1 Monday Week 1 Lecture Jeff Eldred Longitudinal

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1 Monday Week 1 Lecture Jeff Eldred Longitudinal Dynamics, RF manipulations

1 Monday Week 1 Lecture Jeff Eldred Longitudinal Dynamics, RF manipulations

2 Jeffrey Eldred (TA) • Graduated with Ph. D December 2015 • Indiana University

2 Jeffrey Eldred (TA) • Graduated with Ph. D December 2015 • Indiana University working with Shyh-Yuan Lee • Worked at Fermilab on PIP-II upgrade • Slip-stacking and Electron Cloud. Postdoc at Fermilab on IOTA experiment Nonlinear transverse dynamics, Landau damping, space-charge compensation, modern ring-design Kilean Hwang (grader) • Graduating with Ph. D this semester • Indiana University working with Shyh-Yuan Lee • Dipole fringe fields • Electrostatic storage rings using EDM.

3 Overview 1. 2. 3. 4. 5. RF Cavities Longitudinal Dynamics RF bucket phase-space

3 Overview 1. 2. 3. 4. 5. RF Cavities Longitudinal Dynamics RF bucket phase-space RF acceleration Other RF dynamics

4 Longitudinal Motion of Particle Beams

4 Longitudinal Motion of Particle Beams

5 Credit: FNAL Rookie Book

5 Credit: FNAL Rookie Book

6 Numerically Calc. Eigenmodes Credit: University of Rostock

6 Numerically Calc. Eigenmodes Credit: University of Rostock

7 Credit: Q. Wu, S. Belomestnykh W. Xu

7 Credit: Q. Wu, S. Belomestnykh W. Xu

8 Energy in one pass through cavity

8 Energy in one pass through cavity

9 Change in Momentum Fractional Momentum: RF Acc. Per Pass: Change Momentum per unit

9 Change in Momentum Fractional Momentum: RF Acc. Per Pass: Change Momentum per unit time: Sinesoidal potential:

10 Phase-Slip Factor η The arrival time of the particle depends on the momentum:

10 Phase-Slip Factor η The arrival time of the particle depends on the momentum: Higher momentum particles may arrive earlier or later than lower momentum particles: We can write the change in phase per unit time using the phase-slip factor:

11 Longitudinal Focusing

11 Longitudinal Focusing

12 Phase-space Motion

12 Phase-space Motion

13 Hamiltonian & Separatrix Hamiltonian: Separatrix: Stable Phase-space Area:

13 Hamiltonian & Separatrix Hamiltonian: Separatrix: Stable Phase-space Area:

14 Perturbation of Synchrotron Motion

14 Perturbation of Synchrotron Motion

15 Stable Beams

15 Stable Beams

16 Perturbation of Stable Beams

16 Perturbation of Stable Beams

17 Slipping Beams

17 Slipping Beams

18 Perturbation of Slipping Beams

18 Perturbation of Slipping Beams

19 Accelerating Buckets

19 Accelerating Buckets

20 RF Acceleration • A fixed frequency beam longitudinally focuses the beam into a

20 RF Acceleration • A fixed frequency beam longitudinally focuses the beam into a several beam “bunches” in individual RF “buckets”. • Particles in the bucket can be accelerated by adiabatically changing the RF frequency, the other particles are lost.

21 Credit: X. Kang SY. Lee

21 Credit: X. Kang SY. Lee

22 0 15 30 45

22 0 15 30 45

23 Stable Phase-space Area as a function of φs

23 Stable Phase-space Area as a function of φs

24 Other Examples of Longitudinal RF Dynamics

24 Other Examples of Longitudinal RF Dynamics

25 Transition Crossing

25 Transition Crossing

26 Phase-Focusing & Acceleration

26 Phase-Focusing & Acceleration

27 Phase-space at Transition

27 Phase-space at Transition

28 RF + Harmonic RF Cavities

28 RF + Harmonic RF Cavities

29 Harmonic RF 2 nd Harmonic RF: In general you could imagine:

29 Harmonic RF 2 nd Harmonic RF: In general you could imagine:

30 Harmonic RF for H- injection Credit: JPARC

30 Harmonic RF for H- injection Credit: JPARC

31 Harmonic RF for Ph-Sp Dilution Credit: A. Pham

31 Harmonic RF for Ph-Sp Dilution Credit: A. Pham

32 Bunch Rotation by Quadrupole Resonance

32 Bunch Rotation by Quadrupole Resonance

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34 Credit: X. Yang

34 Credit: X. Yang