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Featured researches published by R. Fernow.


Proceedings of the 1999 Particle Accelerator Conference (Cat. No.99CH36366) | 1999

ICOOL: a simulation code for ionization cooling of muon beams

R. Fernow

Current ideas for designing a high luminosity muon collider require significant cooling of the phase space of the muon beams. The only known method that can cool the beams in a time comparable to the muon lifetime is ionization cooling. This method requires directing the particles in the beam at a large angle through a low Z absorber material in a strong focusing magnetic channel and then restoring the longitudinal momentum with an RF cavity. We have developed a new 3-D tracking code ICOOL for examining possible configurations for muon cooling. A cooling system is described in terms of a series of longitudinal regions with associated material and field properties. The tracking takes place in a coordinate system that follows a reference orbit through the system. The code takes into account decays and interactions of /spl sim/50-500 MeV/c muons in matter. Material geometry regions include cylinders and wedges. A number of analytic models are provided for describing the field configurations. Simple diagnostics are built into the code, including calculation of emittances and correlations, longitudinal traces, histograms and scatter plots. A number of auxiliary files can be generated for postprocessing analysis by the user.


Journal of Instrumentation | 2009

Accelerator design concept for future neutrino facilities

M. Apollonio; J. S. Berg; A. Blondel; A. Bogacz; S. Brooks; J.E. Campagne; D. Caspar; C. Cavata; P. Chimenti; J. Cobb; M. Dracos; R. Edgecock; I. Efthymiopoulos; A. Fabich; R. Fernow; F. Filthaut; J. Gallardo; R. Garoby; Stephen H. Geer; F. Gerigk; G. Hanson; R. Johnson; C. Johnstone; Daniel M. Kaplan; E. Keil; H. Kirk; A. Klier; A. Kurup; J. Lettry; Kenneth Long

This document summarizes the findings of the Accelerator Working Group (AWG) of the International Scoping Study (ISS) of a Future Neutrino Factory and Superbeam Facility. The work of the group took place at three plenary meetings along with three workshops, and an oral summary report was presented at the NuFact06 workshop held at UC-Irvine in August, 2006. The goal was to reach consensus on a baseline design for a Neutrino Factory complex. One aspect of this endeavor was to examine critically the advantages and disadvantages of the various Neutrino Factory schemes that have been proposed in recent years.This document summarizes the findings of the Accelerator Working Group (AWG) of the International Scoping Study (ISS) of a Future Neutrino Factory and super-beam Facility. The work of the group took place at three plenary meetings along with three workshops, and an oral summary report was presented at the NuFact06 workshop held at UC-Irvine in August, 2006. The goal was to reach consensus on a baseline design for a Neutrino Factory complex. One aspect of this endeavor was to examine critically the advantages and disadvantages of the various Neutrino Factory schemes that have been proposed in recent years.


arXiv: Accelerator Physics | 2004

NEUTRINO FACTORY AND BETA BEAM EXPERIMENTS AND DEVELOPMENT.

Carl H. Albright; V. Barger; John F. Beacom; E. Black; A. Blondel; S. A. Bogacz; S. J. Brice; S. Caspi; W. Chou; M. Cummings; R. Fernow; D. A. Finley; J. Gallardo; S. Geer; M. C. Goodman; D. A. Harris; Patrick Huber; A. Jansson; C. Johnstone; S. Kahn; Daniel M. Kaplan; H. Kirk; T. Kobilarcik; Manfred Lindner; Kirk T. McDonald; Olga Mena; D. Neuffer; V. Palladino; Robert B. Palmer; K. Paul

