Demonstrating Capability for Radiochemical Analysis of Gaseous Samples at NIF

Similar documents
Charles Cerjan. Nuclear Data Needs and Capabilities for Applications. Lawrence Berkeley National Laboratory. May 28, 2015

Experimental Initiatives in Nuclear Astrophysics

Nuclear astrophysics studies with charged particles in hot plasma environments

Role of radioactive beams in stockpile stewardship science

Fukuoka, Japan. 23 August National Ignition Facility (NIF) Laboratory for Laser Energetics (OPERA)

Measuring Neutron Capture Cross Sections on s-process Radioactive Nuclei

Nuclear-Plasma Interactions on highly excited states Workshop on Level Densities and Gamma Strength University of Oslo Oslo, Norway

The MIT Accelerator for development of ICF diagnostics at OMEGA / OMEGA-EP and the NIF

Hydrodynamic instability measurements in DTlayered ICF capsules using the layered-hgr platform

Lecture 22 Ion Beam Techniques

RADIOACTIVITY: spontaneous disintegration of the nucleus of certain atoms accompanied by the emission (release) of particles and/or energy

Nuclear Physics Questions. 1. What particles make up the nucleus? What is the general term for them? What are those particles composed of?

Nuclear Physics Opportunities at OMEGA and the NIF

Diagnosing OMEGA and NIF Implosions Using the D 3 He Spectrum Line Width

High energy density nuclear physics at UC Berkeley, LLNL, and LBNL. Karl van Bibber & Lee Bernstein

The National Ignition Facility: Transition to a User Facility

Measurements of the Deuterium-Tritium Branching Ratio Using ICF Implosions

Review Package #3 Atomic Models and Subatomic Particles The Periodic Table Chemical Bonding

Cleaning Electronegative Contamination from Gaseous Xenon Through Cryogenic Pumping

Chemistry: A Molecular Approach, 2e (Tro) Chapter 2 Atoms and Elements. Multiple Choice Questions

Recent results of (n,xγ) reaction measurements using GRH at NIF

1. The arrangement of the elements from left to right in Period 4 on the Periodic Table is based on

Principles of Chemistry: A Molecular Approach 2e (Tro) Chapter 2 Atoms and Elements

Unit 1 Test A Atomic Theory & Nuclear Decay 1. Which of these BEST describes any two atoms of the same element? a. same number of protons

The Ignition Physics Campaign on NIF: Status and Progress

EBSS: Hands-on Activity #8. Operation of an electromagnetic isotope separator (EMIS) Dan Stracener Jon Batchelder

Regents Chemistry PRACTICE PACKET. Unit 2: Atomic Theory

Activity # 2. Name. Date due. Assignment on Atomic Structure

Distinguishing fissions of 232 Th, 237 Np and 238 U with beta-delayed gamma rays

The Magnetic Recoil Spectrometer (MRSt) for time-resolved measurements of the neutron spectrum at the National Ignition Facility (NIF)

Relative Sensitivity RS Measurements of Gases

In the investigation, a pressure on the order of 10-6

Chapter 2 Atoms and the Periodic Table

Modern Atomic Theory

This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under contract

Atoms and the Periodic Table

D) g. 2. In which pair do the particles have approximately the same mass?

ICStatus and progress of the National Ignition Facility as ICF and HED user facility

Radioactivity is the spontaneous disintegration of nuclei. The first radioactive. elements discovered were the heavy atoms thorium and uranium.

Laser Spectroscopy on Bunched Radioactive Ion Beams

NJCTL.org 2015 AP Physics 2 Nuclear Physics

Part A Unit-based exercise

NSS Chemistry Part 2 The Microscopic World I HKCEE Past Paper Questions Structural Questions

Principles of Chemistry: A Molecular Approach, 3e (Tro) Chapter 2 Atoms and Elements

UNIT 10 RADIOACTIVITY AND NUCLEAR CHEMISTRY

International Nuclear Physics Conference Adelaide, Australia September 13, 2016

Aluminum Half-Life Experiment

Chemistry Released Questions

LARGE UNDERGROUND XENON

Wednesday, September 16, The Periodic Table

BEAM PROPAGATION FOR THE LASER INERTIAL CONFINEMENT FUSION-FISSION ENERGY ENGINE. S. C. Wilks, B. I. Cohen, J. F. Latkowski, and E. A.

