Requirements on Neutron Detectors Alternative to He-3 · PDF fileRequirements on Neutron Detectors Alternative to He-3 Fraunhofer ... Fraunhofer Institute for Technological Trend

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  • Fraunhofer INT

    Nuclear and Electromagnetic Effects

    Wolfgang Rosenstock and Olaf Schumann

    Requirements on Neutron Detectors Alternative to He-3

    Fraunhofer INT, Euskirchen, Germany Department Nuclear and Electromagnetic Effects

    [email protected]

    Neutron Detector Technologies Workshop in Vienna (22 24 March 2011)

    IAEA short term needs for existing installed SG instrumentation

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Outline

    Fraunhofer INT (spheres of work)

    Irradiation Facilities at INT

    Earlier work performed for IAEA: Qualification of 3He detectors

    Concepts for 3He replacement: advantages and drawbacks

    Conclusion

    nrd 11-10

    Dr. Wolfgang Rosenstock

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    100 Staff (75 Man Years)including

    45 Scientists

    Budget ~7.2 Mio including~3,2 Mio Contract Research

    Fraunhofer Institute for Technological Trend Analysis INT(Fraunhofer Institut fr naturwissenschaftlich-technische Trendanalysen)

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    The Business Areas of INT

    Electromagnetic Effects and Threats

    Nuclear Effects, Threats and Detection Systems

    Trends and Developments in Research and Technology

    Planning, Programs and Structures in R&T

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    NEMP - Origin and Propagation; Modeling and SimulationEffects of Pulsed High Power Microwaves (HPM)EMC, HPM and NEMP MeasurementManagement of Simulation and Measurement Equipment for Electromagnetic Fields

    Electromagnetic Effects and Threats

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Nuclear Effects, Threats and Detection Systems

    Nuclear Security Policy and Detection Techniquesassessment of physical and technological aspects of nuclear threat and security Nuclear Radiation Detection and Identification in the Field

    Nuclear Radiation Effects in Electronics and OptoelectronicsRadiation Effects in Fiber Optic and Electronic Systems

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Analysis of the Effects of Ionizing Radiation on Electronic and Optical Components, esp. on Fiber Optic Systems

    Management of irradiation facilities for Gamma, Electron, Proton and Neutron Radiation

    Qualification of Components and Systems

    Identification of Radiation Hard Products

    Development of New Sensors for Nuclear Radiation

    Advice to Producers and Users of Fiber Optic Systems (Space, High Energy Accelerators, Nuclear Technology Environments and Medicine).

    Highlight Nuclear Radiation Effects in Electronics and Optoelectronics

    Nuclear Effects, Threats and Detection Systems

    Gamma-Irradiation Facility TK 1000

    X-ray flash machineFebetron 705

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Nuclear Security Policy, non-proliferation and arms control, Safeguards

    Non-destructive detection and verification of radioactive material as well as fissile material (appropriate for nuclear weapons) on site (surveying cabin NANU)

    Measuring car DeGeN Detection of Gammas inclusive Neutrons, search and identification of radioactive and nuclear material

    Systems for verification of radioactive and nuclear material, including active interrogation with neutrons by a portable neutron generator and development of mobile neutron radiography

    Mobile measuring systems for non-destructive and non-contact detection as well as identification of radioactive or special nuclear material on site.

    Highlight Nuclear Security Policy and Detection Techniques

    Nuclear Effects, Threats and Detection Systems

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Available irradiation facilities at INT

    several intense Co-60 sources up to 19 TBq ( 4.5 Gy/h in 1 m)

    several neutron generators

    Thermo D-711 (DD & DT)

    Sodern Genie 16C (DD & DT)

    Flash X-Ray and Electron Febetron 705

    Large variety of isotopic sources

    Th-228 , U-238, Am-241, Cm-244

    H-3, C-14, Cl-36, Sr-90, Pm-147, Tl-204

    Na-22, Mn-54, Co-60, Ba-133, Cs-137, Eu-152+Eu-154+Eu-155

    Cf-252, Am/Be, Am/Li

    nrd 11-11

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Qualification of 3He-tubes RS-P4-0812-115and RS-P4-0808-212

    Performed under the German Support Program (GSP)

    Joint Program on the Technical Development and Further Improvement of IAEA Safeguards

    Determination of an Optimized Polyethylene Moderator for He-3 Neutron Detectors

    RS-P4-0812-115 401.3mm x 26.2mm dia Body: aluminum 1100-F 4.2 bar He-3 1500 V HV Surrounded with 50 mm PE

