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Published byFrank Briggs Modified over 9 years ago
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Part III Commissioning
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Proof of Principle FFAG (POP) study The world first proton FFAG –Commissioned in March 2000. –From 50 keV to 500 keV in 1ms. –Proof of proton FFAG –Various beam operations
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Components
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POP synchrotron overview
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Optics with linear approximation SAD calculation
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Multi-turn injection 1 turn (left) and 5 turns (right)
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Beam acceleration BPM signal
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Observations of machine parameters Tune survey (dynamic) aperture survey
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Tune at injection with various F/D ratio
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Energy dependence Synchrotron oscillation frequencyradius position
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Dynamic aperture survey single particle simulation
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Experimental results
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Center of gravity multi-particle simulation
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Amplitude dependent tune shift
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More beam manipulation study Multi bunch acceleration Acceleration with 2 fixed frequency Slow extraction with massless septum Resonance crossing
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Multi bunch acceleration As long as two buckets are separated in longitudinal phase space, simultaneous acceleration is possible. Repetition rate is effectively increased.
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RF pattern Second RF follow the first one.
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Acceleration with two RF buckets Experimental results
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Acceleration with 2 fixed frequency Idea is to accelerate a beam with two (or more) fixed frequency. By simulation, if the timing of two RF is chosen correctly, a part of a beam is accelerated.
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Experimental results Black: simulation with two buckets. Green: simulation with one bucket. Red: experiment with two buckets. It is proven experimentally that energy is increased more than that can be accelerated with one bucket.
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Slow extraction with massless septum Septum without septum blade. Field does not drop off shapely, rather linear decay like a quadrupole.
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Field distribution (calculated and measured) Measured a model magnet.
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How the massless septum works. (a)Kick by massless septum. (b)Cut by electric septum. (c)Restore the beam by massless septum.
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Resonance crossing Crossing speed is a parameter
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Signal at 4 RF patterns 20 deg.10 deg. 4 deg. 2deg. Red arrow indicates time when a beam hits chamber. When the ramping is slow, a beam is lost before hitting chamber.
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