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Featured researches published by S. Molloy.


Physical Review Special Topics-accelerators and Beams | 2010

Present status and first results of the final focus beam line at the KEK Accelerator Test Facility

P. Bambade; M. Alabau Pons; John Amann; D. Angal-Kalinin; R. Apsimon; S. Araki; A. Aryshev; Sha Bai; P. Bellomo; D. R. Bett; G.A. Blair; B. Bolzon; Stewart Boogert; G. Boorman; P. N. Burrows; G. Christian; P. Coe; Ben Constance; J P Delahaye; Laurence Deacon; E. Elsen; A. Faus-Golfe; Masafumi Fukuda; J. Gao; N. Geffroy; E. Gianfelice-Wendt; H. Guler; Hitoshi Hayano; A. Heo; Y. Honda

ATF2 is a final-focus test beam line which aims to focus the low emittance beam from the ATF damping ring to a vertical size of about 37 nm and to demonstrate nanometer level beam stability. Several advanced beam diagnostics and feedback tools are used. In December 2008, construction and installation were completed and beam commissioning started, supported by an international team of Asian, European, and U. S. scientists. The present status and first results are described.


Physical Review Special Topics-accelerators and Beams | 2012

Cavity beam position monitor system for the Accelerator Test Facility 2

Youngim Kim; Robert Ainsworth; A. Aryshev; S. Boogert; G. Boorman; J. Frisch; A. Heo; Y. Honda; W. H. Hwang; Jung-Yun Huang; Eun-Joo Kim; S. H. Kim; A. Lyapin; T. Naito; Justin May; D. McCormick; R. E. Mellor; S. Molloy; J. Nelson; S. J. Park; Y. J. Park; M. Ross; S. Shin; C. Swinson; T.I. Smith; Nobuhiro Terunuma; T. Tauchi; J. Urakawa; Gannon White

The Accelerator Test Facility 2 (ATF2) is a scaled demonstrator system for final focus beam lines of linear high energy colliders. This paper describes the high resolution cavity beam position monitor (BPM) system, which is a part of the ATF2 diagnostics. Two types of cavity BPMs are used, C-band operating at 6.423 GHz, and S-band at 2.888 GHz with an increased beam aperture. The cavities, electronics, and digital processing are described. The resolution of the C-band system with attenuators was determined to be approximately 250 nm and 1 � m for the S-band system. Without attenuation the best recorded C-band cavity resolution was 27 nm.


ieee particle accelerator conference | 2005

A Test Facility for the International Linear Collider, at SLAC End Station a for Prototypes of Beam Delivery and IR Components

M. Woods; Roger Erickson; J. Frisch; C. Hast; R.K. Jobe; L. Keller; T. Markiewicz; T. Maruyama; D. McCormick; J. Nelson; Nan Phinney; T. Raubenheimer; Marc Ross; Andrei Seryi; S.R. Smith; Z. Szalata; P. Tenenbaum; M. Woodley; D. Angal-Kalinin; C. Beard; C. Densham; J. Greenhalgh; F. Jackson; A. Kalinin; F. Zimmermann; Igor Zagorodnov; Y. Sugimoto; S. Walston; J. Smith; A. Sopczak

The SLAC Linac can deliver damped bunches with ILC parameters for bunch charge and bunch length to End Station A. A 10Hz beam at 28.5 GeV energy can be delivered there, parasitic with PEP-II operation. We plan to use this facility to test prototype components of the Beam Delivery System and Interaction Region. We discuss our plans for this ILC Test Facility and preparations for carrying out experiments related to collimator wakefields and energy spectrometers. We also plan an interaction region mockup to investigate effects from backgrounds and beam-induced electromagnetic interference.


Measurement Science and Technology | 2007

High precision SC cavity alignment measurements with higher order modes

S. Molloy; Josef Frisch; D. McCormick; Justin May; Marc Ross; T.I. Smith; N. Eddy; S. Nagaitsev; Ron Rechenmacher; Luciano Piccoli; Nicoleta Baboi; Olaf Hensler; Lyudvig Petrosyan; Olivier Napoly; Rita Paparella; Claire Simon

Experiments at the FLASH linac at DESY have demonstrated that the higher order modes (HOMs) induced in superconducting cavities can be used to provide a variety of beam and cavity diagnostics. The centers of the cavities can be determined from the beam orbit which produces minimum power in the dipole HOM modes. The phase and amplitude of the dipole modes can be used as a high resolution beam position monitor. For most superconducting accelerators, the existing HOM couplers provide the necessary signals, and the downmix and digitizing electronics are straightforward, similar to those for a conventional BPM.


ieee particle accelerator conference | 2007

Picosecond bunch length and energy-z correlation measurements at SLAC's A-line and end station A

S. Molloy; P. Emma; J. Frisch; R. Iverson; Marc Ross; D. McCormick; M. Woods; S. Walston; V. Blackmore

We report on measurements of picosecond bunch lengths and the energy-z correlation of the bunch with a high energy electron test beam to the A-line and end station A (ESA) facilities at SLAC. The bunch length and the energy-Z correlation of the bunch are measured at the end of the linac using a synchrotron light monitor diagnostic at a high dispersion point in the A-line and a transverse RF deflecting cavity at the end of the linac. Measurements of the bunch length in ESA were made using high frequency diodes (up to 100 GHz) and pyroelectric detectors at a ceramic gap in the beamline. Modelling of the beams longitudinal phase space through the linac and A-line to ESA is done using the 2-dimensional tracking program LiTrack, and LiTrack simulation results are compared with data. High frequency diode and pyroelectric detectors are planned to be used as part of a bunch length feedback system for the LCLS EEL at SLAC. The LCLS also plans precise bunch length and energy-Z correlation measurements using transverse RF deflecting cavities.


