Development of a High Intensity EBIT for Basic and Applied Science

Similar documents
Parametric Instabilities in Laser/Matter Interaction: From Noise Levels to Relativistic Regimes

Modeling Laser and e-beam Generated Plasma-Plume Experiments Using LASNEX

Simulation of Double-Null Divertor Plasmas with the UEDGE Code

August 3,1999. Stiffness and Strength Properties for Basic Sandwich Material Core Types UCRL-JC B. Kim, R.M. Christensen.

Analysis of Shane Telescope Aberration and After Collimation

Magnetic Measurements of the Elliptical Multipole Wiggler Prototype

DML and Foil Measurements of ETA Beam Radius

HEAT TRANSFER AND THERMAL STRESS ANALYSES OF A GLASS BEAM DUMP

Modified Kriging: Evaluation, Modification, Recommendations

Applications of Pulse Shape Analysis to HPGe Gamma-Ray Detectors

LLNL DATA COLLECTION DURING NOAAETL COPE EXPERIMENT

Safety Considerations for Laser Power on Metals in Contact with High Explosives-Experimental and Calculational Results

Modeling of MHD Equilibria and Current Profile Evolution during the ERS Mode in TFTR

Fission-Fusion Neutron Source

The Design and Fabrication of a 6 Tesla EBIT Solenoid

Impurity Transport Studies of Intrinsic MO and Injected Ge in High Temperature ECRH Heated FTU Tokamak Plasmas

Controlling Backstreaming Ions from X-ray Converter Targets with Time Varying Final Focusing Solenoidal Lens and Beam Energy Variation

Using the X-FEL to understand X-ray Thomson scattering for partially ionized plasmas

Plutonium 239 Equivalency Calculations

Solid Phase Microextraction Analysis of B83 SLTs and Core B Compatibility Test Units

BWXT Y-12 Y-12. A BWXT/Bechtel Enterprise SMALL, PORTABLE, LIGHTWEIGHT DT NEUTRON GENERATOR FOR USE WITH NMIS

CQNl_" RESPONSE TO 100% INTERNAL QUANTUM EFFICIENCY SILICON PHOTODIODES TO LOW ENERGY ELECTRONS AND IONS

A Distributed Radiator, Heavy Ion Driven Inertial Confinement Fusion Target with Realistic, Multibeam Illumination Geometry

GA A22722 CENTRAL THOMSON SCATTERING UPGRADE ON DIII D

Destruction of 2,4,6=Trinitrotoluene using Ammonium Peroxydisulfate

Partial Discharge Characterization of High-Voltage Cables and Components

Capabilities for Testing the Electronic Configuration in Pu

GA A26686 FAST ION EFFECTS DURING TEST BLANKET MODULE SIMULATION EXPERIMENTS IN DIII-D

Flipping Bits in the James Webb Space Telescope s Cameras

Plasma Response Control Using Advanced Feedback Techniques

Multicusp Sources for Ion Beam Lithography Applications

OAK RIDGE NATIONAL LABORATORY

Scaling of divertor heat flux profile widths in DIII-D

A New Computational Method for non-lte, the Linear Response Matrix

GA A26057 DEMONSTRATION OF ITER OPERATIONAL SCENARIOS ON DIII-D

IMPACT OF EDGE CURRENT DENSITY AND PRESSURE GRADIENT ON THE STABILITY OF DIII-D HIGH PERFORMANCE DISCHARGES

PROJECT PROGRESS REPORT (03/lfi?lfibr-~/15/1998):

Final Technical Report. Department of Energy. for

The Radiological Hazard of Plutonium Isotopes and Specific Plutonium Mixtures

Response to Comment on "The National Ignition Facility Laser Performance Status"

Optimization of NSLS-II Blade X-ray Beam Position Monitors: from Photoemission type to Diamond Detector. P. Ilinski

The Gas Flow from the Gas Attenuator to the Beam Line

Two-Screen Method for Determining Electron Beam Energy and Deflection from Laser Wakefield Acceleration

To be published in the Proceedings of ICEC-22, Seoul Korea, July 2008 MICE Note 232 1

The Highest Redshift Radio Galaxy Known in the Southern Hemisphere

Design of Current Leads for the MICE Coupling Magnet

Turbulent Scaling in Fluids. Robert Ecke, MST-10 Ning Li, MST-10 Shi-Yi Li, T-13 Yuanming Liu, MST-10

GA A27235 EULERIAN SIMULATIONS OF NEOCLASSICAL FLOWS AND TRANSPORT IN THE TOKAMAK PLASMA EDGE AND OUTER CORE

The photoneutron yield predictions by PICA and comparison with the measurements

How Small Can a Launch Vehicle Be?

