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Radiation Safety Considerations of C100 Cryomodule Operation

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Presentation on theme: "Radiation Safety Considerations of C100 Cryomodule Operation"— Presentation transcript:

1 Radiation Safety Considerations of C100 Cryomodule Operation
P. Degtiarenko, J. Jefferson, M. Keller, G. Kharashvili, V. Vylet, K. Welch, M. Washington Radiation Control Department Jefferson Lab Title Page

2 electron field emission
C100 – field emitted electrons may accelerate to energies well above photonuclear reaction thresholds Prompt photon and neutron fields – problem at cryomodule test facilities; Material activation – planning accelerator maintenance, possible relocation of parts, decommissioning; Radiation damage to nearby electronics and materials. Sourceterm difficult to characterize; May vary with time; Challenging to simultaneously model all physical processes involved. Interior Page Design 1 CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

3 electron field emission
Low energy electrons below photonuclear reaction thresholds Electrons capable of accelerating up to the full gradient Iris Electromagnetic cascade ҉ Interior Page Design 1 High energy cascade develops at the end flange at the cryomodule step-down. CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

4 C100s at Jefferson Lab Radiation surveys; Prompt radiation monitoring;
Correlating accelerating gradients and prompt radiation fields; Gamma spectroscopy analysis of activated components Portable HPGe detector GENIE-2000 ISOCSTM Interior Page Design 1 CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

5 Prompt radiation - SL24 & SL25
108 107 106 105 104 103 102 10 1 10-1 10-2 (μSv / h ) (mGy / h ) 10-3 10-4 10-5 Interior Page Design 1 CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

6 Gamma spectroscopy analysis
Nuclide T1/2 (day) Na-24 0.62 Ni-57 1.48 Sc-47 3.35 Mn-52 5.59 Ni-56 6.08 NB-92m 10.2 V-48 16 CR-51 27.7 Fe-59 44.5 CO-58 70.9 CO-56 77.3 Sc-46 83.8 ZN-65 244.3 CO-57 271.8 MN-54 312.3 NA-22 803.6 CO-60 1924.9 Interior Page Design 1 Pulse height spectrum– 2m from beamline between NL25-NL26 CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

7 NL25 accelerating gradients
Data missing NL25 Total Gradient 2.3 GeV push radcon test NL25 Individual Cavity Gradients Interior Page Design 1 CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

8 SL24 accelerating gradients
Data missing SL24 Total Gradient 2.3 GeV push radcon test SL24 Individual Cavity Gradients Interior Page Design 1 CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

9 Activation rates Assuming that all radioactivity was produced during the first 5 days of February 2014 – push for 2.3 GeV – radionuclide production rates were calculated. Expected levels of radioactivity and subsequent dose equivalent rates are then projected for 3-month, 1-year, and 5-year long runs. Interior Page Design 1 CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

10 NL25 forecast Interior Page Design 1
CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

11 SL24 forecast Interior Page Design 1
CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

12 Conclusions High radiation areas are expected near C100s for hours after each typical high gradient run, but not above 1R/h requiring physical barriers. Radiation areas are likely to persist for longer periods of time – for weeks or months. Radiological controls in CEBAF tunnel will have to change accordingly. Prompt neutron field measurements can be used to minimize activation. Further studies: Continue surveying the areas; Gamma spectroscopy during accelerator downs; Investigate neutron monitoring options. Interior Page Design 1 CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

13 Conclusions Besides activation, neutron measurements may be useful for a number of operational issues Heat Vacuum Radiation damage Neutron monitoring can be used as an additional tool in optimizing cryomodule performance. Interior Page Design 1 CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

14 acknowledgements Thanks to the members of the Field Operations Group of Radiation Control Department, Accelerator Operations Department, and Institute for SRF Science and Technology for their contributions. This work was supported by the U.S. Department of Energy under contract number DE-AC05-06OR23177s Interior Page Design 1 CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab

15 references P. Degtiarenko, M. Keller, G. Kharashvili, V. Vylet, K. Welch , “Radiation Safety Consideration of C100 Cryomodule Operation at Jefferson Lab”, JLAB-TN , Newport News, 2012. M. Silari, S. Agosteo, J.-C. Gaborit and L. Ulrici, "Radiation produces by the LEP superconducting RF cavities," Nuclear Instruments and Methods in Physics Research A, vol. 432, pp. 1-13, 1999. R. J. Hernandez Pinto, M. Otto and M. Valentan, "Radiation Measurements in the FLASH Tunnel," DESY Technical Note , Hamburg, Germany, 2006. K. Welch, V. Vylet and B. May, "Lessons Learned: SRF Testing and Activated Components," Accelerator Safety Workshop, Argon National Lab, 2011. F. Marhauser, "Field Emission and Consequences as Observed and Simulated for CEBAF Upgrade Cryomodules," MuPlus Inc. and Jefferson Lab, JLAB-TN , Newport News, 2012. C. Ginsburg and I. Rakhno, "Shielding studies for superconducting RF cavities at Fermilab," in Shielding Aspects of Accelerators, Targets and Irradiation Facilities (SATIF), Geneva, Switzerland, 2010. C. Ginsburg and I. Rakhno, "Optimization Studies for Radiation Shielding of a Seperconducting RF Cavity test Facility," in International Particle Accelerator Conference (IPAC), Kyoto, Japan, 2010. E. Donoghue, G. Wu, J. Mammosser, R. Rimmer, M. Stribet, L. Phillips and H. Wang, "STUDIES OF ELECTRON ACTIVITIES IN SNS-TYPE SUPERCONDUCTING RF CAVITIES," in The 12th International Workshop on RF Superconductivity, Ithaca, New York, 2005. Interior Page Design 1 CEBAF SRF/RF/CRYO Workshop, 3 April 2014, Jefferson Lab


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