Journal Name: AIP Conf.Proc.868:313-324,2006; Conference: Presented at 12th Beam Instrumentation Workshop (BIW06), Fermilab, Batavia, Illinois, 1-4 May 2006 | 2006

Electronics and Algorithms for HOM Based Beam Diagnostics

Josef Frisch; Nicoleta Baboi; N. Eddy; S. Nagaitsev; Olaf Hensler; D. McCormick; Justin May; S. Molloy; Olivier Napoly; Rita Paparella; Lyudvig Petrosyan; Marc Ross; Claire Simon; T.I. Smith

The signals from the Higher Order Mode (HOM) ports on superconducting cavities can be used as beam position monitors and to do survey structure alignment. A HOM-based diagnostic system has been installed to instrument both couplers on each of the 40 cryogenic accelerating structures in the DESY TTF2 Linac. The electronics uses a single stage down conversion form the 1.7 GHz HOM spectral line to a 20MHz IF which has been digitized. The electronics is based on low cost surface mount components suitable for large scale production. The analysis of the HOM data is based on Singular Value Decomposition. The response of the OM modes is calibrated using conventional BPMs.


ieee particle accelerator conference | 2007

Electromagnetic background tests for the ILC interaction-point feedback system

Philip Burrows; G. Christian; C. Clarke; B. Constance; Hamid Dabiri Khah; T. Hartin; C. Perry; C. Swinson; A. Kalinin; R. Arnold; S. Molloy; S. Smith; Gannon White; M. Woods

We present results obtained with the T-488 experiment at SLAC Endstation A (ESA). A material model of the ILC extraction-line design was assembled and installed in ESA. The module includes materials representing the mask, beamline calorimeter, and first extraction quadrupole, encompassing a stripline interaction-point feedback system beam position monitor (BPM). The SLAC high-energy electron beam was used to irradiate the module in order to mimic the electromagnetic (EM) backgrounds expected in the ILC interaction region. The impact upon the performance of the feedback BPM was measured, and compared with detailed simulations of its expected response.


ieee particle accelerator conference | 2007

Simulation of ILC feedback bpm signals in an intense background environment

A. F. Hartin; Philip Burrows; G. Christian; C. Clarke; B. Constance; H. Khan; C. Perry; C. Swinson; R. Arnold; S. Molloy; S. Smith; Glen White; M. Woods; A. Kalinin

Experiment T-488 at SLAC, End station A recorded distorted BPM voltage signals and an accurate simulation of these signals was performed. Geant simulations provided the energy and momentum spectrum of the incident spray and secondary emissions, and a method via image charges was used to convert particle momenta and number density into BPM stripline currents. Good agreement was achieved between simulated and measured signals. Further simulation of experiment T-488 with incident beam on axis and impinging on a thin radiator predicted minimal impact due to secondary emission. By extension to worst case conditions expected at the ILC, simulations showed that background hits on BPM striplines would have a negligible impact on the accuracy of beam position measurements and hence the operation of the FONT feedback system.


ieee particle accelerator conference | 2005

Proposal of the Next Incarnation of Accelerator Test Facility at KEK for the International Linear Collider

Shunsuke Araki; H. Hayano; Yu Higashi; Y. Honda; Kenji Kanazawa; Koichi Kubo; Tsuyoshi Kume; M. Kuriki; Sho Kuroda; M. Masuzawa; Tomoyuki Naito; T. Okugi; R. Sugahara; Tatsuro Takahashi; T. Tauchi; Nobuhiro Terunuma; N. Toge; J. Urakawa; V. Vogel; Hiroshi Yamaoka; K. Yokoya; J. Gao; Wenxin Liu; Guanhong Pei; Jiacheng Wang; B. Grishanov; P. Logachev; F. Podgorny; Valery I. Telnov; D. Angal-Kalinin

To reach design luminosity, the International Linear Collider (ILC) must be able to create and reliably maintain nanometer size beams. The ATF damping ring is the unique facility where ILC emittances are possible. In this paper we present and evaluate the proposal to create a final focus facility at the ATF which, using compact final focus optics and an ILC-like bunch train, would be capable of achieving 37 nm beam size. Such a facility would enable the development of beam diagnostics and tuning methods, as well as the training of young accelerator physicists.


ieee particle accelerator conference | 2007

Investigations of the wideband spectrum of higher order modes measured on tesla-style cavities at the FLASH LINAC

S. Molloy; C. Adolphsen; K. Bane; J. Frisch; Z. Li; J. May; D. McCormick; T. Smith; N. Baboi; N. Eddy; Luciano Piccoli; R. Rechenmacher; R. Jones

Higher Order Modes (HOMs) excited by the passage of the beam through an accelerating cavity depend on the properties of both the cavity and the beam. It is possible, therefore, to draw conclusions on the inner geometry of the cavities based on observations of the properties of the HOM spectrum. A data acquisition system based on two 20 GS/s, 6 GHz scopes has been set up at the FLASH facility, DESY, in order to measure a significant fraction of the HOM spectrum predicted to be generated by the TESLA cavities used for the acceleration of its beam. The HOMs from a particular cavity at FLASH were measured under a range of known beam conditions. The dipole modes have been identified in the data. 3D simulations of different manufacturing errors have been made, and it has been shown that these simulations can predict the measured modes.

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D. McCormick

SLAC National Accelerator Laboratory

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Marc Ross

SLAC National Accelerator Laboratory

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