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The AGS-Booster Lattice

The AGS-Booster Lattice
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Release: 1987
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The AGS Booster has three objectives. They are to increase the space charge limit of the AGS, to increase the intensity of the polarized proton beam by accumulating many linac pulses (since the intensity is limited by the polarized ion source), and to reaccelerate heavy ions from the BNL Tandem Van de Graaff before injection into the AGS. The machine is capable of accelerating protons at 7.5 Hertz from 200 MeV to 1.5 GeV or to lower final energies at faster repetition rates. The machine will also be able to accelerate heavy ions from as low as 1 MeV/nucleon to a magnetic rigidity as high as 17.6 Tesla-meters with a one second repetition rate. As an accumulator for polarized protons, the Booster should be able to store the protons at 200 MeV for several seconds. We expect that the Booster will increase the AGS proton intensity by a factor of four, polarized proton intensity by a factor of twenty to thirty, and will also enable the AGS to accelerate all species of heavy ions (at present the AGS heavy ion program is limited to the elements lighter than sulfur because it can only accelerate fully stripped ions). The construction project started in FY 1985 and is expected to be completed in 1989. The purpose of this paper is to provide a future reference for the AGS Booster lattice.


Design and Status of the AGS Booster Accelerator

Design and Status of the AGS Booster Accelerator
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Release: 1987
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Comments are given on some areas of the design considered for the AGS Booster Accelerator, including lattice design, energy and repetition rate, injection, radio frequency system, and the vacuum system. The current status is then briefly described. (LEW).


A Study of the Coupling Resonances in the AGS Booster

A Study of the Coupling Resonances in the AGS Booster
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Release: 1988
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Analytic method is used to analyze the tracking results for the AGS-BOOSTER lattice. We found the amplitude dependence of the tune is very important in understanding characteristic of the tracking result. With the perturbed tune, the effective second order perturbation theory work very well. The method can be used to analyze the optimized operational condition for the lattice. For the Booster, the analysis suggests that chromaticity of -2 and -5 and a minimum unperturbed tune split chemically bond[Delta][nu]°chemically bond> 0.01. At the zero chromaticity point, the required unperturbed tune split is considerably larger in order to obtain a similar performance. 7 refs., 4 figs.


Rematching AGS Booster Synchrotron Injection Lattice for Smaller Transverse Beam Emittances

Rematching AGS Booster Synchrotron Injection Lattice for Smaller Transverse Beam Emittances
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Total Pages: 5
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The polarized proton beam is injected into the booster via the charge-exchange (H- to H+) scheme. The emittance growth due to scattering at the stripping foil is proportional to the beta functions at the foil. It was demonstrated that the current scheme of reducing the beta functions at the stripping foil preserves the emittance better; however the betatron tunes are above but very close to half integer. Due to concern of space charge and half integer in general, options of lattice designs aimed towards reducing the beta functions at the stripping foil with tunes at more favorable places are explored.


Chromatic Perturbation and Resonance Analysis for the AGS Booster

Chromatic Perturbation and Resonance Analysis for the AGS Booster
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Release: 1987
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We have investigated the nonlinear effects with the emphasis on nonlinear resonances. We present some of our findings (e.g., the structure resonances; stop-bandwiths, etc.) for the AGS-Booster Lattice using program HARMON. Comparison with the results obtained from our algorithm ''NONLIN'' is presented.