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A technique using RF bucket reduction for acquiring information about the particle distribution in longitudinal phase space has been applied in the Fermilab Booster. Data sets were obtained at six important time intervals of a Booster cycle…

Accelerator Physics · Physics 2007-05-23 Xi Yang , C. Ankenbrandt

The development of magnetic cogging is part of the Fermilab Booster upgrade within the Proton Improvement Plan (PIP). The Booster is going to send 2.25E17 protons/hour which is almost double the present flux, 1.4E17 protons/hour to the Main…

Accelerator Physics · Physics 2015-02-03 K. Seiya , S. Chaurize , C. Drennan , W. Pellico , A. K. Triplett , A. Waller

The Fermilab booster has an intensity upgrade plan called the Proton Improvement plan (PIP). The flux throughput goal is 2E17 protons/hour which is almost double the current operation at 1.1E17 protons/hour. The beam loss in the machine is…

Accelerator Physics · Physics 2013-01-31 K. Seiya , C. Drennan , W. A. Pellico , K. Triplett , A. Waller

We examine the potential impacts to slip-stacking from a change of the Booster cycle-rate from 15- to 20-Hz. We find that changing the Booster cycle-rate to 20-Hz would greatly increase the slip-stacking bucket area, while potentially…

Accelerator Physics · Physics 2014-06-27 Jeffrey Eldred , Robert Zwaska

The Fermilab Booster uses multi-turn beam injection with all its cavities phased such that beam sees a net zero RF voltage even when each station is at the same maxi-mum voltage. During beam capture the RF voltage is increased slowly by…

A new beam injection scheme is proposed for the Fermilab Booster to increase beam brightness. The beam is injected on the deceleration part of the sinusoidal magnetic ramp and capture is started immediately after the injection. During the…

Accelerator Physics · Physics 2015-04-28 C. M. Bhat

At the Fermilab Booster, and many other proton facili-ties, an intense proton beam is accumulated by multi-turn injection of an H- beam through a stripping foil. The circu-lating beam scatters off the injection foil and large-angle Coulomb…

Accelerator Physics · Physics 2019-12-09 J. Eldred , C. M. Bhat , S. Chaurize , V. Lebedev , S. Nagaitsev , K. Seiya , C. Y. Tan , R. J. Tesarek

The Recycler Ring at Fermilab uses a barrier rf system for all of its rf manipulations. In this paper, I will give an overview of historical perspective on barrier rf systems, the longitudinal beam dynamics issues, aspects of rf…

Accelerator Physics · Physics 2012-08-30 C. M. Bhat

During Nova operations it is planned to run the Fermilab Recycler in a 12 batch slip stacking mode. In preparation for this, measurements of the tune during a six batch injection and then as the beam is slipped by changing the RF frequency,…

Accelerator Physics · Physics 2013-02-01 D. J. Scott , D. Capista , I. Kourbanis , K. Seiya , M. -J. Yan

Currently a fast vertical 1.08-m long kicker (notcher) located in the Fermilab Booster Long-5 straight section is used to remove 3 out of 84 circulating bunches after injection to generate an abort gap. With magnetic field of 72.5 Gauss it…

Accelerator Physics · Physics 2013-01-24 I. L. Rakhno , A. I. Drozhdin , N. V. Mokhov , V. I. Sidorov , I. S. Tropin

In synchrotron machines, the beam extraction is accomplished by a combination of septa and kicker magnets which deflect the beam from an accelerator into another. Ideally the kicker field must rise/fall in between the beam bunches. However,…

The Fermilab Booster is being upgraded under the Proton Improvement Plan (PIP) to be capable of providing a proton flux of $2.25^{17}$ protons per hour. The intensity per cycle will remain at the present operational $4.3^{12}$ protons per…

Accelerator Physics · Physics 2015-11-05 K. Seiya , C. M. Bhat , D. E. Johnson , V. V. Kapin , W. A. Pellico , C. Y. Tan , R. J. Tesarek

Two barrier RF systems were fabricated, tested and installed in the Fermilab Main Injector. Each can provide 8 kV rectangular pulses (the RF barriers) at 90 kHz. When a stationary barrier is combined with a moving barrier, injected beams…

Accelerator Physics · Physics 2010-01-18 W. Chou , D. Capista , J. Griffin , K-Y. Ng , D. Wildman

We develop a configuration of radio-frequency (rf) cavities to dramatically improve the performance of slip-stacking. Slip-stacking is an accumulation technique used at Fermilab to nearly double proton intensity by maintaining two beams of…

Accelerator Physics · Physics 2016-11-23 Jeffrey Eldred , Robert Zwaska

This paper introduces a new method for stacking beams in the longitudinal phase space. It uses RF barriers to confine and compress beams in an accelerator, provided that the machine momentum acceptance is a few times larger than the…

Accelerator Physics · Physics 2007-05-23 Weiren Chou , Akira Takagi

A double kicker system which extracts the ultra-low emittance multi-bunch beam stably from ATF damping ring was developed. The performance of the system was studied comparing an orbit jitter with single kicker extraction in single bunch…

Accelerator Physics · Physics 2007-05-23 T. Imai , K. Nakai , H. Hayano , J. Urakawa , N. Terunuma

The transfer line for beam extraction from the Recycler ring to P1 line provides a way to deliver 8 GeV kinetic energy protons from the Booster to the Delivery ring, via the Recycler, using existing beam transport lines, and without the…

Accelerator Physics · Physics 2017-02-20 M. Xiao , D. Capista , P. Adams , D. Morris , M. J. Yang , K. Hazewood

It is well known that timing jitter can degrade the bit error rate (BER) of receivers that recover the clock from input data. However, timing jitter can also result in an indefinite increase in the settling time of clock recovery circuits,…

Emerging Technologies · Computer Science 2019-12-06 Naveen Kadayinti , Amitalok J. Budkuley , Maryam S. Baghini , Dinesh K. Sharma

A second harmonic RF cavity which uses perpendicularly biased garnet for frequency tuning is currently being constructed for use in the Fermilab Booster. The cavity will operate at twice the fundamental RF frequency, from ~76 - 106 MHz, and…

Fermilab is upgrading its Booster synchrotron to increase ramp rate and intensity. This is part of the Proton Improvement Plan (PIP-II) that will allow the Main Injector to achieve proton beam power of 1.2 MW within the next few years. This…

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