Betatron Motion with Coupling of Horizontal and Vertical
Betatron Motion with Coupling of Horizontal and Vertical Degrees of Freedom – Part I S. A. Bogacz, G. A. Krafft, S. De. Silva and R. Gamage Jefferson Lab and Old Dominion University Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 1
Outline Introduction Equations of Motion, Symplecticity and Eigen-vectors and Particle Ellipsoid in 4 D Phase Space Generalized Twiss Functions Derivatives of Tunes and Beta-Functions – 4 D Floque formulae Second order moments in terms of generalized Twiss functions V. Lebedev, A. Bogacz, ‘Betatron Motion with Coupling of Horizontal and Vertical Degrees of Freedom’, 2000, http: //dx. doi. org/10. 1088/1748 -0221/5/10/P 10010 Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 2
Introduction Courant-Snyder representation for one-dimensional betatron motion Simple relations between Twiss parameters, eigen-vectors and bilinear form for the particle ellipsoid Symplecticity 2 2 – 1 = 3 parameters From uncoupled to strongly coupled motion by design “Moebius Twist Accelerator” to create round beams (Cornell) Ionization cooling channel for Neutrino Factory and Muon Collider Vertex to plane adapter for electron cooling (Fermilab) Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 3
Two dimensional coupled betatron motion Symplecticity 4 4 – 6 = 10 parameters Effective parameterization in terms of generalized Twiss functions Shortcomings of the existing representations Edwards and Teng, Fermilab (1973) Ambiguity of the rotation angle Physical meaning of the betatron phase advance? G. Ripken, et al. , DESY (1987) Oriented for circular accelerators Incomplete parametrization (one needs 10 independent parameters to fully describe 2 D betatron motion) Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 4
Unresolved issues for both parametrizations Quest for versatile representation conveniently describing both storage rings and transfer lines 2 D emittances - how are they related to the 4 D beam emittance? How to determine the beam emittances and the generalized Twiss parameters from the particle beam ellipsoid (bilinear form), and from the secondorder moments of the particle distribution? Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 5
Equations of Motion and Symplecticity Condition Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 6
Hamiltonian formulation - equations of motion Hamiltonian matrix: Unit symplectic matrix : Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 7
Hamiltonian formulation - equations of motion Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 8
Hamiltonian formulation - equations of motion Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 9
Hamiltonian formulation - Sympecticity Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 10
Eigen-vectors Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 11
Eigen-vectors Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 12
Eigen-vectors Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 13
Eigen-vectors and Particle Ellipsoid in 4 D Space Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 14
Eigen-vectors and Particle Ellipsoid in 4 D Space Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 15
Eigen-vectors and Particle Ellipsoid in 4 D Space Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 16
Beam emittance 4 -D Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 17
Beam emittance 4 -D Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 18
Beam emittance 4 -D Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 19
Second order moments of the particle distribution Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 20
Beam emittance 4 -D Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 21
Beam emittance 4 -D Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 22
Beam emittance 4 -D Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 23
Beam emittance 4 -D Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 24
Twiss Functions for Coupled 2 D Motion Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 25
Twiss Functions for Coupled 2 D Motion Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 26
Twiss Functions for Coupled 2 D Motion Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 27
Twiss Functions for Coupled 2 D Motion Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 28
Twiss Functions for Coupled 2 D Motion Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 29
Twiss Functions for Coupled 2 D Motion Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 30
Twiss Functions for Coupled 2 D Motion Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 31
Beam sizes Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 32
Derivatives of Tunes and Beta-Functions Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 33
Derivatives of Tunes and Beta-Functions Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 34
Transfer Matrix in terms of Twiss Functions Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 35
Transfer Matrix in terms of Twiss Functions Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 36
Transfer Matrix in terms of Twiss Functions Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 37
Transfer Matrix in terms of Twiss Functions Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 38
Beam ellipsoid in 4 D space - bilinear form Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 39
Beam ellipsoid in 4 D space - bilinear form Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 40
Beam ellipsoid in 4 D space - bilinear form Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 41
Second order moments in terms of Twiss functions Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 42
Second order moments in terms of Twiss functions Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 43
Summary Thomas Jefferson National Accelerator Facility Operated by JSA for the U. S. Department of Energy Lecture 7 - Coupled Betatron Motion I USPAS, Fort Collins, CO, June 13 -24, 2016 44
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