SDDS-based software tools for accelerntor design

Borland, M.; Emery, L.; Shang, Hairong; Soliday, R.

doi:10.1109/pac.2003.1289948

Cited by 5 publications

(4 citation statements)

References 5 publications

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“…Instead, we chose to make a grid of solutions covering the tune plane on ν straightforward by the fact that elegant saves and loads lattice data in self-describing data sets (SDDS) files [20][21][22], which allowed collation and interpolation of the quadrupole strength table without writing any new code, using the SDDS toolkit programs.…”

Section: Tune Variationmentioning

confidence: 99%

Multi-objective direct optimization of dynamic acceptance and lifetime for potential upgrades of the Advanced Photon Source.

Borland¹,

Sajaev²,

Emery³

et al. 2010

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The Advanced Photon Source (APS) is a 7 GeV storage ring light source that has been in operation for well over a decade. In the near future, the ring may be upgraded, including changes to the lattice such as provision of several long straight sections (LSS). Because APS beamlines are nearly fully built out, we have limited freedom to place LSSs in a symmetric fashion. Arbitrarilyplaced LSSs will drastically reduce the symmetry of the optics and would typically be considered unworkable. We apply a recently-developed multi-objective direct optimization technique that relies on particle tracking to compute the dynamic aperture and Touschek lifetime. We show that this technique is able to tune sextupole strengths and select the working point in such a way as to recover the dynamic and momentum acceptances. We also show the results of experimental tests of lattices developed using these techniques.

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Section: Tune Variationmentioning

confidence: 99%

Multi-objective direct optimization of dynamic acceptance and lifetime for potential upgrades of the Advanced Photon Source.

Borland¹,

Sajaev²,

Emery³

et al. 2010

Self Cite

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“…The RF gun should generate a beam with a high linearity of bunch energy to bunch length at the high energy part which can be compressed by an alphamagnet from few tens of picoseconds to few hundreds of femtoseconds. We use the simulation codes such as SUPERFISH [5] , PARMELA [6] , and ELEGANT [7] to get the beam profile and the cavity dimensions.…”

Section: Cavity Design and Manufacturementioning

confidence: 99%

RF gun for an intense THz radiation source

Zhao

Tong

et al. 2008

Chinese Phys. C

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“…We used the program sddsbrightness [17] to compute brightness curves for the beam at the end of a turn for the ZD lattice, for a standard APS ''undulator A,'' which has a 3.3-cm period and a length of 2.4 m. Fig. 10 shows a comparison of average brightness for the ERL beam to the present APS at 100 mA and 1% coupling.…”

Section: Article In Pressmentioning

confidence: 99%

Evaluation of the possibility of upgrading the advanced photon source to an energy recovery linac

Borland

2006

Nuclear Instruments and Methods in Physics Research Section A:

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SDDS-based software tools for accelerntor design

Cited by 5 publications

References 5 publications

Multi-objective direct optimization of dynamic acceptance and lifetime for potential upgrades of the Advanced Photon Source.

Multi-objective direct optimization of dynamic acceptance and lifetime for potential upgrades of the Advanced Photon Source.

RF gun for an intense THz radiation source

Evaluation of the possibility of upgrading the advanced photon source to an energy recovery linac

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