Summary HiLuMI LHC Collimation Materials Irradiation Damage Study at BNL EuCARD N. Simos Effort consists of: IRRADIATION o 200 MeV proton irradiation at.

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Presentation transcript:

Summary HiLuMI LHC Collimation Materials Irradiation Damage Study at BNL EuCARD N. Simos Effort consists of: IRRADIATION o 200 MeV proton irradiation at BNL Linear Isotope Producer (BLIP) of 4 candidate materials (Molybdenum, Glidcop, Mo-Graphite and Cu-CD (copper-diamond). Irradiation parameters: 8-weeks at 110 uA o Neutron irradiation of Cu-CD from 118 MeV protons o 28-MeV proton irradiation of Mo (including spallation neutron irradiation of Mo, Glidcop, Cu-CD and Mo-GR) PIE X-ray diffraction studies at NSLS X17B1/X17A beamlines (completed) X-ray diffraction studies at NSLS II XPD beamline (proposed) Comprehensive macroscopic analysis at BNL Isotope extraction facility (initiated) Spectral Analysis (initiated) Nano- micro-structural characterization at Center of Functional Nanomaterials (initiated) 1

Irradiated LHC HiLuMi Collimation materials Preliminary Assessment: 200 MeV heavily bombarded LHC array is still in cool-down mode due to extremely high dose levels. One of the two Molybdenum (Mo) capsules has been opened for visual examination. Mo samples appear to be fully intact. In coming weeks the proton irradiated array will be opened and examined (followed by transport to the PIE hot cells for sorting and studies) Neutron irradiated Cu-CD has seen no structural degradation 28 MeV protons and spallation neutrons at Tandem have not affected the structural integrity of the LHC HiLuMI array 2

200 MeV Proton Irradiation 3

Spallation Neutron Irradiation - Cu-CD Neutron spectrum downstream of isotope target array 4

28 MeV Proton (plus spallation neutron) irradiation at Tandem Mo – direct 28 MeV protons Mo/MoGR/CuCD/Glidcop: spallation neutrons 28 MeV ( 1 uA, 200 x 200 um x um ) protons 5

X17A (monochromatic x-rays) X-Ray ring (3 GeV) X17B1 X-ray diffraction studies at NSLS -Monochromatic 70 KeV beam (X17A beamline) -White beam 200 KeV, X17B1 beamline Mo-GR Glidcop (SLAC LHC rotating collim) Glidcop (HiLuMI) 6

incident collimation system Transmission detector (radiography) Ge-Detector specimen Diffraction volume 22 kk “White Beam” STRAIN MAPPING Energy Dispersive Diffraction Mode 1m diff. coll.  y X-17B o ~ Like having imbedded inter-atomic strain gauges !!!!  m 7

From concept to a versatile experimental stage at X17B1 beamline at NSLS Multi-functional stage capable of handling Real size irradiated specimens, under vacuum and four point bending state of stress and eventually Heating/annealing via a portable, collimated laser beam Tensile stress-strain test 8

stress strain 9

EXCELLENT matching with the experimental data at X17B1 using x-rays and loading to assess the displacement. Load 1 Load 2 GOAL: LATTICE strain and global strain are very different in magnitude 10

STATE of PIE 8-week proton Irradiation at BLIP Target Capsules (still extremely hot) were transported to the Hot Cell Facility for opening and sorting; Capsules opened so far: Two proton irradiated Mo Proton irradiated Glidcop Proton Irradiated Cu-CD Low-dose proton irradiated Mo-GR Neutron irradiated Cu-CD 11

Status of HiLuMI LHC Irradiation Damage Studies at BNL BLIP  200 MeV proton irradiation (8 weeks): COMPLETED  Neutron irradiation from 112 MeV protons COMPLETED  Cooling of highly radioactive samples in Hot Cell Lab 66: ON-GOING TANDEM VAN DER GRAAF  28 MeV proton irradiation: COMPLETED X-ray Diffraction Experiments at NSLS  X-Ray diffraction studies for phase and strain mapping of some cold and irradiated samples: COMPLETED (to be continued in NSLS II in late 2015)  Data analysis: ON-GOING X-ray Diffraction Experiments at NSLS II (XPD Beamline)  Beamtime proposal preparation at XPD (due Feb. 2, 2015) CFN (BNL Center of Functional Nanomaterials)  Annealing and Electron Microscopy analysis: NOT STARTED (foreseen for beginning 2015) IEF (BNL Isotope Extraction Facility)  Activity and dose measurements per sample: COMPLETED  γ-spectra for selected samples: PARTIALLY COMPLETED 12

Mo #1 Mo #2 13

Mo-GR Irradiated with 200 MeV protons full beam for 2 hours at BLIP before it was removed from beam due to overheating and closing the cooling channel Shows signs of distress even with minimum beam 14

Mo X-ray Diffraction Studies (preliminary) 15

16

X-ray Diffraction of Mo Irradiated with 28 MeV focused PROTON beam at TANDEM 17

Cu_CD_unirrad Cu_CD_Irradiated with FAST neutrons at BLIP 18

Mo-GR_unirrad Mo-GR: Irradiated with modest FLUENCE of protons at BLIP Mo-GR: Irradiated with modest FLUENCE of neutrons at TANDEM 19

Mo-Gr (unirradiated) Mo-Gr (irradiated at Tandem with neutron flux) 20

21 Graphite Mo-Gr Irradiated at BLIP with 200 MeV Protons and very modest fluence Scanning across the irradiated zone

SUMMARY An extensive PIE (both macroscopic at the BNL Hot Cells and Microscopic using X-rays at the new Synchrotron and the XPD beamline and CFN for unirradiated materials studies) The large volume of experimental data to-date from the different irradiations and X-ray diffraction as well as baseline studies will continue to be analyzed THE CRUCIAL steps are those associated with the HEAVILY IRRADIATED array of Mo, Mo- Gr, Cu-CD and Glidcop at BLIP Complete opening all capsules and sort all of them Conduct all the macroscopic studies (including photon spectra) Anticipate cool-down below levels that they can be studied at the XPD beamline of NSLS II (proposal under preparation) ASSESS what materials from array should be looked further and which should not 22

PRELIMINARY ASSESSMENT on LHC Collimator Materials of PHASE I 2-D Carbon/Carbon Composites Graphite Glidcop PARENTHESIS 23

Glidcop – Irradiated with 200 MeV protons Irradiated 24 Unirradiated

25

Effects of Proton irradiation (180 MeV) on graphite and C/C composite X-ray diffraction studies at NSLS Unirradiated GRAPHITE irradiated GRAPHITE 26

Effects of Proton irradiation (180 MeV) on graphite and LHC C/C composite 27

Global volumetric changes vs. crystal-level changes Activation Energy 28

Irradiation and Thermal “anomalies” of Tungsten – Possible Similarities to Mo 29