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Dive into the research topics where M. Ellison is active.

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Featured researches published by M. Ellison.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1995

Effects of rf voltage modulation on particle motion

D. Li; M. Ball; B. Brabson; J. Budnick; D.D. Caussyn; A.W. Chao; V. Derenchuk; S. Dutt; G. East; M. Ellison; D. Friesel; B. Hamilton; H. Huang; W.P. Jones; S.Y. Lee; J.Y. Liu; M.G. Minty; K.Y. Ng; X. Pei; A. Riabko; T. Sloan; M. Syphers; Y. Wang; Y. Yan; P.L. Zhang

Abstract The effects of rf voltage modulation on synchrotron motion were studied experimentally. The experimental data revealed the resonance islands generated by the rf voltage modulation. With electron cooling, beam particles were observed to damp to the basins of these resonance islands or attractors, which were observed to rotate about the origin of the phase space at a half of the modulation frequency. The measured amplitude of the attractors as a function of the modulation frequency agreed very well with the theoretical prediction. The Poincare maps in the resonance rotating frame were obtained from the experimental data and compared with tori of the Hamiltonian flow. Based on our theoretical formulation, slow beam extraction using rf voltage modulation and a bent crystal are also studied.


Proceedings Particle Accelerator Conference | 1995

The Indiana University Cooler injection synchrotron RF cavity

A. Pei; M. Ellison; D. Friesel; D. Jenner; Xiaoshen Kang; S.Y. Lee; D. Li; J.Y. Liu; A. Riabko; L. Wang; K. Hedblom

A small 2.2 Tesla-meter booster synchrotron is under construction at the Indiana University Cyclotron Facility to boost polarized beam performance in the electron cooled Indiana University Cooler Synchrotron. Polarized light proton or deuteron beam from a high intensity polarized ion source will be preaccelerated to 7 and 6 MeV respectively by an RFQ/DTL accelerator. The beams are then debunched to reduce the energy spread and strip-injected into the booster synchrotron. The booster RF system must accomplish the tasks of beam capture and acceleration. At the end of the acceleration cycle, the beam phase needs to be aligned to the Cooler synchrotron RF for bucket-to-bucket beam transfer. A single RF cavity in the ring will provide the necessary RF field to accomplish the above tasks.


international conference on particle accelerators | 1993

Experimental results of the betatron sum resonance

Y. Wang; M. Ball; B. Brabson; J. Budnick; D.D. Caussyn; A.W. Chao; J. Collins; V. Derenchuk; S. Dutt; G. East; M. Ellison; D. Friesel; B. Hamilton; H. Huang; W.P. Jones; S.Y. Lee; D. Li; M.G. Minty; S. Nagaitsev; K.Y. Ng; X. Pei; T. Sloan; M. Syphers; L. Teng; Y.T. Yan; P.L. Zhang

The experimental observations of motion near the betatron sum resonance, /spl nusub x/+2/spl nusub z/=13, are presented. A fast quadrupole (Panofsky-style ferrite picture-frame magnet with 8 pulsed power supplies) producing a betatron tune shift of the order of 0.03 at rise time of 1 /spl mu/s was used. This quadrupole was used to produce betatron tunes which jumped past and then crossed back through a betatron sum resonance line. The beam response as function of initial betatron amplitudes were recorded turn by turn. The correlated growth of the action variables, J/sub x/ and J/sub z/, was observed. The phase space plots in the resonance frame reveal the features of particle motion near the nonlinear sum resonance region.<<ETX>>


Proceedings Particle Accelerator Conference | 1995

Space charge effects and intensity limits of electron-cooled bunched beams

S. Nagaitsev; T. Ellison; M. Ball; V. Derenchuk; G. East; M. Ellison; B. Hamilton; P. Schwandt

For stripping injection of proton beams in the IUCF Cooler, electron cooling permits us to accumulate beam currents several times higher than what can be obtained without cooling. Paradoxically, the electron cooling system also appears to be responsible for limiting peak currents in the ring at 45 MeV to about 6 mA. Thus the tool which allows us to accumulate beam also prevents us from accumulating more beam. At this point we can account for some of the observed beam features when we include space charge effects. Presently, we do not, however, have any techniques to counteract the space charge effects and thus raise this intensity limit.


Proceedings Particle Accelerator Conference | 1995

The Indiana University Cooler injector synchrotron RF system

A. Pei; M. Ellison; D. Friesel; D. Jenner; Xiaoshen Kang; S.Y. Lee; D. Li; J.Y. Liu; A. Riabko; L. Wang; K. Hedblom

A 2.2 Tesla-meter synchrotron with 17.4 m circumference is being built at the Indiana University Cyclotron Facility (IUCF). The purpose of the project is to achieve higher luminosity for nuclear physics experiments using electron cooled polarized light ion beams in the IUCF Cooler synchrotron. The injection line for the booster synchrotron consists of an RFQ/DTL linear accelerator delivering a 7 MeV proton beam and a 6 MeV deuteron beam for the booster injection. A debunching system will be installed in the injection beamline to reduce the energy spread of beams out of the linear accelerators. Charge-exchange injection is used for high intensity multiturn beam accumulation. The booster output beams, 200 MeV for protons and 105 MeV for deuterons, will be transferred bucket to bucket to the IUCF Cooler synchrotron. The rf system design for the booster synchrotron is presented in this paper.


