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Featured researches published by M. Minty.


arXiv: Accelerator Physics | 2013

Status of head-on beam-beam compensation in RHIC

W. Fischer; Zeynep Altinbas; M. Anerella; M. Blaskiewicz; D. Bruno; M. Costanzo; W.C.Dawson; D. Gassner; X. Gu; R. Gupta; K. Hamdi; J. Hock; L.T. Hoff; R. Hulsart; A. Jain; R. Lambiase; Y. Luo; M. Mapes; A. Marone; R. Michnoff; Toby Miller; M. Minty; C. Montag; J. Muratore; S. Nemesure; D. Phillips; A. Pikin; S.R.Plate; P. Rosas; L. Snydstrup

In polarized proton operation, the performance of the Relativistic Heavy Ion Collider (RHIC) is limited by the head-on beam-beam effect. To overcome this limitation, two electron lenses are under commissioning. We give an overview of head-on beam-beam compensation in general and in the specific design for RHIC, which is based on electron lenses. The status of installation and commissioning are presented along with plans for the future.


Optics Express | 2017

Generation of 180 W average green power from a frequency-doubled picosecond rod fiber amplifier

Zhi Zhao; B. Sheehy; M. Minty

We report on the generation of 180 W average green power from a frequency-doubled picosecond rod fiber amplifier. In an Yb-doped fiber master-oscillator-power-amplifier system, 2.3-ps 704 MHz pulses are first amplified in small-core fibers and then in large-mode-area rod fibers to produce 270 W average infrared power with a high polarization extinction ratio and diffraction-limited beam quality. By carrying out frequency doubling in a lithium triborate (LBO) crystal, 180 W average green power is generated. To the best of our knowledge, this is the highest average green power achieved in fiber-based laser systems.


Archive | 2018

Proposed BPM-Based Bunch Crabbing Angle Monitor

P. Thieberger; M. Minty; C. Montag

A tilted (i.e. with different transverse displacements of the bunch head and tail) bunch traversing a button beam profile monitor will produce signals on opposite pickup electrodes that will have different degrees of distortion depending on the tilt angle. In particular, the zero-crossing time difference between the two signals will be approximately proportional to the tilt angle. We perform simulations to study this effect as a possible diagnostic tool for measuring the crabbing angles in a future electron-ion collider.


Archive | 2018

ER@CEBAF, a 7 GeV, 5-Pass, Energy Recovery Experiment

Francois Méot; P. Thieberger; Michael Tiefenback; M. Minty; Chase Dubbé; Wencan Xu; Chen Xu; C. Liu; Michael Spata; David Douglas; Vadim Ptitsyn; Alex Bogacz; Michael Bevins; T. Satogata; Ilan Ben-Zvi; Christopher Tennant; Y. Hao; Guillaume Robert-Demolaize; Nicholaos Tsoupas; Yves Roblin; T. Roser; Tim Michalski

A multiple-pass, high-energy ERL experiment at the JLab CEBAF will be instrumental in providing necessary information and technology testing for a number of possible future applications and facilities such as Linac-Ring based colliders, which have been designed at BNL (eRHIC) and CERN (LHeC), and also drivers for high-energy FELs and 4th GLS. ER@CEBAF is aimed at investigating 6D optics and beam dynamics issues in ERLs, such as synchrotron radiation effects, emittance preservation, stability, beam losses, multiple-pass orbit control/correction, multiple-pass beam dynamics in the presence of cavity HOMs, BBU and other halo studies, handling of large (SR induced) momentum spread bunches, and development of multiple-beam diagnostics instrumentation. Figure 1: 12 GeV CEBAF recirculating linac. Location of chicane and dump line for ER@CEBAF. Since it was launched 2+ years ago, the project has progressed in defining the necessary modifications to CEBAF (Fig. 1, Tab. 1, 2), including a 4-dipole phase chicane in recirculation Arc A, beam extraction and a dump line at the end of the south linac, and additional dedicated multiplebeam diagnostics. This equipment can remain in place to Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy, † and by Jefferson Science Associates, LLC under Contract No. DEAC05-06OR23177 with the U.S. Department of Energy. ‡ Spokesperson. [email protected]; [email protected] Table 1: Machine/Lattice Parameters of ER@CEBAF fRF 1497 MHz RF frequency Elinac 700 MeV Gain per linac (baseline) Einj 79 MeV = Elinac × 123/1090 φFODO 60 deg Per cell, at first NL pass and last SL pass M56 <90 cm Compression, Arc A Extraction 8 deg Angle to dump line


7th Int. Particle Accelerator Conf. (IPAC'16), Busan, Korea, May 8-13, 2016 | 2016

RHIC Performance with Stochastic Cooling for Ions and Head-on Beam-beam Compensation for Protons

W. Fischer; James Alessi; Zeynep Altinbas; Elke Aschenauer; Grigor Atoian; M. Bai; Edward Beebe; Severino Binello; Ian Blackler; Michael Blaskiewicz; Joseph Brennan; Kevin Brown; D. Bruno; R. Connolly; Michael Costanzo; T. D'Ottavio; Yann Dutheil; Alexei Fedotov; C. Gardner; David Gassner; X. Gu; Caitlin Harper; M. Harvey; T. Hayes; Jon Hock; Haixin Huang; R. Hulsart; James Jamilkowski; Takeshi Kanesue; Nicholas Kling

The Relativistic Heavy Ion Collider (RHIC) has two main operating modes with heavy ions and polarized protons respectively. In addition to a continuous increase in the bunch intensity in all modes, two major new systems were completed recently mitigating the main luminosity limit and leading to significant performance improvements. For heavy ion operation stochastic cooling mitigates the effects of intrabeam scattering, and for polarized proton operation head-on beam-beam compensation mitigates the beam-beam effect. We present the performance increases with these upgrades to date, as well as an overview of all operating modes past and planned.