ION EXCHANGE SEPARATION OF PLUTONIUM AND GALLIUM (1) Resource and Inventory Requirements, (2) Waste, Emissions, and Effluent, and (3) Facility Size

GA A25853 FAST ION REDISTRIBUTION AND IMPLICATIONS FOR THE HYBRID REGIME

PRINCETON PLASMA PHYSICS LABORATORY PRINCETON UNIVERSITY, PRINCETON, NEW JERSEY

m w n? r i OF,THISDOCUMENT IS UNLIMITED

GA A23736 EFFECTS OF CROSS-SECTION SHAPE ON L MODE AND H MODE ENERGY TRANSPORT

GA A22677 THERMAL ANALYSIS AND TESTING FOR DIII D OHMIC HEATING COIL

A Germanium Detector with Optimized Compton Veto for High Sensitivity at Low Energy

Initial Results from the Lick Observatory Laser Guide Star Adaptive Optics System

GA A23713 RECENT ECCD EXPERIMENTAL STUDIES ON DIII D

Curvature of a Cantilever Beam Subjected to an Equi-Biaxial Bending Moment. P. Krulevitch G. C. Johnson

(4) How do you develop an optimal signal detection technique from the knowledge of

GA A26474 SYNERGY IN TWO-FREQUENCY FAST WAVE CYCLOTRON HARMONIC ABSORPTION IN DIII-D

Sputter Deposition of Nanocones for Field Emission

INTERMOLECULAR POTENTIAL FUNCTIONS AND HIGH RESOLUTION MOLECULAR SPECTROSCOPY OF WEAKLY BOUND COMPLEXES. Final Progress Report

Shock compression of precompressed deuterium

Modeling of psec-laser-driven Ne-like and Ni-like X-ray lasers. Joseph Nilsen

UNDERSTANDING TRANSPORT THROUGH DIMENSIONLESS PARAMETER SCALING EXPERIMENTS

Novel Nanoparticles for Ultrasensitive Detection and Spectroscopy

GA A27806 TURBULENCE BEHAVIOR AND TRANSPORT RESPONSE APPROACHING BURNING PLASMA RELEVANT PARAMETERS

Alex Dombos Michigan State University Nuclear and Particle Physics

Determine the Inside Wall Temperature of DSTs using an Infrared Temperature Sensor

GA A22689 SLOW LINER FUSION

Colliding Crystalline Beams

GA A25658 PRECISION X-RAY OPTICAL DEPTH MEASUREMENTS IN ICF SHELLS

UPGRADED CALIBRATIONS OF THE THOMSON SYSTEM AT DIII D

RESEARCH OPPORTUNITIES AT THE CNS (Y-12 AND PANTEX) NUCLEAR DETECTION AND SENSOR TESTING CENTERS (NDSTC)

Vector Potential Remap for 2d MHD

sample-specific X-ray speckle contrast variation at absorption edges $ & ~ 0

Three-Dimensional Silicon Photonic Crystals

Data Comparisons Y-12 West Tower Data

Study of a Non-Intrusrve blectron

GA A24166 SUPER-INTENSE QUASI-NEUTRAL PROTON BEAMS INTERACTING WITH PLASMA: A NUMERICAL INVESTIGATION

FUSION TECHNOLOGY INSTITUTE

+.V) eo(o) -2 so - sx. hngc)90w3-- Beam-beam collisions and crossing angles in RHIC*

GA A27857 IMPACT OF PLASMA RESPONSE ON RMP ELM SUPPRESSION IN DIII-D

SciDAC CENTER FOR SIMULATION OF WAVE-PLASMA INTERACTIONS

Preparation of DielectAcs HR Mirrors from Colloidal Oxide Suspensions Containing Organic Polymer Binders

ADSORPTION ON NANOSURFACES: A DETAILED LOOK AT METAL CLUSTERS USING INFRARED SPECTROSCOPY

~ _- IDOCLRXKT DMSP SATELLITE DETECTIONS OF GAMMA-RAY BURSTS. J. Terrell, NIS-2 P. Lee, NIS-2 R W.

