Measurements of Radiation Doses Induced by High Intensity Laser between and W/cm 2 onto Solid Targets in LCLS MEC Instrument

Transcription

1 Measurements of Radiation Doses Induced by High Intensity Laser between and W/cm 2 onto Solid Targets in LCLS MEC Instrument SLAC RP: Johannes Bauer, Maranda Cimeno, James Liu, Sayed Rokni, Henry Tran, Mike Woods Ted Liang Georgia Tech/SLAC Anna Ferrari Helmholtz-Zentrum Dresden SLAC LCLS: Eric Galtier, Eduardo Granados, Phil Heimann, Hae Ja Lee, D. Milathianaki, Bob Nagler, Alyssa Prinz SLAC National Accelerator Laboratory (SLAC), California, USA RadSynch, June 3-5, 2015

2 Outline SLAC MEC FEL and Laser Facility Electron and Photon Source Terms and SLAC-RP Photon Dose Yield Model Measurements ( ) o Set-up of active and passive detectors o Characterization of Laser-optic-target parameters o Measured dose results o Comparison with RP model o Preliminary electron spectrometry and FLUKA and PIC code results Summary 2

3 LCLS Facility and MEC FEL Instrument Matter in Extreme Conditions (MEC) instrument combines the unique LCLS FEL beam with high power optical laser beam to study the transient behavior of matter in extreme conditions. Roll-up door (Steel) Hutch wall (Pb) Target chamber (Al) FEL beam Short pulse laser (40 fs, 8 J, f3 1x10 21 W/cm 2 ) Long pulse laser (2-20 ns, 50 J) MEC serves key scientific areas including Warm Dense Matter physics, High Pressure studies, shock physics, and High Energy Density physics. 3

4 Ionizing Radiation from High Intensity Laser on Target Laser Plasma Target H.A. Baldis, et al., Handbook of Plasma Physics,(1991). e - e - hadrons X ray 1 J, 40 fs, 10 µm 1/e 2 radius, I = 1.6x10 19 W/cm 2 SLAC RP Note

5 Hot Electron Temperature T h Ponderomotive theory Meyerhofer 1993 Hui Chen 2009 MEC λ = 0.8 µm I (W/cm 2 ) T h (MeV) T (kev) x x x Iλ (W / cm µ m ) SLAC RP Note

6 Bremsstrahlung Dose Yield and Spectrum X-ray Dose Yield (Sv/J) at 1 m and 0-degree: P ef - laser energy to hot electron energy conversion efficiency (30% for I 1x10 19 W/cm 2 and 50% for I > 1x10 19 W/cm 2 ) T h - hot electron temperature in MeV R - distance from target to dose point in cm X-ray Maxwellian Spectrum for Shielding Design: N p ( E p ) = C 1 E E exp( T E p - photon energy in kev T - electron temperature in kev C - normalization constant p p ) SLAC RP Note

7 Original and Adjusted RP Photon Dose Yield Models and Maximal Doses Measured 1,0E+01 Photon Dose yield (msv/j at 1 m) 1,0E+00 1,0E-01 1,0E-02 1,0E-03 1,0E-04 1,0E-05 1,0E-06 RP model (5mm glass) RP model (2.54cm Al) Adjusted RP (2.54cm Al) MEC Sep-2014 (Al,Cu,Au,CH3) MEC Aug-2014 (Cu,Ni) MEC Jul-2014 (Cu,nanowire) MEC Feb-2014 (Cu) MEC Mar-2012 (Au,Cu) LLNL Titan 2011 (Au,foam) 1,0E-07 1,0E+16 1,0E+17 1,0E+18 1,0E+19 1,0E+20 1,0E+21 Intensity (W/cm 2 ) 7

8 Measurements at LLNL Titan and SLAC MEC 2011 at Titan (RP-11-11) : 1x10 20 to 6x10 20 W/cm J Single shots CH foam with Au foil backing 2012 at MEC (SLAC-PUB ): 3x10 16 to 6x10 17 W/cm mj per pulse 10 Hz 10 & 100 µm Au, 1 mm Cu Inside Target Chamber 8

9 Measurements around MEC Target Chamber Ion Chamber photon detectors: Victoreen 450/451, PTW, HPI SLAC-made moderated BF 3 neutron detectors Passive dosimeters (RADOS, PIC, TLD and OSLD) inside blue boxes 10

10 Target and Dosimeters inside MEC Target Chamber Gold foil target in center from Landauer Al 2 O 3 Landauer nanodot OSLD ~30 cm from target 11