Advanced beam dynamics workshop on effects of errors in accelerators their diagnosis and corrections | 2008

Nonlinear beam dynamics studies at the IUCF cooler ring

S.Y. Lee; M. Ball; B. Brabson; D.D. Caussyn; J. Collins; S. Curtis; V. Derenchuck; D. DuPlantis; G. East; M. Ellison; T. Ellison; D. Friesel; B. Hamilton; W.P. Jones; W. Lamble; D. Li; M. G. Minty; T. Sloan; G. Xu; A. W. Chao; S. Tepikian; K.Y. Ng

The nonlinear beam dynamics of transverse betatron oscillations were studied experimentally at the IUCF Cooler Ring. Particles were kicked onto resonance islands and the properties of these islands were studied. The island tune was determined with high precision by Fourier analyzing the spectrum containing the islands and the properties of these island were studied. The island tune was determined with high precision by Fourier analyzing the spectrum containing the island oscillations. The island width was estimated based on a single resonance model. The Hamiltonian of particle motion near a resonance condition was thus deduced.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996

A method of detecting coherent synchrotron modes

C. M. Chu; M. Ball; J. Budnick; G. East; M. Ellison; B. Hamilton; X. Kang; S.Y. Lee; J.Y. Liu; A. Pei; A. Riabko; T. Sloan; L. Wang

Abstract A method for measuring coherent longitudinal synchrotron modes is developed and tested at the Indiana University Cyclotron Facility Cooler Ring. This method can be used to detect the onset of coherent instability and can provide important diagnosis for the control of beam brightness. Some possible improvement of this technique is discussed.


international conference on particle accelerators | 1993

Experimental simulation of ground motion effects

M. Syphers; M. Ball; B. Brabson; J. Bucnick; D.D. Caussyn; A.W. Chao; J. Collins; V. Derenchuk; S. Dutt; G. East; M. Ellison; T. Ellison; D. Friesel; W. Gabella; B. Hamilton; H. Huang; W.P. Jones; S.Y. Lee; D. Li; M.G. Minty; S. Nagaitsev; K.Y. Ng; X. Pei; G. Rondeau; T. Sloan; L. Teng; S. Tepikian; Y. Wang; Y.T. Yan; P.L. Zhang

Synchro-betatron coupling in a proton storage ring with electron cooling was studied by modulating a transverse dipole field close to the synchrotron frequency. The combination of the electron cooling and transverse field modulation on the synchrotron oscillation is equivalent to a dissipative parametric resonant system. The proton bunch was observed to split longitudinally into two pieces, or beamlets, converging toward strange attractors of the dissipative system. These phenomena might be important to understanding the effect of ground vibration on the SSC beam, where the synchrotron frequency is about 4/spl sime/7 Hz, and the effect of power supply ripple on the RHIC beam, where the synchrotron frequency ramps through 60 Hz at 17 GeV/c.<<ETX>>


Orbit correction and analysis in circular accelerators | 2008

Determination of the linear coupling resonance strength using 2D invariant Tori

J.Y. Liu; M. Ball; B. Brabson; J. Budnick; D.D. Caussyn; J. Collins; V. Derenchuk; G. East; M. Ellison; D. Friesel; B. Hamilton; H. Huang; W.P. Jones; S.Y. Lee; D. Li; A. Riabko; T. Sloan; Y. Wang; N. Y. Ng

Experimentally obtained Poincare maps in the resonant precessing frame for particle motion with linear coupling revealed invariant tori of the 2D Hamiltonian. Using these tori, we obtained the linear coupling strength, the tune shift with betatron amplitude coefficient and the proximity parameter to the resonance. The coupling strengh obtained with this method agreed well with that obtained from measuring the betatron tune separation of the normal modes.


AIP Conference Proceedings (American Institute of Physics); (United States) | 2008

Longitudinal phase‐space measurements at IUCF

D.D. Caussyn; M. Ball; B. Brabson; J. Budnick; A. W. Chao; J. Collins; V. Derenchuk; S. Dutt; G. East; M. Ellison; T. Ellison; D. Friesel; W. Gabella; B. Hamilton; H. Huang; W.P. Jones; S.Y. Lee; D. Li; M.G. Minty; S. Nagaitsev; K.Y. Ng; X. Pei; G. Rondeau; T. Sloan; M. Syphers; S. Tepikian; Y. Wang; Y. Yan; P. L. Zhang

Synchrotron motion in the IUCF cooler ring was studied using turn‐by‐turn beam tracking on ten‐turn intervals, where the beam phase relative to the rf and the closed‐orbit position in a high‐dispersion region were measured. The synchrotron tune shift with amplitude was measured and is compared with theory. The driven response of the system was also studied using the same techniques, and was found to share many of the same characteristics of other parametric resonant systems. The experimental results did not exhibit any effects of bunch decoherence expected from the tune shift with amplitude.

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S.Y. Lee

Indiana University Bloomington

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M. Ball

Indiana University Bloomington

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B. Hamilton

Indiana University Bloomington

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D. Li

Indiana University Bloomington

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B. Brabson

Indiana University Bloomington

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J. Budnick

Indiana University Bloomington

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G. East

Indiana University Bloomington

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A. Riabko

Indiana University Bloomington

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