7th Int. Particle Accelerator Conf. (IPAC'16), Busan, Korea, May 8-13, 2016 | 2016

Record Performance of SRF Gun with CsK2Sb Photocathode

I.V. Pinayev; Zeynep Altinbas; Sergey Belomestnykh; Ilan Ben-Zvi; Kevin M. Brown; Jean Clifford Brutus; Anthony Curcio; Anthony Di Lieto; Charles Folz; D. Gassner; M. Harvey; Thomas Hayes; R. Hulsart; James Jamilkowski; Yichao Jing; D. Kayran; Robert Kellermann; Robert Lambiase; Vladimir N. Litvinenko; G. Mahler; Michael Mapes; W. Meng; K. Mernick; R. Michnoff; Toby Miller; M. Minty; Geetha Narayan; Paul Orfin; David J. Phillips; T. Rao

High-gradient CW photo-injectors operating at high accelerating gradients promise to revolutionize many sciences and applications. They can establish the basis for super-bright monochromatic X-ray and gamma-ray sources, high luminosity hadron colliders, nuclearwaste transmutation or a new generation of microchip production. In this paper we report on our operation of a superconducting RF electron gun with a record-high accelerating gradient at the CsK2Sb photocathode (i.e. ~ 20 MV/m) generating a record-high bunch charge (i.e., 2 nC). We briefly describe the system and then detail our experimental results. INTRODUCTION The coherent electron cooling experiment (CeC PoP) [1, 2] is expected to demonstrate cooling of a single hadron bunch in RHIC. A superconducting RF gun operating at 112 MHz frequencies generates the electron beam. 500MHz normal conducting cavities provide energy chirp for ballistic compression of the beam. 704-MHz superconducting cavity will accelerate beam to the final energy. The electron beam merges with the hadron beam and after cooling process is steered to a dump. The FEL-like structure enhances the electron-hadron interaction. The electron beam parameters are shown in the Table 1. Table 1: Parameters of the Electron Beam


Journal of Physics: Conference Series | 2011

Observation of snake resonances at Relativistic Heavy Ion Collider

M. Bai; L. Ahrens; I G Alekseev; J. Alessi; E. D. Courant; A. Drees; W. Fischer; C. Gardner; R Gill; J. W. Glenn; H. Huang; Vladimir N. Litvinenko; A. Luccio; Y. Luo; F. Pilat; W. W. MacKay; Y. I. Makdisi; A. Marusic; M. Minty; C. Montag; V. Ptitsyn; T. Roser; D Svirida; T. Satogata; S. Tepikian; D. Trbojevic; N. Tsoupas; Anatoli Zelenski; K. Zeno; S.Y. Zhang

The Siberian snakes are powerful tools in preserving polarization in high energy accelerators has been demonstrated at the Brookhaven Relativistic Heavy Ion Collider (RHIC). Equipped with two full Siberian snakes in each ring, polarization is preserved during acceleration from injection to 100 GeV. However, the Siberian snakes also introduce a new set of depolarization resonances, i.e. snake resonances as first discoverd by Lee and Tepikian [1]. The intrinsic spin resonances above 100 GeV are about a factor of two stronger than those below 100 GeV which raises the challenge to preserve the polarization up to 250 GeV. In 2009, polarized protons collided for the first time at the RHIC design store energy of 250 GeV. This paper presents the experimental measurements of snake resonances at RHIC. The plan for avoiding these resonanances is also presented.


arXiv: Accelerator Physics | 2014

eRHIC Design Study: An Electron-Ion Collider at BNL

E. C. Aschenauer; G. McIntyre; E. Wang; O. Tchoubar; L. Zheng; J. Tuozzolo; K. Boyle; E. Sichtermann; B. Parker; C. Brutus; M. Stratmann; A. Fedotov; T. Ullrich; A. Kiselev; Y. Hao; Baker; Wencan Xu; S. Fazio; D. Kayran; T. Burton; Qiong Wu; Stephen Brooks; M.A.C. Lamont; Toby Miller; I. Ben-Zvi; I.V. Pinayev; T. Toll; J. Skaritka; G. Wang; M. Minty


international free electron laser conference | 2011

Proof-of-principle experiment for FEL-based coherent electron cooling

Vladimir N. Litvinenko; Sergei Belomestnykh; I. Ben-Zvi; Jean Clifford Brutus; A. Fedotov; Y. Hao; D. Kayran; G. Mahler; A. Marusic; W. Meng; G. McIntyre; M. Minty; Vadim Ptitsyn; I.V. Pinayev; T. Rao; T. Roser; B. Sheehy; S. Tepikian; Yatming Than; Dejan Trbojevic; J. Tuozzolo; G. Wang; V. Yakimenko; Mathew Poelker; A. Hutton; Geoffrey Kraft; Robert Rimmer; David L. Bruhwiler; Dan T. Abell; Chet Nieter


Presented at | 2010

Global orbit feedback at RHIC

M. Minty; R. Hulsart; A. Marusic; R. Michnoff; Vadim Ptitsyn; G. Robert-Demolaize; T. Satogata

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W. Fischer

Brookhaven National Laboratory

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C. Liu

Brookhaven National Laboratory

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D. Gassner

Brookhaven National Laboratory

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A. Marusic

Brookhaven National Laboratory

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R. Hulsart

Brookhaven National Laboratory

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R. Michnoff

Brookhaven National Laboratory

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Y. Luo

Brookhaven National Laboratory

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K. Mernick

Brookhaven National Laboratory

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Y. Hao

Brookhaven National Laboratory

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P. Thieberger

Brookhaven National Laboratory

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