The long-term prospects for fully exploring three-flavor mixing in the neutrino sector depend upon an ongoing and increased investment in the appropriate accelerator R&D. Two new concepts have been proposed that would revolutionize neutrino experiments, namely the Neutrino Factory and the Beta Beam facility. These new facilities would dramatically improve our ability to test the three-flavor mixing framework, measure CP violation in the lepton sector, and perhaps determine the neutrino mass hierarchy, and, if necessary, probe extremely small values of the mixing angle {theta}{sub 13}. The stunning sensitivity that could be achieved with a Neutrino Factory is described, together with our present understanding of the corresponding sensitivity that might be achieved with a Beta Beam facility. In the Beta Beam case, additional study is required to better understand the optimum Beta Beam energy, and the achievable sensitivity. Neither a Neutrino Factory nor a Beta Beam facility could be built without significant R&D. An impressive Neutrino Factory R&D effort has been ongoing in the U.S. and elsewhere over the last few years and significant progress has been made towards optimizing the design, developing and testing the required accelerator components, and significantly reducing the cost. The recent progress is described here.


PACS2001. Proceedings of the 2001 Particle Accelerator Conference (Cat. No.01CH37268) | 2001

Target studies with BNL E951 at the AGS

H. Kirk; Kevin Brown; R. Fernow; Charles Finfrock; D. Gassner; G.A. Greene; S. Kahn; Bruce J. King; R. Prigl; Roman Samulyak; J. Scaduto; N. Simos; P. Thieberger; T. Tsang; H. Wang; Robert Weggel; Audrey Bernandon; Adrian Fabich; Jacques Lettry; H. L. Ravn; Al Zeller; David Beshears; Michael Cates; J.R. Haines; Bernie Riemer; Phil Spampinato; James Tsai; Kirk T. McDonald; Yasuo Fukui

We report initial results of exposing low-Z solid and high-Z liquid targets to 150-ns, 4/spl times/10/sup 12/ proton pulses with spot sizes on the order of 1 to 2 mm. The energy deposition density approached 100 J/g. Diagnostics included fiberoptic strain sensors on the solid target and high-speed photography of the liquid targets. This work is part of the R&D program of the Neutrino Factory and Muon Collider Collaboration.


Journal of Applied Physics | 1992

Intense electron emission due to picosecond laser‐produced plasmas in high gradient electric fields

X. J. Wang; T. Tsang; H. Kirk; T. Srinivasan-Rao; J. Fischer; K. Batchelor; P. Russell; R. Fernow

Picosecond laser pulses at a wavelength of 266 nm have been focused onto a solid metal cathode in coincidence with high gradient electric fields to produce high brightness electron beams. At power densities exceeding 109 W/cm2, a solid density plasma is formed and intense bursts of electrons are emitted from the target accompanied by macroscopic surface damage. An inferred ∼1 μC of integrated charge with an average current of ∼20 A is emitted from a radio‐frequency cavity driven at electric field gradients of ∼80 MV/m. In another experiment, where a dc extraction field of ∼6 MV/m is used, we observed an electron charge of ∼0.17 μC. Both results are compared with the Schottky effect and the Fowler–Nordheim field emission. We found that this laser‐induced intense electron emission shares many features with the explosive electron emission processes. No selective wavelength dependence is observed in the production of the intense electron emission in the dc extraction field. The integrated electrons give an ap...


ieee particle accelerator conference | 2007

A complete scheme of ionization cooling for a muon collider

Robert B. Palmer; J. S. Berg; R. Fernow; J. Gallardo; H. Kirk; Yuri Alexahin; D. Neuffer; S.A. Kahn; D. J. Summers

A complete scheme for production and cooling a muon beam for three specified muon colliders is presented. Parameters for these muon colliders are given. The scheme starts with the front end of a proposed neutrino factory that yields bunch trains of both muon signs. Emittance exchange cooling in slow helical lattices reduces the longitudinal emittance until it becomes possible to merge the trains into single bunches, one of each sign. Further cooling in all dimensions is applied to the single bunches in further slow helical lattices. Final transverse cooling to the required parameters is achieved in 50 T solenoids using high TC superconductor at 4 K. Preliminary simulations of each element are presented.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1992

