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Lecture 6 ACCELERATOR PHYSICS MT 2011 E. J. N. Wilson.

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Presentation on theme: "Lecture 6 ACCELERATOR PHYSICS MT 2011 E. J. N. Wilson."— Presentation transcript:

1 Lecture 6 ACCELERATOR PHYSICS MT 2011 E. J. N. Wilson

2 Lecture 6 - Longitudinal dynamics II -contents
Transition - does an accelerated particle catch up - it has further to go Phase jump at transition Synchrotron motion Synchrotron motion (continued) Large amplitudes Buckets Adiabatic capture A chain of buckets

3 Recap of previous lecture - Longitudinal dynamics I
RF Cavity Cells Phase stability Bucket and pendulum Closed orbit of an ideal machine Analogy with gravity Dispersion Dispersion in the SPS Dispersed beam cross sections Dispersion in a bend (approx) Dispersion – from the “sine and cosine” trajectories From “three by three” matrices..

4 Transition - does an accelerated particle catch up - it has further to go
Is a function of two, momentum dependent, terms b and R. and Using partial differentials to define a slip factor: This changes from negative to positive and is zero at ‘ transition’ when: GAMMA TRANSITION

5 Phase jump at transition
BECAUSE .....

6 Synchrotron motion Recall Elliptical trajectory for small amplitude
Note that frequency is rate of change of phase From definition of the slip factor h Substitute and differentiate again But the extra acceleration is THUS

7 Synchrotron motion (continued)
This is a biased rigid pendulum For small amplitudes Synchrotron frequency Synchrotron “tune”

8 Large amplitudes and become Integrated becomes an invariant
The second term is the potential energy function

9 Buckets Seen from above this is a bucket (in phase space) for different values of The equation of each separatrix is

10 A chain of buckets

11 Bucket length I The right hand side is negative beyond:
This diagram is flipped left to right

12 Bucket length II And the other limit in phase when at

13 Bucket height And the half height when at

14 Adiabatic capture Area of a stationary bucket is :

15 Longitudinal Dynamics II – Summary
Transition - does an accelerated particle catch up - it has further to go Phase jump at transition Synchrotron motion Synchrotron motion (continued) Large amplitudes Buckets Adiabatic capture A chain of buckets


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