Proposal for a Transparent Off-Axis Injection Scheme for BESSY II

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Presentation transcript:

Proposal for a Transparent Off-Axis Injection Scheme for BESSY II Peter Kuske, HZB and Humboldt-Innovation GmbH August 29, 2017, Workshop on Injection and Injection Systems (TWIIS), BESSY II, Berlin, Germany

Traditional Injection – 4 Kicker Bump – not Transparent Content Introduction Traditional Injection – 4 Kicker Bump – not Transparent Alternative Injection Schemes with Single Non-Linear Kicker – Potentially Transparent Limitations and Ultimate Injection Scheme? Summary

I. Transparent Injection - Definition Injection is transparent if users don‘t see any perturbation of the photon beam is s/10 still the figure of merit? is off-axis injection transparent? how transparent is swap-out injection? injection efficiency approaches 100% radiation safety protection of sophisticated IDs and of lattice elements with permanent magnets What makes it so difficult?

II. Traditional Injection Scheme with 4 Kicker Bump and Septum Magnet oscillation amplitude of injected particles as small as possible

II. Traditional Injection Scheme with 4 Kicker Bump and Septum Magnet small emittance of injected beam

II. Traditional Injection Scheme with 4 Kicker Bump and Septum Magnet orbit bump large enough

II. Traditional Injection Scheme with 4 Kicker Bump and Septum Magnet With smaller and smaller beam sizes the oscillation amplitude of injected electrons is determined by the 2-3 mm thick septum blade

II. 4 Kicker Orbit Bump and Correct Timing

II. Traditional Injection Scheme with 4 Kicker Bump and Septum Magnet Key factors for 100% injection efficiency: dynamic aperture large enough (transverse and longitudinal, IDs, …) emittance of injected beam small enough (transverse and longitudinal, beam stability in synchrotron) stable hardware operation (injection/extraction kicker, septa and bumper, timing and amplitudes) good optics and beam matching between injector and storage ring Why does the traditional injection scheme create beam perturbations? fast orbit bump is never closed and purely one dimensional – despite many attempts the adjustment of 4 kicker pulses to be identical has never been achieved (pulse shape, timing and amplitude jitter, coatings of ceramic chambers, special shims, feed-forward correction, …) septum magnet stray field has been reduced significantly – alternatively the effect can be nearly cancelled with feed forward compensation. Will this be good enough for the small beam sizes foreseen in the future? We need alternative injection schemes: like on-axis-off-momentum injection (taking advantage of the large momentum acceptance or with double/triple RF-system), on-axis swap-out injection or off-axis injection with a single non-linear kicker magnet.

III. Single Non-Linear Kicker Injection Scheme logical improvement: Replacement of pulsed quadrupole or sextupole magnet by more suitable magnet (NLK, the non-linear kicker magnet) ESLS workshop, Diamond, 2007

III. BESSY II Non-Linear Kicker (NLK)

III. Injection Scheme Based on Single Non-Linear Kicker and Septum Magnet NLK

III. Injection Scheme Based on Single Non-Linear Kicker and Septum Magnet NLK smaller amplitude with closer wires difficult, large ßy

III. Injection Scheme Based on Single Non-Linear Kicker and Septum Magnet NLK smaller kick angle with larger distance

III. Injection Scheme Based on Single Non-Linear Kicker and Septum Magnet NLK even smaller NLK strength after one revolution

III. Injection Scheme Based on Single Non-Linear Kicker and Septum Magnet NLK NLK can be placed more optimally

III. Injection Scheme Based on Single Non-Linear Kicker and Septum Magnet NLK NLK can be placed more optimally

III. Injection Scheme Based on Single Non-Linear Kicker and Septum Magnet NLK NLK can be placed at vertical focus septum placed at down stream end of injection straight

III Optics Modifications for Improved Injection Efficiency Larger ßx and smaller ßy in the center of the injection straight smaller ßx in D-straights mitigates impact of strong APPLE II undulators smaller ßy in injection straight allows for smaller vertical gap of NLK

III. Simulations for BESSY II with this Injection Geometry NLK

aperture requirement vs ßx and x with injection angle -0.35 mrad III. Simulation Results for 100% Injection Efficiency aperture requirement vs ßx and x with injection angle -0.35 mrad

aperture requirement vs ßx and x with injection angle -0.30 mrad III. Simulation Results for 100% Injection Efficiency aperture requirement vs ßx and x with injection angle -0.30 mrad

aperture requirement vs ßx and x with injection angle -0.25 mrad III. Simulation Results for 100% Injection Efficiency aperture requirement vs ßx and x with injection angle -0.25 mrad

aperture requirement vs ßx and x with injection angle -0.20 mrad III. Simulation Results for 100% Injection Efficiency aperture requirement vs ßx and x with injection angle -0.20 mrad

aperture requirement vs ßx and x with injection angle -0.15 mrad III. Simulation Results for 100% Injection Efficiency aperture requirement vs ßx and x with injection angle -0.15 mrad

IV. Limitations and Ultimate Injection Scheme? In the 4 kicker orbit bump injection scheme the thickness of the septum blade eats up most of the valuable dynamic aperture, less so for single NLK injection Low emittance rings demand low emittance injectors – synchrotron in the storage ring tunnel (Swiss Light Source) – or LINAC (MAXIV) What would be helpful: Septum magnet without blade – the non-linear kicker for example, any multipole magnet → beam injected under smaller angles Smaller vertical gap of NLK – would we accept 1 mm vertical aperture over 50 cm? → 2 mm off-axis injection ALS-U, 8BA-lattice – can ßx be larger and ßy smaller in injection straight without sacrificing emittance and aperture? Is swap-out injection the only way? M. Venturini, LER Workshop, Oct. 2016, Soleil, Paris, France

V. SUMMARY Off-Axis injection into electron storage rings can be performed transparent and with high efficiency if: an alternative to the 4 kicker injection scheme is used emittance of the injected beam approaches the emittance of the stored beam sufficient dynamic aperture available septum blade as thin as possible NLK operated with smaller vertical vacuum gap Swap-Out injection will not be fully transparent – amplitude and timing jitter of kicker magnets Neither will be the off-axis injection even if the stored beam remains perfectly stable users have to live with that In the future high injection efficiency will become even more important: radiation safety protection of sophisticated IDs protection of lattice elements with permanent magnets High injection efficiency - challenge for all alternative injection schemes

any questions?