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Record W2558460697

Design and test of the triple-harmonic buncher for the NSCL reaccelerator

2008· article· en· W2558460697 on OpenAlexaboutno aff
Qiang Zhao, V. Andreev, John Brandon, Guillaume Machicoane, F. Marti, Jorge Oliva, J. Ottarson, John J. Vincent

Bibliographic record

Venuenot available
Typearticle
Languageen
FieldEngineering
TopicParticle accelerators and beam dynamics
Canadian institutionsnot available
Fundersnot available
KeywordsCyclotronRadio-frequency quadrupoleThermal emittanceLinear particle acceleratorResonatorPhysicsHarmonicBeam (structure)Nuclear physicsOpticsElectronAcoustics
DOInot available

Abstract

fetched live from OpenAlex

A unique triple-harmonic buncher operating at the fundamental frequency of 80.5 MHz upstream the Radio Frequency Quadrupole (RFQ) linac has been designed, manufactured and tested at the National Superconducting Cyclotron Laboratory (NSCL) to meet the requirement of a small output longitudinal beam emittance from the reaccelerator. The buncher consists of two coaxial resonators with a single gridded gap. One cavity provides both the fundamental and the third harmonic simultaneously with λ/4 and 3λ/4 modes respectively, while the other provides the second harmonic in λ/4 mode. This buncher combines the advantages of using high quality factor resonator and only a pair of grids. Details on design considerations, electromagnetic simulations, and primary test results are presented. INTRODUCTION The National Superconducting Cyclotron Laboratory (NSCL) at Michigan State University is developing a facility named ReA3 to demonstrate the technical feasibility and performance characteristics for stopping and reaccelerating rare-isotope beams, as an important step towards a next-generation rare-isotope facility in the United States [1]. Beams of rare isotopes will be produced and separated in-flight at the NSCL Coupled Cyclotron Facility and subsequently stopped by a novel gas stopper, breeded by a state-of-the-art electron beam ion trap based charge-breeder, and reaccelerated by a modern linear accelerator. The linac consists of a low energy beam transport line, a cw radio-frequency quadrupole, a quarter wave resonator based superconducting linac, and a high energy beam transport line [2]. ReA3 will delivery various exotic beams with charge-to-mass ratios (Q/A) of 0.2 – 0.4 and variable energies of about 0.3 to 3 MeV/u. Nuclear experimental programs require a beam on target with an energy spread of ~1 keV/u and a bunch length of ~1 ns simultaneously. Therefore, a longitudinal beam emittance of less than 0.3 π·ns·keV/u from ReA3 is demanded. Since the intensities of the rare-isotope beams will be low, the scheme of using an external multiharmonic buncher upstream of the RFQ has been adopted to produce a small longitudinal emittance beam from RFQ with high bunching efficiency [3-6]. A unique triple harmonic buncher using two high quality factor resonators with one pair of grids has been designed, fabricated and tested at NSCL for this application. DESIGN CONSIDERATIONS The buncher is designed to operate with three harmonics, a fundamental frequency of 80.5 MHz and two additional harmonics of 161 and 241.5 MHz, respectively. The fundamental frequency, same as that of the downstream RFQ and superconducting cavities, is mainly determined by the small longitudinal beam emittance requirement. Since beams from the charge breeder will have a larger intrinsic energy spread (e.g. ΔE ~ ±25eV/u for Q/A = 0.25), the beam micro-bunch frequency should not be lower than ~80 MHz, otherwise the longitudinal emittance of the bunched beam will be too large to achieve the required time and energy resolution on target. Considering the higher bunching efficiency and lower output longitudinal emittance needed, a total of three harmonics are chosen for the operation of the buncher [6]. A high quality factor resonator was proposed, which needs a lower power amplifier to drive it. This buncher consists of two coaxial cavities, as shown in Fig. 1. One cavity provides both the fundamental and the third harmonics. The other cavity provides the second harmonic with a λ/4 mode. The dual frequency cavity will operate simultaneously at the λ/4 and 3λ/4 modes, as was done at PIAVE in Legnaro [5]. The buncher bunches beams with a nominal relativistic velocity β = 0.00507 (beam energy of 12keV/u), so the βλ is small especially for harmonics. For example, βλ = 9.4 mm for second harmonic. On the other hand, the beam diameter is about 30mm at the buncher position in order to match it into RFQ. Therefore gridded electrode tubes are necessary to achieve uniform field distributions and thus satisfactory transit time factors. We proposed to design the buncher in such a way that all three harmonics are applied in one single gridded gap. This configuration with only one pair of grids minimizes the beam losses on grids and makes the buncher longitudinally more compact as well. Figure 1: Triple harmonic buncher with two coaxial resonators and a single gridded gap: design drawing (top), photograph (bottom). ________________________________________ *Work supported by Michigan State University. zhao@nscl.msu.edu THP069 Proceedings of LINAC08, Victoria, BC, Canada

Fetched live from OpenAlex and de-inverted. Abstracts are not stored in this database: the inverted indexes are 8.6 GB of the frame’s 9.3 GB of text, and the host has 13 GB free.

How this classification was reachedexpand

Full frame machine prediction

Teacher imitation

Not calibrated prevalence, not ground truth. Human validation pending. The Gemma side is a direct model label for every work in the frame, read from the title-only record. The Codex side is a classifier learned from the 10,348 direct Codex labels and calibrated to design-weighted sample rates; fields without enough sample support carry no Codex call. Candidate is the union of the two sides; consensus is their intersection. These outputs are machine_predicted_unvalidated and are not human labels.

metaresearch head score (Codex)0.001
metaresearch head score (Gemma)0.001
Version: metacan-v3-hybrid-931329e0061cValidation status: machine_predicted_unvalidated
Candidate categoriesnone
Consensus categoriesnone
DomainCandidate signal: none · Consensus signal: none
Study designCandidate signal: Bench or experimental · Consensus signal: Bench or experimental
GenreCandidate signal: Empirical · Consensus signal: Empirical
Teacher disagreement score0.002
Threshold uncertainty score0.009

Distilled classifier scores by category (both heads)

CategoryCodexGemma
Metaresearch0.0010.001
Meta-epidemiology (narrow)0.0000.000
Meta-epidemiology (broad)0.0000.000
Bibliometrics0.0000.000
Science and technology studies0.0000.000
Scholarly communication0.0000.000
Open science0.0010.000
Research integrity0.0010.000
Insufficient payload (model declined to judge)0.0020.001

Machine scores (provisional)

The two teacher heads of the student model, read on this work. A score orders the frame for review; it never asserts a category, and the validation status ships verbatim with every row.

Baseline scores from an immature model (maturity gate not passed, 7 training rounds). Scores rank; they never assert a category.

Opus teacher head0.036
GPT teacher head0.222
Teacher spread0.187 · how far apart the two teachers sit on this one work
Validation statusscore_only:v0-immature-baseline · verbatim from the scoring run: score_only means the number may rank works, and no category label ships from it

Classification

machine, unvalidated

Machine predicted; a candidate call from one source (direct Gemma or distilled Codex), not a consensus.

The models applied no category: nothing in the taxonomy fit this work.
Study designBench or experimental
Domainnot available
GenreEmpirical

How this classification was reached, model by model and score by score, is at the end of the page under "How this classification was reached".

Quick stats

Citations5
Published2008
Admission routes1
Has abstractyes

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