Synchro-betatron Resonanzen: eine Einführung und Berechnung der Resonanzstärken für verschiedene HERA Optiken F. Willeke Betriebsseminar Salzau 5-8. Mai.

Präsentation zum Thema: "Synchro-betatron Resonanzen: eine Einführung und Berechnung der Resonanzstärken für verschiedene HERA Optiken F. Willeke Betriebsseminar Salzau 5-8. Mai."—  Präsentation transkript:

1 Synchro-betatron Resonanzen: eine Einführung und Berechnung der Resonanzstärken für verschiedene HERA Optiken F. Willeke Betriebsseminar Salzau 5-8. Mai 2003 Einführung und Definition Hamilton Funktion für die Bewegung mit 3 Freiheitsgraden Einführung der Dispersion und Enkopplung von transversalen und longitudinalen Schwingungen Behandlung von Resonanzen mit 2Freiheitsgraden Diskussion der Ergebnisse für HERA

2 Es gibt große Probleme die Polarizations- tunes bei HERA einzustellen:
Einführung Es gibt große Probleme die Polarizations- tunes bei HERA einzustellen: fx= 6.5 kHz und fz=9kHz Der horizontale Tune liegt zwischen dem 2-fachen und dem 3-fachen der Synchrotronfrequenz fs=2.5kHz Verdacht: Der Bereich der gewünschten Arbeitspunkte ist durch starke Synchrobetaronresonanzen eingeschränkt. Synchrobetatron-Resonanzen wurden bei DORIS I entdeckt (Piwinski 1972) Ursache: Starker vertikaler Kreuzungswinkel der kollidierenden Elektron und Positronstrahlen: Die transversale Strahl-Strahl-Kraft hängt bei einem Kreuzungswinkel von der longitudinalen Position im Bunch ab DORIS

3 Allgemein Der Strahl kann in 3 Ebenen oszillieren.
1) Hängt die triebende Kraft in einer Ebene von der Koordinate oder dem Impuls in der anderen Ebene ab, sind die jeweiligen Schwingungsebenen gekoppelt. 2) Wie alle Kräfte können koppelnde Kräfte mit der gleichen Frequenz oszillieren wie der Strahl selbst: Dann kommt es zu einer resonanzartigen Verstärkung selbst sehr kleiner Kräfte. Resonanzen führen zum Energieaustausch zwischen den Schwingungsebenen oder zu Instabilität

4 Synchro-Betatron Resonances in HERA Introduction to the Theory and Recent Evaluations HERA Betriebsseminar Salzau, 5-7 May 2003 Coupled Synchro-betatron Motion Decoupling of Synchro-betatron Oscillation Non-linear Coupling between Synchrotron and Betatron Oscillations Width of multi-dimensional Nonlinear Resonances Comparison of the width of Satellite Resonances in HERA for various Beam Optics

5 Synchrobetatron-Resonances
Coupling between transverse and longitudinal oscillations gives rise to excitation of resonances for tunes which satisfy Qx+mQs+q=0 Such resonances can be driven by Dispersion in the cavities Dispersion in sextupoles Chromaticity A crossing angle or Dispersion a the Collision Point Wakefields RF Quadrupoles …

6 Coupled Synchro-betatron Oscillations
Horizontal Betatron Oscillations and Synchrotron oscillations are strongly coupled by a term x·e /r x is the horizontal coordinate, e is the relative energy deviation from nominal and r is he curvature of he design orbit) This is shown in the following slides

7 Expressing L in accelerator coordinates
Lagrangian for charged relativistic particle using the accelerator coordinate system m0c2 rest mass, r is the position vector, A is the vector potential, f is the scalar potential Expressing L in accelerator coordinates One obtains

8 Hamiltonian picture z=x,y,s b= v / c ˜= 1

9 Path length s as independent variable
The Hamiltonian is symmetric in all coordinates (Variation principle) (gauge) as=e/cAs/E0 m0c2/E0<<1

10 Hamiltonian for motion in x-s plane
Expanded and without solenoid fields The term px2x/r is considered small and has been dropped

11 Cavity Field as=1/2 V · s 2 + 1/6 W · s 3
Expanded and without constants, energy loss concentrated at cavity, damping neglected as=1/2 V · s /6 W · s 3

12 Hamiltonian with cavities and sextupoles
Longitudinal focussing Linear optics NonlinearitiesTransverse motion chromatics Approximations: v=c p2x/r neglected Square root expanded 1/(1+e) expanded into 1-e Strong linear coupling between horizontal and longitudinal motion Nonlinearities longitudinal motion

13 Linear Decoupling of Synchrobetatron Oscillations
Introduction of the dispersion function Generating function transformation

14 Decoupled Hamiltonian
Transverse linear optics Longitudinal linear optics Linear coupl. by dispersion in cavities Chromatics 2nd satellite driving terms Nonlinearities trans. Nonlinearities lon.