CHAPTER 6. Chemical Periodicity

Measurements of the Prompt Fission Neutron Spectrum at LANSCE: The Chi-Nu Experiment

Developing the Periodic Table

There are 7 trends on the periodic table that we will follow. Using your periodic table, answer all of the questions in the packet. Think hard.

THE BIG IDEA: ELECTRONS AND THE STRUCTURE OF ATOMS. BONDING AND INTERACTIONS.

Nuclear Science and Engineering Institute, University of Missouri, USA and Sidney Kimmel Institute for the Nuclear Renaissance

Note that the protons and neutrons are each almost 2,000 times more massive than an electron; What is the approximate diameter of an atom?

[2] State in what form the energy is released in such a reaction.... [1]

A. They are noble (inert) gases. B. They are nonmetals. C. They have the same thermal conductivity. D. They have the same number of protons.

Noble Gas Mass Spectrometer

Teacher Workbooks. Science and Nature Series. Atomic Structure, Electron Configuration, Classifying Matter and Nuclear Chemistry, Vol.

Supervised assessment: Ionising radiation

Inertial Confinement Fusion DR KATE LANCASTER YORK PLASMA INSTITUTE

Biotech 2: Atoms and Molecules OS Text Reading pp Electron cloud Atoms & Nucleus 2e Subatomic Particles Helium Electron cloud

Science 10. Unit 4:Physics. Block: Name: Book 3: radioactivty

Chapter 2. The Chemical Context of Life

CALIBRATION OF SCINTILLATION DETECTORS USING A DT GENERATOR Jarrod D. Edwards, Sara A. Pozzi, and John T. Mihalczo

Chem 1A Chapter 5 and 21 Practice Test Grosser ( )

29th Monitoring Research Review: Ground-Based Nuclear Explosion Monitoring Technologies AUTOMATED QA/QC CHECK

Principles of Chemistry: A Molecular Approach (Tro) Chapter 2 Atoms and Elements

Budget Uncertainty and Minimum Detectable Concentrations for the INAA Laboratory of the ETRR-2

anti-compton BGO detector

Am cross section measurements at GELINA. S. Kopecky EC JRC IRMM Standards for Nuclear Safety, Security and Safeguards (SN3S)

Atomic Notation (or Nuclear Symbol): Shorthand for keeping track of protons and neutrons in the nucleus

Science 10- Course Review Unit 1-Chemistry

Nuclear Decays. Alpha Decay

Method for Detection of Nuclear-Plasma Interactions in a 134 Xe-Doped Exploding Pusher at the National Ignition Facility )

Chemistry 1 1. Review Package #3. Atomic Models and Subatomic Particles The Periodic Table Chemical Bonding

Hydrodynamic growth experiments with the 3-D, native-roughness modulations on NIF

Quadrupole Mass Spectrometry Concepts. Mass spectrometers for residual gas analysis: Intermediate Level Users Guide

The Pursuit of Indirect Drive Ignition at the National Ignition Facility

Isotopes Atoms of an element (same # p+) that differ in their number of neutrons

A new scintillator detector for nuclear physics experiments: the CLYC scintillator

High precision neutron inelastic cross section measurements

Number of protons. 2. What is the nuclear symbol for a radioactive isotope of copper with a mass number of 60? A) Cu

Objectives: Atomic Structure: The Basics

HSVD Ms. Chang Page 1

FTF Day 9. April 9, 2012 HW: Assessment Questions 13.1 (Wed) Folder Check Quiz on Wednesday Topic: Gas laws Question: What are gasses like?

ION Pumps for UHV Systems, Synchrotrons & Particle Accelerators. Mauro Audi, Academic, Government & Research Marketing Manager

Application of prompt gamma activation analysis with neutron beams for the detection and analysis of nuclear materials in containers

09. CLASSIFICATION OF ELEMENTS THE PERIODIC TABLE

Full file at

Observations. Qualitative: descriptive observation that is not numerical. Quantitative: Numerical observation.