S.A. Kreek J.E. Kammeraad D. Beckedahl G.J. Schmid J.J. Blair B. Payne A. Friensehner

Hydra Fault Current Limiting HTS Cable to be Installed in the Consolidated Edison Grid

Laser Intensity Modulation by Nonabsorbing Defects. M. D. Feit A. M. Rubenchik

GA A THERMAL ION ORBIT LOSS AND RADIAL ELECTRIC FIELD IN DIII-D by J.S. degrassie, J.A. BOEDO, B.A. GRIERSON, and R.J.

Bandgap Photons to GaInP2

Status and Progress of a Fault Current Limiting HTS Cable To Be Installed In The Consolidated Edison Grid

Use of Nuclear Explosives for Excavation of Sea-Level Canal Across the Negev Desert (Canal Studies Filefolder)

INITIAL RESULTS OF THE COMMISSIONING OF THE HRIBF RECOIL MASS SPECTROMETER

TARGET PLATE CONDITIONS DURING STOCHASTIC BOUNDARY OPERATION ON DIII D

Excitations of the transversely polarized spin density. waves in chromium. E3-r 1s

Walter P. Lysenko John D. Gilpatrick Martin E. Schulze LINAC '98 XIX INTERNATIONAL CONFERENCE CHICAGO, IL AUGUST 23-28,1998

Transcription:

UCRL-ID- 129832 Development of a High Intensity EBIT for Basic and Applied Science R.E. Marrs D. Schneider February 5,1998 This is an informal report intended primarily for internal or limited external distribution. The opinions and conclusions stated are those of the author and may or may not be those of the Laboratory. Work performed under the auspices of the U.S. Department of Energy by the Lawrence Livermore National Laboratory under Contract W-7405ENG-48.

DISCLAIMER This document was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor the University of California nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or the University of California. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or the University of California, and shall not be used for advertising or product endorsement purposes. This report has been reproduced directly from the best available copy. Available to DOE and DOE contractors from the Office of Scientific and Technical Information P.O. Box 62, Oak Ridge, TN 37831 Prices available from (423) 5768401 Available to the public from the National Technical Information Service U.S. Department of Commerce 5285 Port Royal Rd., Springfield, VA 22161

Final Report for LDRD Project 97-ERD-109 Development of a High Intensi& EBIT for Basic and Applied Science Principal Investigator: R E. Marrs Co-Investigator: D. Schneider Prepared February 5, 1998 Introduction The electron-beam ion trap (EBIT) is a device for producing and studying cold, very highly charged ions of any element, up to a fully ionized U92+. These highly charged ions occur in hot plasmas and therefore play important roles in nuclear weapons, controlled fusion, and astrophysical phenomena. The remarkable interaction of these ions with surfaces may lead to technological applications. The highly charged ions can either be studied inside the EBIT itself with measurements of their x-ray emission spectra, or the ions can be extracted from the EBIT in order to study their interaction with solid material. Both types of measurements are being pursued vigorously with the two existing low-intensity EBITs at LLNL and with similar EBITs that have been built at six other laboratories around the world since the EBIT was first developed at LLNL 10 years ago. However, all existing EBITs have approximately the same intensity as the original LLNL EBIT; that is, they all produce about the same number of very-highly-charged ions (roughly 2 x lo6 per second) and the same number of x-ray photons (roughly lo7 per second). The goal of the High-Intensity-EBIT project is to increase the x-ray emission per centimeter of length along the electron beam by a factor of 100 and to increase the ion output by a factor of 1000. This dramatic increase in intensity will enable the next generation of basic and applied experimental research in the structure of highly charged ions. For example, the precision of EBIT x-ray measurements of atomic energy levelswhich is now limited by count rate-can be improved by an order of magnitude, and new applications in surface science, nanotechnology, and microscopy will be possible with the expected intense ion beams. When the high ion output is combined with the