15 Integer Satellite Driving Terms
Qx+Qs+p=0 -DVs p + D’Vs x Qx+2Qs+p=0 -D’ p e2 + ½ mD2 e2x + ½ WD s2p Chromatics sextupole contribution dispersion in cavities

16 Resonances in x-s Phase Space
K = Klin + Knl Linear optics Smooth rf model Variation of constant: Keep the form for x, p s,e but vary the invariants Jx,s and fx,s to solve for the nonlinearities and coupling (transformation to action and angle variables) Result Hamiltonian form of e.o.m. with Knl as new Hamiltonian ∂J/ ∂s = - ∂Knl/ ∂f ∂ f / ∂s = ∂Knl/ ∂J

17 Procedure to calculate resonance widths
Express Knl in J-f coordinates Factorise into ring periodic and nonperiodic terms Express periodic forms in Fourier Series Realise, that only slow terms can affect a change in invariants Drop nonresonant terms Transform into a rotating system to get a time-indpendent system Calculated fixpoints Find distance from resonance to reach the fix points for a given amplitude

18 Perform this for the term ½ WDs2p
Since we are only near one resonance at a time, we are only interested in one of the terms x+2y

19 Periodic factor non-periodic factor
Fourier Series for periodic part Select only the one resonant term and ‘drop’ all the others, replace 2ps/L by q (change independent variable from s to q)

20 Resonance Hamiltonian
Transformation into rotating system via generating function F

21 Note there is a similar term denoted by “s” which comes from the sine part of p
The two driving terms k12qs and k12qc are combined into a single one

22 Resonance Width 2Ix-Is is an invariant and we can reduce the system to a 1-dim system Note: sum resonances are instable and difference resonances stable!! R DI Separatrix, unstable trajectory I0=unstable fix point I

23 D12q=½ k12q Is0 Ix0-1/2 Condition for unstable fix point
Evaluate this for Ix = Ix0 D12q=½ k12q Is0 Ix0-1/2

24 Satellite Resonance with
Hamilonian vs action Satellite Resonance with h=0.1m-1 Horizonal projection of separatrix Longitudinal projection of separatrix

25 Evaluations Optics Qx+Qs Qx+2Qs Cavities Chrom. sext total helum72gj
Integrals are replaced by sums, optical functions are replaced by their integrated value over the elements, then a thin lens treatment is applied Beam Parameters used optics amco [10-4] bs/m es[10-6m] ex[10-9m] helumv6 6.8 11.5 9.0 42 helum72gj 4.75 9.9 14.5 22 helum72sm Results: Resonance width for a 10 sigma particle in Hz (nsx2+nss2=100) Optics Qx+Qs Qx+2Qs Cavities Chrom. sext total helum72gj 19 297 487 747 1306 helum72sm 22 276 476 405 948 helumv6 24 93 222 250 458

26 Resonance Optics 3Qx Qx Qx+2Qy Qx-2Qy Qx+0Qy 2Qx+Qs Helum72gj 77 63
Comparison of sextupole driven transverse resonances for one sigma transverse, full coupling and width of horizontal half integer stopband for 10 sigma long. Resonance Optics 3Qx Qx Qx+2Qy Qx-2Qy Qx+0Qy 2Qx+Qs Helum72gj 77 63 167 2289 223 2231 Helum72sm 252 73 303 983 210 1470 Helumv6 88 161 759 239 492 990

27 Conclusions The 3rd order transverse and satellite resonances are stronger in the 72deg optics compared to the old 60 degree optics The stronger satellite resonances are due to more unfavorable ratio of Longitudinal and transverse emittance The SM optics has lower contributions from sextupole driven satellites