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FBCT experience at Desy

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FBCT experience at Desy. Presenter : Matthias Werner, DESY At CERN Workshop: „ Improving the accuracy of the BCT measurements in the LHC“ January 2011. About this presentation :. - PowerPoint PPT Presentation
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FBCT experience at Desy Presenter: Matthias Werner, DESY At CERN Workshop: „Improving the accuracy of the BCT measurements in the LHC“ January 2011
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Page 1: FBCT  experience at Desy

FBCT experience at Desy

Presenter:Matthias Werner, DESY

At CERN Workshop:„Improving the accuracy of the BCT measurements in the LHC“January 2011

Page 2: FBCT  experience at Desy

About this presentation:This presentation consists mainly of

information from our BCT expert Reinhard Neumann and shows developments of our former BCT expert Willi Radloff.

I just present their results.

Page 3: FBCT  experience at Desy

FBCTs used at DESYBergoz FBCTs e.g. for Petra

accelerator for high bandwidthInhouse development (by W.Radloff)

e.g. for FLASH and XFEL accelerator for low beam position dependence.

Page 4: FBCT  experience at Desy

FBCTs with reduced beam position dependence The monitors are equipped with 4 symmetric coils to

minimize beam position dependence. In the original design, each coil has 10 turns. In the actual design for FLASH, each coil has 1 turn and an

RF transformer (w1/w2 = 1/10), resulting in increased bandwidth (in the order of 100 MHz) for optimized design, but decreased amplitude.

The currents of the 4 coils are added up by a summing network combined with an impedance matching transformer (improved version under development).

Unconfirmed tests showed an amplitude change of ±0.3% for position changes of ±6 mm – this could be further improved by trimming.

Page 5: FBCT  experience at Desy

Pickup and Electronics

Page 6: FBCT  experience at Desy

Halfcore in PEEK-Carrier

Page 7: FBCT  experience at Desy

Both Halfcores

Fully equipped beam transformer halfcores

Page 8: FBCT  experience at Desy

Split Pickup Electrode

Transformer halfcores embedded in shielding halfcovers

Page 9: FBCT  experience at Desy

Toroid TTF2- Dump

Complete, with cables, combiner and filter

Page 10: FBCT  experience at Desy

Toroid in TTF2 Linac

LP-FilterCombiner

Page 11: FBCT  experience at Desy

Precision of BCTs at DESY

Info from Reinhard Neumann:Up to now, a precision of ≈1%

(reproducibility, not absolute accuracy) of full range was achieved, this was enough for the Desy accelerators, so no further development was done to improve the precision.

Page 12: FBCT  experience at Desy

What can affect precision and resolution of a BCT? Calibration method Amplitude stability of signal processing chain Temperature dependence Beam position dependence Baseline suppression: Take zero reference from bunch gap

or before every bunch? Lowpass filter directly after BCT or processing a high

bandwidth signal? Interference: symmetric or asymmetric data transmission? Signal processing principle: integrating over a window or

sampling a filtered signal? Noise in the signal processing chain: Amplifier, Integrator

(if any), ADC Digital processing algorithm

Page 13: FBCT  experience at Desy

Thank you!

Page 14: FBCT  experience at Desy

Transparencies beyond the presentation at the workshop

Page 15: FBCT  experience at Desy

Hardware Schematics of the PC based Bunch Current Monitor

Page 16: FBCT  experience at Desy

100 MHz Amplifier

Page 17: FBCT  experience at Desy

Types of BCTs at DESYInfo from Reinhard Neumann: At Petra (light source, max. planned bunch frequency =

500 MHz): BCT: Bergoz type (Spec: BW=2GHz, rise time 175 ps) –

only one coil Considerable position dependence observed Acquisition: Oscilloscope (8 bit resolution)

FLASH accelerator (max. bunch frequency = 9 MHz): BCT: „Radloff“-Type (selfmade with 4 coils) Acquisition: VME ADC modules (14 bit, 2 samples per

bunch) Other accelerators and transport lines:

BCT: „Radloff“-Type (selfmade with 4 coils) Acquisition: PC ADC boards

Page 18: FBCT  experience at Desy

Impedance matching at BCT coil outputNumber of turns on the toroid and

Impedance ratio of successive RF transformers determines impedance matching.

What is the source impedance of the coils?For some termination, we get optimum

amplitude, for maximum bandwith we need a lower termination resistance.

What is the optimum for our case? (Especially important if resolution is limited by noise.)


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