demonstrated low emittance of EBIT ions, we will have a high-brightness source of highly charged ions that can be focused to submicrometer spots. One example of a measurementhat will benefit from increased x-ray intensity is our study of the binding energy of high-2 heliumlike ions. The small two-electron contribution to this binding energy is a fundamental aspect of atomic structure. It arises from the small forces that the two electrons exert on each other in the presence of the much larger force from the atomic nucleus. Our existing EBIT measurements are sensitive to the so-called second order contribution to the two-electron binding energy, but with the High-Intensity EBIT we can probe an even more subtle effect: the screening by one electron of the quantum electrodynamic (QED) energy contribution from the other electron. Design of the High-Intensity EBIT Although the basic EBIT concept of highly charged ions trapped within the spacecharge potential of an electron beam remains the same, the design of our High-Intensity EBIT is very different from that of existing EBITs. We have made three significant changes to obtain higher intensity: (1) We doubled the magnetic field (from 3 to 6 T) to obtain greater electron-beam compression; (2) We designed a new electron gun with a higher cathode brightness and a total electron current that is two times greater (and can be upgraded to ten times greater) than that of existing EBITs; and (3) We made the ion trap 10 times longer. The electron beam collector is designed to dissipate a power of more than 20 kw in order to handle the largest anticipated beam current. The cryostat has been designed for minimal consumption of liquid helium (we expect the High-Intensity EBIT to consume an order of magnitude less liquid helium than the existing LLNL EBITs), thereby greatly reducing a large operating expense. Accomplishments The development of the High-Intensity EBIT was approximately 90% complete at the end of FY 1997. Nearly all of the parts have been fabricated except for the drift-tube subassembly. We have completed and tested the electron gun, and verified that the measured compression of the electron beam in a magnetic field agrees with theoretical predictions. To measure the electron beam compression, we developed a novel x-ray technique for studying electron beams injected into magnetic fields. 2

The most critical component of the High-Intensity EBIT is the 6-T superconducting magnet. This magnet is of a unique design that is split into four coils to allow radial access at two different elevations: the midplane of the trap and a second location near the end of the trap. In spite of large gaps between the coils to facilitate x- ray measurements, the 6-T magnetic field is uniform to within 1% over the 2%cm length of the trap. The inside bore of the magnet bobbin is 10 cm, a value large enough to allow the ion trap to float at very high voltage (up to 100 kv) or accommodate large-solid-angle x-ray detectors for future coincidence measurements. The magnet will operate in persistent mode in a SO-liter liquid helium dewar. We have also completed fabrication of the electron beam collector and most of the cryostat parts. The collector includes two water-cooled magnets that operate at room temperature. Like the electron gun, the collector is designed to float at voltages up to 200 kv. When combined with the high voltage on the ion trap electrodes, this will result in an even higher electron beam energy than that of the LLNL Super EBIT. EBIT devices are known to have a low emittance, which means that the ions extracted from them can be focused to a small spot with a small divergence. The large number of ions expected from the High-Intensity EBIT suggests that it could become a very bright source of highly charged ions. (Brightness is defined as the number of ions per second per unit area per unit solid angle.) One reason for the low emittance (high brightness) is the process of evaporative ion cooling that takes place in an EBIT trap. Suspecting that the brightness could be increased even further by self-cooling of the highly charged ions as they are released from the trap, we constructed a computer model of this process. The results indicate that the High-Intensity EBIT can be operated as a very-high-brightness source of highly charged ions. In fact, the brightness may be several orders of magnitude beyond what was previously suspected. Future Plans Although LDRD support for this project ended in FY 1997, we plan to complete the fabrication and assembly of the High-Intensity EBIT and begin initial experiments with the highly charged ions it produces. The expected capabilities of the High-Intensity EBIT will enable a new generation of basic and applied science with highly charge ions.

Technical Information Department Lawrence Livermore National Laboratory University of California Livermore, California 94551