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Abstracts Brochure - CERN

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THPLS087<br />

THPLS088<br />

THPLS089<br />

THPLS090<br />

29-Jun-06 16:00 - 18:00 THPLS — Poster Session<br />

A Control Theory for Dynamic Aperture<br />

The dynamic aperture problem dates back<br />

J. Bengtsson (BNL)<br />

to the design of the first synchrotrons. Over<br />

time, both analytical and numerical methods<br />

have been pursued. In the former case mainly by applying techniques developed for celestial mechanics to rather<br />

simplified equations of motion. Over the last decade, analysis of the Poincare map has become the method of choice.<br />

In particular, application of symplectic integrators, truncated power series algebra, and Lie series techniques has<br />

led to a complete set of tools for self-consistent numerical simulations and analytic treatment of realistic models.<br />

Nevertheless, a control theory for the general nonlinear case remains elusive. We summarize how to apply this<br />

framework to the design of modern synchrotron light sources. Moreover, we also outline how a control theory can be<br />

formulated based on the Lie generators for the nonlinear terms.<br />

Optimizing the Dynamic Aperture for Triple Bend Achromatic Lattices<br />

The Triple Bend Achromatic (TBA) lattice has<br />

S.L. Kramer, J. Bengtsson (BNL)<br />

the potential for lower natural emittance per<br />

period than the Double Bend Achromatic<br />

(DBA) lattice for high brightness light sources. However, the DBA has been chosen for 3rd generation light sources<br />

more often due to the higher number of undulator straight section available for a comparable emittance. The TBA has<br />

considerable flexibility in linear optics tuning while maintaining this emittance advantage. We have used the tune<br />

and chromaticity flexibility of a TBA lattice to minimize the lowest order nonlinearities using a high order achromatic<br />

tune condition, while maintaining a constant emittance. This frees the geometric sextupoles to counter the higher<br />

order nonlinearities. This procedure is being used to improve the nonlinear dynamics of the TBA as a proposed lattice<br />

for the NSLS-II facility. The flexibility of the TBA lattice will also provide for future upgrade capabilities of the beam<br />

parameters.<br />

Comparison of Double Bend and Triple Bend Achromatic Lattice Structures for NSLS-II<br />

The Double Bend Achromatic (DBA) and the<br />

S.L. Kramer (BNL)<br />

Triple Bend Achromatic (TBA) lattice have<br />

been studied rather extensively for use for<br />

the NSLS-II storage ring. The well known advantage of the TBA compared to the DBA is that the emittance per period<br />

has the potential to be considerably lower. However, the DBA has been chosen more often due to the greater number<br />

of ID straight sections for the users for a desired emittance. We present a comparison of these lattice structures based<br />

on the optimization of the non-linear driving terms from the chromatic sextupole and the ease of compensation of<br />

these terms using the higher order achromatic cancellation.<br />

Consideration of the Double Bend Achromatic Lattice for NSLS-II<br />

We present the results of a study of the Dou-<br />

S. Krinsky, J. Bengtsson, S.L. Kramer (BNL)<br />

ble Bend Achromatic (DBA) lattice as a possible<br />

choice for the NSLS-II storage ring. The<br />

DBA possesses a large number of straight sections with easily tunable beta functions which can be used for insertion<br />

472

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