LAWRENCE Livermore has long been recognized as a leader in the world of scientific computer simulations--creating multidimensional models of the dynamic and complex forces unleashed by nuclear explosives, visualizing the processes at work in the birth and death of stars, and studying the effects of greenhouse gases on global climate and of pollutants in our environment. It is not surprising, then, that the Laboratory is also a leading developer of computer codes that simulate propagation and interaction of electromagnetic (EM) fields.![]() ![]() |
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Livermore Codes
Rick Ratowsky calls it a Virtual Optical Bench, a user-friendly graphics interface for designers of photonic circuits, the optical world's equivalent of electronic circuits. "It is a photonics design tool with broad applicability," says Ratowsky, an electrical engineer.
Some photonics components have very small features, at a single wavelength scale; some features are very large, say thousands of wavelengths. Such devices have been very difficult to design because there is no easy way to put these differently scaled parts together.
A modeling code known as MELD (Multi-Scale Electrodynamics) will allow different length scales to be used concurrently--saving optoelectronics researchers much time and effort. (See figure below.) The MELD code draws on techniques of both the electromagnetics and optics communities and integrates them in a way never used before.
"I can't say that all the techniques themselves are unique to Livermore," observes Ratowsky, "but their implementation and integration are." MELD joins a long list of EM codes developed at Livermore. Following is a brief summary of key modeling codes. All are used to solve equations arising from the fundamental classical electromagnetic field equations enunciated by James Clerk Maxwell in 1873.
Specialized Models for Analysis and Design![]() ![]() ![]() ![]() ![]()
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Understanding Wakefields
A charged particle beam traveling through an accelerator transport system, or beamline, has an associated electromagnetic (EM) field.
If the beamline is free of perturbations, the beam's EM field is not disturbed. However, a perturbation can modify the local electrodynamic properties of the structure.
Perturbations can consist of changes in cross section, apertures in the transport system wall, curved beamlines, or the introduction of different materials into the beam transport line.
As the charged particle beam streams past these perturbations in the structure, the beam's EM field is scattered from the structure. This EM field is called a wakefield (Figure 3) because the scattering occurs in the wake of the very-high-velocity particle.
This wakefield can interact with other particles traveling down the beamline behind the exciting particle, sometimes in an undesirable way, leading to the beam's degradation or, worse, breakup.
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Key Words: electromagnetic field, electromagnetic susceptibility, kicker, modeling, opto-electronics, photonics, wakefield.
Reference
1. K. S. Yee, "Numerical Solution of Initial Boundary Value Problems Involving Maxwell's Equations in Isotopic Media," IEEE Transactions on Antennas and Propagation AP-14, 302-307 (May 1966).
For additional information contact Clifford C. Shang (510) 422-6174 (shang1@llnl.gov).
Electrical engineers who collaborate in the Laboratory's computational electronics and electromagnetic thrust area include: (first row) DAVID STEICH, STEVE SAMPAYAN, JEFF KALLMAN, CLIFF SHANG, and BRIAN POOLE; (second row) RICK RATOWSKY, TOM ROSENBURY, and SCOTT D. NELSON. For more information about their work, visit their Internet home page on EM codes at http://www.llnl.gov/eng/ee/documents/ceeta.html and EM facilities at http://www-dsed.llnl.gov/documents/facilities.html. The group is pictured in front of the Experimental Test Accelerator-II (ETA-II). The ETA is a testbed for beam experiments n advanced hydrodynamics testing to characterize the accelerator and design key components. The accelerator ultimately will be a part of the Laboratory's Advanced Hydrotest Facility.