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NASA Scientific and Technical Aerospace Reports

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20060002069 Fermi National Accelerator Lab., Batavia, IL, USA<br />

New Technique for Making Bright Proton Bunches Using Barrier RF Systems<br />

Bhat, C. M.; January 2005; 8 pp.; In English<br />

Report No.(s): DE2005-15017083; FERMILAB-CONF-05-140-AD; No Copyright; Avail.: National <strong>Technical</strong> Information<br />

Service (NTIS)<br />

I describe here a very promising scheme for producing bright proton bunches for proton-antiproton <strong>and</strong> proton-proton<br />

colliders. The method is based on the use of wide-b<strong>and</strong> barrier rf systems. First, I explain the principle of the method. The<br />

beam dynamics simulations applied to the Fermilab Main Injector (MI) suggest that the scheme allows a wide range of bunch<br />

intensities <strong>and</strong> emittances for ppbar collider. This method has the potential to increase the instantaneous luminosity by greater<br />

than or equal to 30% at the Tevatron.<br />

NTIS<br />

Protons; Radio Frequencies; Proton-Antiproton Interactions; Emittance; Particle Accelerators<br />

20060002070 Fermi National Accelerator Lab., Batavia, IL, USA<br />

Iso-Adiabatic Merging of Pbar Stacks in the Fermilab Recycler<br />

Bhat, C. M.; January 2004; 8 pp.; In English<br />

Report No.(s): DE2005-15017084; FERMILAB-CONF-05-150; No Copyright; Avail.: Department of Energy Information<br />

Bridge<br />

Considerable longitudinal emittance (LE) dilution is seen during merging of two stacks of pbars in the Fermilab Recycler.<br />

The emittance dilution results from the sequence of RF manipulations used for merging. Here the author presents a new<br />

scheme for merging two stacks adiabatically. This involves energy matching of the two stacks before merging. An analytical<br />

expression is derived for energy matching condition. The scheme is illustrated with multi-particle beam dynamics simulations<br />

<strong>and</strong> beam measurements. The beam experiments have shown that one can preserve the emittance to better than 15%.<br />

NTIS<br />

Stacks; Particle Beams<br />

20060002198 Fermi National Accelerator Lab., Batavia, IL, USA, New Mexico Univ., Albuquerque, NM, USA, Los Alamos<br />

National Lab., NM USA, Rutherford Appleton Lab., Chilton, UK<br />

8 GeV H- Ions: Transport <strong>and</strong> Injection<br />

Chou, W.; Bryant, H.; Drozhdin, A.; Hill, C.; Kostin, M.; January 2005; 8 pp.; In English<br />

Report No.(s): DE2005-15017059; FERMILAB-CONF-05-225-AD; No Copyright; Avail.: National <strong>Technical</strong> Information<br />

Service (NTIS)<br />

Fermilab is working on the design of an 8 GeV superconducting RF H(sup -) linac called the Proton Driver. The energy<br />

of H(sup -) beam will be an order of magnitude higher than the existing ones. This brings up a number of technical challenges<br />

to transport <strong>and</strong> injection of H(sup -) ions. This paper will focus on the subjects of stripping losses (including stripping by<br />

blackbody radiation, field <strong>and</strong> residual gas) <strong>and</strong> carbon foil stripping efficiency, along with a brief discussion on other issues<br />

such as Stark states lifetime of hydrogen atoms, single <strong>and</strong> multiple Coulomb scattering, foil heating <strong>and</strong> stress, radiation<br />

activation, collimation <strong>and</strong> jitter correction, etc.<br />

NTIS<br />

Injection; Linear Accelerators; Protons<br />

20060002200 Fermi National Accelerator Lab., Batavia, IL, USA<br />

Feasibility Study of Beam-Beam Compensation in the Tevatron with Wires<br />

Sen, T.; Erdelyi, B.; January 2005; 8 pp.; In English<br />

Report No.(s): DE2005-15017078; No Copyright; Avail.: National <strong>Technical</strong> Information Service (NTIS)<br />

We explore the possibility of compensating long-range beam-beam interactions in the Tevatron by current carrying wires.<br />

Compensation strategies depend on whether the compensation is done close to the interaction or nonlocally, on the aspect ratio<br />

of the strong beam <strong>and</strong> on other details. Strategies for each case have been developed <strong>and</strong> applied to the Tevatron. We discuss<br />

the results of these strategies at injection <strong>and</strong> collision energy.<br />

NTIS<br />

Beam Interactions; Feasibility; Particle Accelerators; Wire<br />

190

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