Seaborg s Plutonium?

Fission-Fusion Neutron Source

GASEOUS AND VOLATILE FISSION PRODUCT RELEASE FROM MOLTEN SALT NUCLEAR FUEL

ICF ignition and the Lawson criterion

2. Atoms with nearly empty valence shells give up electrons. They are called

Concept 2.1: Matter consists of chemical elements in pure form and in combinations called compounds

Transcription:

Demonstrating Capability for Radiochemical Analysis of Gaseous Samples at NIF Carol Velsko, William Cassata, Don Jedlovec, Evgeny Tereshatov, Wolfgang Stoeffl, Charles Yeamans, Dawn Shaughnessy This work was performed under the auspices of the U.S. Department of Energy by under Contract DE-AC52-07NA27344. Lawrence Livermore National Security, LLC

Outline Radiochemical Analysis of Gaseous Samples (RAGS) Description Results from participation on NIF shots RAGS performance Future Plans 2

RAGS has equipment on many levels of NIF Target Bay RAGS Tracer Injector on L2 RAGS Transfer line runs from L1 turbo exhaust to B3 NIF Cryo and Turbo Pumps RAGS Room on B3 3

Tracer injector allows high precision and high accuracy assays RGA Accuracy: Stable - 1% Rad - counting statistics Tracers injected a few seconds after Tzero Stable Tracer- 128, 129 Xe in nitrogen Radioactive Tracerradioxenons in nitrogen transferred from 252 Cf source in Building 151 4

RAGS room processes shot gas for in situ and off-line measurements Xenon Collector Ge Cold Getters RGA Inlet, Water Trap LaBr 3 Sample Bottle Cold Getters RGA Abort Tank LaBr 3 Hot Getters LaBr 3 Xenon Collector Cart Filter Cart 5

RAGS capabilities ρr studies via n,γ and n,2n reactions Xenon-loaded DT Exploding Pusher capsule ready Mix studies with n,2n and/or charged particle reactions Xenon-implanted Symcap capsules ready Cross sections Fission products 6

RAGS has identified short-lived products at all detector locations Hot Getter LaBr 3 Detector 100 Abort Tank LaBr 3 Detector 511 kev Count per second 80 60 40 440 kev Ne-23 T 1/2 = 34.2 s Mg-26(n,α)Ne-23 511 kev F-18 T 1/2 = 109.77 min F-19(n,2n)F-18 20 0 10 100 1,000 10,000 100,000 Time, sec We use energy and half-life for identification. 7

In situ Ge detector on Collector Cart comparing signals from a DU hohlraum shot to a RAGS Faux test N140120 (DT w/du Hohlraum) Germanium Detector: Short-lived fission products 91 Kr (t 1/2 = 8.57 sec.) 140 Xe (t 1/2 = 13.6 sec.) 139 Xe (t 1/2 = 39.7 sec.) 138 Xe (t 1/2 = 14.1 min.) 138 Cs (t 1/2 = 32.2 min.) RAGS Faux 133 Xe (t 1/2 = 5.24 day) 133m Xe (t 1/2 = 2.19 day) 135 Xe (t 1/2 = 9.1 hour) 8

We extract the time history of peaks on the Ge detector Background subtracted peak intensities (about 200 observed peaks total) 18 F (511 kev), 110 minutes half-life 138 Cs, 32.2 minutes half-life 140 Ba, 12.75 day half-life 9

We see fission and activation products in the abort tank (LaBr 3 detector) 138 Cs N140120 (DT w/du Hohlraum) Short-lived fission products 90 Kr (t 1/2 = 32.3 sec.) 89 Kr (t 1/2 = 3.15 min.) 88 Kr (t 1/2 = 2.84 hour) 87 Kr (t 1/2 = 76.2 min.) 90 Rb (t 1/2 = 2.6 min.) 89 Rb (t 1/2 = 15.4 min.) 138 Xe (t 1/2 = 14.08 min.) 137 Xe 137 Xe (t 1/2 = 3.82 min.) 138 Cs (t 1/2 = 32.2 min.) Activation products 18 F 511keV (t 1/2 = 110 min.) 23 Ne (t 1/2 = 37.2 sec.) 10