    RS-P4-0808-212 303.0mm x 26.2mm dia Body: stainless steel 304 4.1 bar He-3 1750 V HV Surrounded with 50 mm PE

    nrd 11-12

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Experimental Setup: Evaluation of Gamma Sensitivity

    60Co Source

    He-3 Detectorwith PE moderator

    Co-60 source

    Activity: 17.2 TBq

    Different distances to vary flux

    Cf-252

    Activity: 1.4 MBq

    Emission: 1.5 105 n/s in 4Placed 1.3 m from He-3 tube

    Flux: 0.75 n/(cm2 s)

    PNPI Electronics

    Preamplifier, shaping amplifier and threshold

    Threshold from 0 to 1.2 V

    nrd 11-13

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Neutron Pulse Hight Spectrum of He-3 Tube

    0

    20

    40

    60

    80

    100

    120

    0 200 400 600 800 1000 1200 1400 1600

    Pulse Height [Channel No.]

    Cou

    nts

    / 300

    s

    n + 3He 3H + p + 764 keV

    Full energydeposited byionisation

    3H energy lost in tube wall,only p seen

    nrd 11-14

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Comparison of Neutron / Gamma only spectrum

    1

    10

    100

    1000

    10000

    100000

    0 100 200 300 400 500 600 700 800

    Pulse Height [Channel No.]

    Cou

    nts

    / 100

    s

    Gamma, 0.7 Gy/h

    Neutrons

    Channels overlapDiscrimination bythreshold

    nrd 11-15

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Combined Neutron / Gamma spectra

    1

    10

    100

    1000

    10000

    100000

    0 100 200 300 400 500 600 700 800

    Pulse Height [Channel No.]

    Cou

    nts

    / 100

    s

    n

    Neutron + Gamma

    Pile-up due tosimultaneous n+

    Channels overlap,Discrimination bythreshold

    nrd 11-16

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Effect of amplifier threshold

    1

    10

    100

    1000

    10000

    100000

    1000000

    0 100 200 300 400 500 600 700 800

    Pulse Height [Channel No.]

    Cou

    nts

    / 300

    s

    No threshold

    500 mV800 mV

    Gammas could besuppressed bythreshold value

    Reduces absolutefficiency for n

    nrd 11-17

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    High Gamma dose rate

    At 5.77 Gy/h (former slides 0.7 Gy/h) Gammas clearly dominate

    1

    10

    100

    1000

    10000

    0 100 200 300 400 500 600 700 800 900

    Pulse Height [Channel No.]

    Cou

    nts

    / 300

    s

    Neutrons

    Gamma +Neutrons(red)

    No morediscriminationpossible

    nrd 11-18

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Efficiency vs. Threshold

    0

    10

    20

    30

    40

    50

    60

    70

    80

    90

    100

    110

    0 200 400 600 800 1000 1200

    Discriminator Threshold [mV]

    Rel

    ativ

    e N

    eutr

    on C

    ount

    ing

    Effic

    ienc

    y [%

    ]

    0.3 Gy/h0.7 Gy/h1.29 Gy/h5.77 Gy/h

    Gamma Dose Rate

    Up to a Gammadose rate of 1.3 Gy/hcompleteneutron/gammadiscrimination possible

    }{}{}{

    ++

    =n

    nEff

    nrd 11-19

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Influence of neutron flux and neutron energy

    50

    60

    70

    80

    90

    100

    110

    0 200 400 600 800 1000 1200

    Discriminator Threshold [mV]

    Rel

    ativ

    e N

    eutro

    n C

    ount

    ing

    Effic

    ienc

    y [%

    ]

    Cf-252

    Am-Be

    Gamma Dose Rate: 0.7 Gy/h

    Am/Be source with 106.6 GBqFlux: 29.7 n/cm2 s40 times the flux of Cf-252

    Above threshold of ~ 700 mV no change in discrimination

    0

    50

    100

    150

    200

    250

    300

    350

    400

    0 200 400 600 800 1000 1200 1400 1600

    Pulse Height [Channel No.]

    Cou

    nts

    / 100

    s

    Neutron flux39 n/cm2s

    Neutron flux280 n/cm2s

    14 MeV DT neutrons, no additional GammaFlux: 39 and 280 n/cm2s

    Large pile-up effects

    Pile-up

    nrd 11-20

  • Fraunhofer INT

    Nuclear and Electromagnetic Effects Dr. Wolfgang Rosenstock

    Summary of performed experimentsGamma and Neutron irradiation of IAEA employed He-3 counters and electronic

    Determination of relative and absolute ef