summary of background budget

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SLIDE 25

Estimated sensitivity for the baseline design

September 11, 2019 TAUP 2019 - Toyama, Japan 24

! (1) Observe any reactor ̅ ! signal over background?

25 km

! (3) Observe ON/OFF transition of one reactor?

25 km

!

known known unknown

~1 week of detector live time (95% C.L.) ~10 months of detector live time (95% C.L.)

Component Events/week Core-1 4.2 Core-2 4.2 World reactors 1.5 Accidentals 0.9 Fast neutrons* 0.6 Radionuclides 0.1 Total 11.3

*Fast neutron sims with FLUKA still in progress

Summary of background budget WATCHMAN simulations use combination of customized rat-pac with BONSAI for event reconstruction ! (2) Observe the presence of another reactor?

25 km

!

unknown known

~1 month of detector live time (95% C.L.)

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SLIDE 26

Approximate Timeline for WATCHMAN

September 11, 2019 TAUP 2019 - Toyama, Japan 25

2019 2020 2021 2022 2023 2024 2025

Design Phase Excavation AIT Installation Commission/Calibrate WATCHMAN

2026 2027

AIT Future

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SLIDE 27

Future R&D for the Advanced Instrumentation Testbed (AIT)

September 11, 2019 TAUP 2019 - Toyama, Japan 26

We are actively pursuing technology that could be deployed in WATCHMAN to greatly enhance reactor monitoring and increase physics

  • potential. Improved calorimetry, particle ID,

and directionality are key interest. Water-based Liquid Scintillator (WbLS) Large Area Picosecond Photodetectors (LAPPDs) Dichroic Winston Cones (“Dichroicons”)

Courtesy of T. Kaptanoglu (U. Penn), DPF 2019

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Potential physics in current and future phases

September 11, 2019 TAUP 2019 - Toyama, Japan 27

Baseline WATCHMAN will be a valuable trigger for supernova neutrinos, providing input to

  • SNEWS. Roughly 4,000 total

events are expected for a SN located 10,000 light years away.

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SLIDE 29

Potential physics in current and future phases

September 11, 2019 TAUP 2019 - Toyama, Japan 28

Baseline WATCHMAN will be a valuable trigger for supernova neutrinos, providing input to

  • SNEWS. Roughly 4,000 total

events are expected for a SN located 10,000 light years away.

WATCHMAN

Could the addition of WbLS, with greatly improved energy resolution, yield interesting oscillation physics? Investigations are currently underway…

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SLIDE 30

AIT-WATCHMAN Collaboration

September 11, 2019 TAUP 2019 - Toyama, Japan 29

20 Institutions and 96 Collaborators from the US and UK

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SLIDE 31

Backup

September 11, 2019 TAUP 2019 - Toyama, Japan 30