Kiran G. Sonnad
Cornell University
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Featured researches published by Kiran G. Sonnad.
arXiv: Accelerator Physics | 2013
J. Sikora; Robert Schwartz; Kiran G. Sonnad; Stefano De Santis; D. Alesini
In the TE wave method, microwaves are coupled into the beam-pipe and the effect of the electron cloud on these microwaves is measured. An electron cloud (EC) density can then be calculated from this measurement. There are two analysis methods currently in use. The first treats the microwaves as being transmitted from one point to another in the accelerator. The second more recent method, treats the beam-pipe as a resonant cavity. This paper will summarize the reasons for adopting the resonant TE wave analysis as well as give examples from CESRTA and DA{Phi}NE of resonant beam-pipe. The results of bead-pull bench measurements will show some possible standing wave patterns, including a cutoff mode (evanescent) where the field decreases exponentially with distance from the drive point. We will outline other recent developments in the TE wave method including VORPAL simulations of microwave resonances, as well as the simulation of transmission in the presence of both an electron cloud and magnetic fields.
arXiv: Accelerator Physics | 2013
G.F. Dugan; H.A. Williams; K. Ohmi; K. Butler; J.A. Crittenden; M. Venturini; R. L. Holtzapple; R.C. Campbell; J. Flanagan; M. C. Rendina; M. Randazzo; D.L. Kreinick; M. Pivi; R. E. Meller; J. Chu; M. Furman; N. T. Rider; Kiran G. Sonnad; M. Palmer; M. Billing; G.A. Ramirez; M. Forster
In this paper, we will describe some of the recent experimental measurements [1, 2, 3] performed at CESRTA [4], and the supporting simulations, which probe the interaction of the electron cloud with the stored beam. These experiments have been done over a wide range of beam energies, emittances, bunch currents, and fill patterns, to gather sufficient information to be able to fully characterize the beam-electron-cloud interaction and validate the simulation programs. The range of beam conditions is chosen to be as close as possible to those of the ILC damping ring, so that the validated simulation programs can be used to predict the performance of these rings with regard to electroncloud- related phenomena. Using the new simulation code Synrad3D to simulate the synchrotron radiation environment, a vacuum chamber design has been developed for the ILC damping ring which achieves the required level of photoelectron suppression. To determine the expected electron cloud density in the ring, EC buildup simulations have been done based on the simulated radiation environment and on the expected performance of the ILC damping ring chamber mitigation prescriptions. The expected density has been compared with analytical estimates of the instability threshold, to verify that the ILC damping ring vacuum chamber design is adequate to suppress the electron cloud single-bunch head-tail instability.
Journal of Instrumentation | 2016
R. L. Holtzapple; M. Billing; R.C. Campbell; G.F. Dugan; J. Flanagan; K.E. McArdle; M.I. Miller; Mark Palmer; G.A. Ramirez; Kiran G. Sonnad; M.M. Totten; S.L. Tucker; H.A. Williams
Electron cloud related emittance dilution and instabilities of bunch trains limit the performance of high intensity circular colliders. One of the key goals of the Cornell electron-positron storage ring Test Accelerator (CesrTA) research program is to improve our understanding of how the electron cloud alters the dynamics of bunches within the train. Single bunch beam diagnotics have been developed to measure the beam spectra, vertical beam size, two important dynamical effects of beams interacting with the electron cloud, for bunch trains on a turn-by-turn basis. Experiments have been performed at CesrTA to probe the interaction of the electron cloud with stored positron bunch trains. The purpose of these experiments was to characterize the dependence of beam-electron cloud interactions on the machine parameters such as bunch spacing, vertical chromaticity, and bunch current. The beam dynamics of the stored beam, in the presence of the electron cloud, was quantified using: 1) a gated beam position monitor (BPM) and spectrum analyzer to measure the bunch-by-bunch frequency spectrum of the bunch trains; 2) an x-ray beam size monitor to record the bunch-by-bunch, turn-by-turn vertical size of each bunch within the trains. In this paper we report on the observations from these experiments and analyze the effects of the electron cloud on the stability of bunches in a train under many different operational conditions.
PAC09, Vancouver, Canada, May 3-9, 2009 | 2009
J.-L. Vay; C. M. Celata; Miguel A. Furman; Marco Venturini; Kiran G. Sonnad; G. Penn; David Peter Grote
5th Int. Particle Accelerator Conf. (IPAC'14), Dresden, Germany, June 15-20, 2014 | 2014
M. Billing; Kaitlin Butler; G. Dugan; John Flanagan; M. Forster; Robert Holtzapple; Kaitlin McArdle; Mikhail Miller; Gabriel Ramirez; Nate Rider; Kiran G. Sonnad; Molly Totten; Heather Williams
arXiv: Accelerator Physics | 2013
M. Billing; J. Conway; E. E. Cowan; J.A. Crittenden; J. Lanzoni; Y. Li; C. S. Shill; J. Sikora; Kiran G. Sonnad
Archive | 2007
John R. Cary; Miguel A. Furman; Kiran G. Sonnad; Peter Stoltz; Seth A. Veitzer
arXiv: Accelerator Physics | 2015
Kiran G. Sonnad
5th International Particle Accelerator Conference, IPAC 2014 | 2014
J.A. Crittenden; M. Billing; W. Hartung; C.S. Shill; J. Sikora; Kiran G. Sonnad
Archive | 2013
J.A. Crittenden; Joe Conway; G. Dugan; M. Palmer; David Rubin; J. Shanks; Kiran G. Sonnad; Laura Boon; K. Harkay; Takuya Ishibashi; Miguel A. Furman; S. Guiducci; Mauro Pivi; Lanfa Wang