18 F scales linearly with 14 MeV neutron yield and impacts other signals High levels of 18 F could obscure lower-energy gamma signals on the in situ Ge detector, losing diagnostic data. Requested replacement of fluorine-containing materials in the target assembly. However, charged-particle reactions on oxygen in the target may also make 18 F, and oxygen may not be removable. For offline counting with high 18 F, precision of short-lived xenons is 5-10x poorer than samples with low 18 F. 11

Characterizing RAGS Xenon Collection Use stable and radioactive isotope tracers injected into the target chamber a few seconds after Tzero Run faux tests with tracers RAGS, no lasers, no target, no nuclear yield Participate on Keyhole shots, use tracers RAGS, lasers fire, modified target and hohlraum, no nuclear yield Participate on shots with nuclear yield, use tracers RAGS, lasers fire, targets with DT fill 12

On faux tests, 90% of radioxenon tracer is trapped in collector cart and 60-75% is transferred to the sample bottle. Shots with lasers and targets collect and transfer lower xenon amounts. Xe135 signal, 249 kev Sample transferred to bottle Residual sample frozen Fraction of tracer in Collector cart is calculated from RAGS sample bottle fraction and time history of Xe135 signal on Ge detector. 13

Target chamber and RAGS pressures are higher on shots, and gas composition is different, compared to RAGS faux tests. Target Chamber Pressure during RAGS collections Shot Gases Produced: Carbon Monoxide Carbon Dioxide Methane Shot Gases from Target & Hohlraum: Hydrogen Helium Shot Gases released from TC Surfaces: Water Chamber Air leak on shot and RAGS faux: Nitrogen Oxygen Argon 14

RAGS collects >90% of methane from target chamber RAGS pumping model predicts 120 second time interval for half of the shot gas to be removed from the target chamber. Methane measurements for 50% signal reduction range from 140-170 seconds (Filter Cart RGA). Expect xenon acts like methane due to similar physical properties. 15

Gases may be passing through the xenon collector into the abort tank Residual sample frozen Presence of radioxenon and 18 F in the abort tank suggest that more collector capacity is needed on shots compared to faux tests. New collector design and fab are planned for FY15. Some xenon is cotrapped with water in the Filter Cart; increasing trap temperature may mitigate losses here. 16

Plans for FY15 New collector Higher capacity Lower temperature - extend to krypton Calibrate 124 Xe n,2n cross section relative to 136 Xe 124 Xe and 136 Xe in DT-filled exploding pusher Execute xenon-doped ablator mix experiment 124 Xe at 45 microns from inner surface, 136 Xe at 70 microns Improve precisions of independent yield fission product measurements 17

Acknowledgments Arthur Carpenter Tony Golod Amber Marsh Essex Bond Ken Moody Todd Wooddy Phil Torretto B151 Operations NIF Operations NIF Shot RIs Dan Casey Charlie Cerjan Hye-Sook Park Dieter Schneider 18

Questions? 19

Cross sections of n,γ and n,2n reactions on Xe-124 superimposed on the schematic NIF neutron spectrum, which is based on typical neutron time-of-flight spectra 20

Relevant cross-sections for Xe activation Large differences between measured Xe-124 n,2n cross section values can be evaluated at NIF by measurements relative to Xe-136 using targets loaded with both isotopes. Cross-section [b] 2 1.5 1 0.5 0 Xe-124(n2n) ENDF/B-VII.1 Xe-124(n2n) - data: Bazan [1989], Sigg [1976], Kondaiah [1968] Xe-136(n2n) ENDF/B-VII.1 Xe-136(n2n) - data: Sigg [1976], Kondaiah [1968] Xe-136 Bhatia[2013] 5 10 15 20 Neutron Energy [MeV] *Bhatia Phys. Rev. C 87, 011601(R) (2013) 21

Cross sections of neutron induced reactions for background gases observed during a NIF shot 0.10 0.08 F-19(n,2n)F-18 F-19(n,p)O-18 Mg-26(n,a)Ne-23 Cross section, barn 0.06 0.04 0.02 0.00 4 6 8 10 12 14 16 18 20 Energy, MeV 22