Use of ionization friction in the storage of heavy particles

Ado, Yu.M.; Balbekov, V.

doi:10.1007/bf01123390

Cited by 24 publications

(20 citation statements)

References 2 publications

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“…The magnetic energy stored in the gap is minimized by reducing its size. Cool muons [6] with low beam emittance allow this. Stored energy goes as B 2 /2µ.…”

Section: Introductionmentioning

confidence: 99%

“…Skin Depth = δ = ρ / π f µ 0 = 1.8 × 10 −8 / π 4600 µ 0 = 0.97mm (6) Now calculate the dissipation due to eddy currents in this .25 mm wide conductor, which will consist of transposed strands to reduce this loss [22,12]. To get an idea, take the maximum B-field during a cycle to be that generated by a 0.025m radius conductor carrying 26000 amps.…”

Section: Combined Function Magnetsmentioning

confidence: 99%

See 1 more Smart Citation

Muon acceleration with a very fast ramping synchrotron for a neutrino factory

Summers

Berg

Garren

et al. 2003

J. Phys. G: Nucl. Part. Phys.

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Abstract. A 4600 Hz fast ramping synchrotron is explored as an economical way of accelerating muons from 4 to 20 GeV/c for a neutrino factory. Eddy current losses are minimized by the low machine duty cycle plus thin grain oriented silicon steel laminations and thin copper wires. Combined function magnets with high gradients alternating within single magnets form the lattice we describe. Muon survival is 83%.

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“…The magnetic energy stored in the gap is minimized by reducing its size. Cool muons [6] with low beam emittance allow this. Stored energy goes as B 2 /2µ.…”

Section: Introductionmentioning

confidence: 99%

Section: Combined Function Magnetsmentioning

confidence: 99%

Muon acceleration with a very fast ramping synchrotron for a neutrino factory

Summers

Berg

Garren

et al. 2003

J. Phys. G: Nucl. Part. Phys.

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show abstract

“…In this case the 6D phase space is reduced by approximately a factor of 10 6 , while with stacking the phase space density [6,7] is increased by a factor of 10 10 . The technique of ionization cooling is proposed for the m 1 m 2 collider [8][9][10][11]. This technique is uniquely applicable to muons because of their minimal interaction with matter.…”

Section: Introductionmentioning

confidence: 99%

“…Conventional cooling techniques (stochastic cooling [56] and electron cooling [16]) take too long. The technique proposed for cooling muons is called ionization cooling [8,10,11], and will be discussed in detail in Sec. V. Briefly, the muons traverse some material in which they lose both longitudinal and transverse momentum by ionization losses (dE͞dx).…”

Section: Introductionmentioning

confidence: 99%

Status of muon collider research and development and future plans

Ankenbrandt¹,

Ataç²,

Autin³

et al. 1999

Phys. Rev. ST Accel. Beams

293

190

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The status of the research on muon colliders is discussed and plans are outlined for future theoretical and experimental studies. Besides work on the parameters of a 3-4 and 0.5 TeV center-of-mass (COM) energy collider, many studies are now concentrating on a machine near 0.1 TeV (COM) that could be a factory for the s-channel production of Higgs particles. We discuss the research on the various components in such muon colliders, starting from the proton accelerator needed to generate pions from 1098-4402͞99͞2(8)͞081001(73)$15.00 © 1999 The American Physical Society 081001-1 PRST-AB 2 CHARLES M. ANKENBRANDT et al. 081001 (1999) a heavy-Z target and proceeding through the phase rotation and decay (p ! m n m ) channel, muon cooling, acceleration, storage in a collider ring, and the collider detector. We also present theoretical and experimental R&D plans for the next several years that should lead to a better understanding of the design and feasibility issues for all of the components. This report is an update of the progress on the research and development since the feasibility study of muon colliders presented at the Snowmass '96

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“…Established (electron, stochastic, and laser) beam-cooling methods take minutes to hours and so are ineffective on the microsecond timescale of the muon lifetime. However, the muon's penetrating character enables rapid cooling via ionization energy loss [32,33]. At sufficiently high energy (e.g., a Higgs Factory or higher-energy muon collider), optical stochastic cooling [34,35] can also be considered and may enable higher luminosity or reduced energy spread.…”

Section: Muon Coolingmentioning

confidence: 99%

Muon colliders and neutrino factories

Kaplan¹,

collaborations²

2015

EPJ Web of Conferences

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Abstract. Muon colliders and neutrino factories are attractive options for future facilities aimed at achieving the highest lepton-antilepton collision energies and precision measurements of Higgs boson and neutrino mixing matrix parameters. The facility performance and cost depend on how well a beam of muons can be cooled. Recent progress in muon cooling design studies and prototype tests nourishes the hope that such facilities could be built starting in the coming decade. The status of the key technologies and their various demonstration experiments is summarized. Prospects "post-P5" are also discussed.

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Use of ionization friction in the storage of heavy particles

Cited by 24 publications

References 2 publications

Muon acceleration with a very fast ramping synchrotron for a neutrino factory

Muon acceleration with a very fast ramping synchrotron for a neutrino factory

Status of muon collider research and development and future plans

Muon colliders and neutrino factories

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