Performance of the Brookhaven Photocathode RF Gun

K. Batchelor; I. Ben-Zvi; R. Fernow; J. Fischer; Alan Fisher; Juan C. Gallardo; G. Ingold; H. Kirk; K.P. Leung; Robert M. Malone; Igor Pogorelsky; T. Srinivasan-Rao; J. Rogers; T. Tsang; J. Sheehan; S. Ulc; M. Woodle; Jialin Xie; R.S. Zhang; Li-Yi Lin; Kirk T. McDonald; D.P. Russell; C.M. Hung; X.J. Wang

The Brookhaven Accelerator Test Facility (ATF) uses a photocathode rf gun to provide a high-brightness electron beam intended for FEL and laser-acceleration experiments. The rf gun consists of 1{1/2} cells driven at 2856 MHz in {pi}-mode with a maximum cathode field of 100 MV/m. To achieve long lifetimes, the photocathode development concentrates on robust metals such as copper, yttrium and samarium. We illuminate these cathodes with a 10-ps, frequency-quadrupled Nd:YAG laser. We describe the initial operation of the gun, including measurements of transverse and longitudinal emittance, quantum efficiencies, and peak current. The results are compared to models.


Physical Review Special Topics-accelerators and Beams | 2005

Ionization cooling ring for muons

Robert B. Palmer; V. Balbekov; J. S. Berg; S. B. Bracker; L. Cremaldi; R. Fernow; J. Gallardo; R. Godang; G. Hanson; Amit Klier; D. J. Summers

Practical ionization cooling rings could lead to lower cost or improved performance in neutrino factory or muon collider designs. The ring modeled here uses realistic three-dimensional fields. The performance of the ring compares favorably with the linear cooling channel used in the second U.S. Neutrino Factory Study. The normalized 6D emittance of an ideal ring is decreased by a factor of approximately 240, compared with a factor of only 15 for the linear channel. We also examine such real-world effects as windows on the absorbers and rf cavities and leaving empty lattice cells for injection and extraction. For realistic conditions the ring decreases the normalized 6D emittance by a factor of 49.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1992

Performance of a superconducting, high field subcentimeter undulator

I. Ben-Zvi; R. Fernow; Juan C. Gallardo; G. Ingold; W. Sampson; M. Woodle

A Superconducting 8.80mm wavelength undulator is under construction for the 500nm Free-Electron Laser at the Accelerator Test Facility (ATF) at Brookhaven National Laboratory. We present results on the design, construction and performance of this novel undulator structure. A field on axis of 0.51T has been measured for a 4.40mm gap, with a current 20% below the quench current. Our simple design focuses on minimizing the accumulation of errors by minimizing the numbers of parts and by using a ferromagnetic yoke. The magnetic field error is less than 0.30% rms as manufactured (without shimming). The third harmonic content is less than 0.1% of the fundamental.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1990

A microwiggler free-electron laser at the Brookhaven accelerator test facility

K. Batchelor; I. Ben-Zvi; R. Fernow; Juan C. Gallardo; H. Kirk; C. Pellegrini; A. van Steenbergen; Anup Bhowmik

Abstract We report the design and status of an FEL experiment at the Brookhaven National Laboratory Accelerator Test Facility. A 50 MeV high-brightness electron beam will be utilized for an oscillator experiment in the visible-wavelength region. The microwiggler to be used is a superferric planar undulator with a 0.88 cm period, 60 cm length and K = 0.35. The optical cavity is a 368 cm long stable resonator with broadband dielectric coated mirrors.

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H. Kirk

Brookhaven National Laboratory

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Robert B. Palmer

Brookhaven National Laboratory

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S. U. Chung

Brookhaven National Laboratory

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Juan C. Gallardo

Brookhaven National Laboratory

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J. H. Goldman

Florida State University

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V. Hagopian

Florida State University

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A. Dzierba

Indiana University Bloomington

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