dorsal/arxiv
View SchemaReconstruction of Initial Beam Conditions at the Exit of the DARHT II Accelerator
| Authors | Arthur C. Paul |
|---|---|
| Categories | |
| ArXiv ID | physics/0008057 |
| URL | https://arxiv.org/abs/physics/0008057 |
| Journal | eConf C000821 (2000) TUB10 |
Abstract
We consider a technique to determine the initial beam conditions of the DARHT II Accelerator by measuring the beam size under three different magnetic transport settings. This may be time gated to resolve the parameters as a function of time within the 2000 nsec pulse. This technique leads to three equations in three unknowns with solution giving the accelerator exit beam radius, tilt and emittance. We find that systematic errors cancel and so are not a problem in unfolding the initial beam conditions. Random uncorrelated shot to shot errors can be managed by one of three strategies: 1) make the transport system optically de-magnifying; 2) average over many individual shots; or 3) make the random uncorrelated shot to shot errors sufficiently small. The high power of the DARHT II beam requires that the beam transport system leading to a radius measuring apparatus be optically magnifying. This means that the shot to shot random errors must either be made small (less than about 1%) or that we average each of the three beam radius determinations over many individual shots.
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"abstract": "We consider a technique to determine the initial beam conditions of the DARHT\nII Accelerator by measuring the beam size under three different magnetic\ntransport settings. This may be time gated to resolve the parameters as a\nfunction of time within the 2000 nsec pulse. This technique leads to three\nequations in three unknowns with solution giving the accelerator exit beam\nradius, tilt and emittance. We find that systematic errors cancel and so are\nnot a problem in unfolding the initial beam conditions. Random uncorrelated\nshot to shot errors can be managed by one of three strategies: 1) make the\ntransport system optically de-magnifying; 2) average over many individual\nshots; or 3) make the random uncorrelated shot to shot errors sufficiently\nsmall. The high power of the DARHT II beam requires that the beam transport\nsystem leading to a radius measuring apparatus be optically magnifying. This\nmeans that the shot to shot random errors must either be made small (less than\nabout 1%) or that we average each of the three beam radius determinations over\nmany individual shots.",
"arxiv_id": "physics/0008057",
"authors": [
"Arthur C. Paul"
],
"categories": [
"physics.acc-ph"
],
"journal_ref": "eConf C000821 (2000) TUB10",
"title": "Reconstruction of Initial Beam Conditions at the Exit of the DARHT II Accelerator",
"url": "https://arxiv.org/abs/physics/0008057"
},
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