11 MEC Laser Shot Rastering by Moving Solid Target Gold foils after shots 100 µm & 10 µm Au foils 100 µm Cu plates 15 µm Ni nanowire 12

12 MEC Laser-Optic-Target Characterization (1 J, 25 TW) Feb July 2014 August 2014 Sept Intensity (W/cm 2 ) 2 x x x x Main peak energy on target (J) Pulse length (fs) /e 2 radius HxV (μm) 13 x 8 37 x x 9 3 x 2 Target 100 μm Cu 5 & 100 μm Cu 15 μm Ni nanowire Feb. 2014: Bimodal peaks 100 μm Cu 15 μm Ni nanowire 10 & 15 μm Al 5 μm Au and Cu 2.5 & 5 μm CH 3 August 2014: Gaussian peak SLAC PUB RP RP Spot size (m) Intensity (W/m 2 ) 9

13 Photon Dose Rate Measurements PTW ion chamber HPI 6032 ion chamber 6x10 17 W/cm 2, 30 mj 10 Hz 1 mm Cu 100 µm Au 13

14 Passive and Active Detector Performance at LLNL 2011 at Titan (RP-11-11): 1x10 20 to 6x10 20 W/cm J Single shots CH foam with Au foil backing Active detectors, e.g., Victoreen 450 meters, affected by EMP (from laser and/or plasma)! TLD agreed with OSLD 1000 PIC agreed with TLD/OSLD Panasonic dose readtout (mrem) Panasonic versus Luxel Passive dosimeters and Victoreen readout (mrem) Luxel+ versus PIC Panasonic versus PIC Victoreen versus PIC PIC dose readout(mr) Luxel+ dose readout (mrem) 15

15 Complete Measurement Data for W/cm 2 with Adjusted RP Dose Yield Model Original RP model was adjusted based on measurements (account partly for electron angular distribution) Measurement is still 1/10 of adjusted RP model at W/cm 2 and 1/3 at W/cm 2 (due to electron spectrum model) Adjusted RP model used for shielding design 16

16 Neutron Doses 1,0E-03 Dose yield at 1 m (msv/j) 1,0E-04 1,0E-05 1,0E-06 1,0E-07 LULI 2002 MEC Jul Aug Feb Sep-14 1x10 18 W/cm 2 1,0E-08 1,0E+17 1,0E+18 1,0E+19 1,0E+20 Intensity (W/cm 2 ) 1x10 19 W/cm 2 Correlation between neutron and photon Nearly isotropic angular distribution 17

17 Dose Comparison between FLUKA and Measurements nanodot shallow dose 18

18 Current Work Refine hot electron source term Current Model Laser to hot electron conversion 30% or 50% Hot electron energy distribution Hot electron angular distribution Maxwellian and Rel. Maxwellian Mono-directional Refined Model Lower for < W/cm 2? Emitted in 4π, Not Isotropic Refine photon dose yield model Refine shielding attenuation By comparing electron spectrometry results with FLUKA simulation and PIC calculations 19

19 10 19 W/cm 2, T h = 0.70 MeV 100 µm Cu foil (0.7 J, 340 shots on target) FLUKA simulation with T h = 0.70 MeV shows Maxwellian spectrum agrees better with measured depth-dose curves 20

20 Electron Spectrum Shape and T h from PIC Calculations W/cm 2 Maxwellian Ponderomotive formula gives T h = 0.70 MeV Ponderomotive formula gives T h = 2.4 MeV PIC (particle-in-cell) is a multi-dimensional, fully electromagnetic, relativistic code that simulates higher energy density physics such as the generation of plasma from a high intensity laser interacting with matter. 21

21 Shielding Tenth Value Layer (TVL) FLUKA calculations with Maxwellian photon spectrum Approaching equilibrium TVL at high intensities 22

22 Summary Systematic and comprehensive measurements performed for laser focused onto solid targets between 3x10 16 to 6x10 20 W/cm 2 Various types of active and passive dosimeters Characterization of laser and optic parameters Photon doses detected starting at 3x10 16 W/cm 2 Low neutron doses detected starting at 6x10 17 W/cm 2 High doses from low-energy electrons inside chamber RP photon dose model adjusted to be reasonably conservative based on measurements (still overestimates by x10 at W/cm 2 ) Hazard analysis and controls, including shielding and interlocked system, for MEC user experiments and future PW facility Work on electron source terms with PIC/FLUKA and photon TVLs with FLUKA 23

23 Thank You!

24 Maximum Photon Dose Rates from Victoreen 451 1x10 19 W/cm 2, 0.7 J 50 fs, 1 Hz more photons pass through thinner Al flanges 14