X-ray beam size monitor Gives turn by turn beam size

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06/21/22 1 -ray beam size monitor ives turn by turn beam size Tune dependence ne scan of vertical beam size December 22, 2009

description

Tune dependence. Tune scan of vertical beam size. December 22, 2009. X-ray beam size monitor Gives turn by turn beam size. Tune dependence. Smallest measured beam size. Largest measured beam size. Cta_2085mev_20090516. Q z =0.066=25.7kHz. nominal. Zero dispersion in RF. Horizontal tune. - PowerPoint PPT Presentation

Transcript of X-ray beam size monitor Gives turn by turn beam size

Page 1: X-ray beam size monitor Gives turn by turn beam size

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X-ray beam size monitorGives turn by turn beam size

Tune dependenceTune scan of vertical beam size

December 22, 2009

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Smallest measured beam size

Largest measured beam size

Tune dependence

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Cta_2085mev_20090516

nominal Zero dispersion in RF

Qz=0.066=25.7kHz

Horizontal tune Horizontal tune

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Qh<0.5

Horizontal tune

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Reverse sextupole steering windings - skew quads

Skew quad k~0.002/m2 @ 14A

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Closed dispersion/coupling bumps

ηy at 18-19

η'y at 18-19

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BPM systematics

Gain mapping

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Signal at each button depends on bunch current (k) and position (x,y)

Signals on the four buttons are related by symmetry

Combining sums and differences we find the following relationship, good to second order

Characterization of BPM Gain Errors

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Using a map that reproduces the “exact” dependence of the button signals on the bunch positions we generate B1,B2,B3,B4 for each of 45 points on a 9mm x 5mm grid

Gain characterization simulation

The small deviations from the straight line at large amplitudes is a measure of the higher than second order contributions.

In first order c=0, and therefore B(+--+) = 0. Evidently the first order approximation is not very good enough this range.

Simulation

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Zero offset, nonlinearity, and multi - valued relationship i n is a measure of gain errors.

Simulation with gain errors

Introduce gain errors

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To fit for gains

Fix g1=1, and minimize with respect to g2,g3,g4,c

Fitted gains = 1,0.95,0.96,0.97

Orbit data collected on a grid

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BPM 75 - fitted gain = 1,1.02,0.96,0.91

BPM 77 - fitted gain = 1,0.92,0.96,0.9

Fit typically reduces 2 by two orders of magnitude

Orbit data collected on a grid

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Turn by turn data, December 10, 2009

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Average gains computed for 6 turn by turn data sets

Error bar is the standard deviation of the 6

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Fitted gains from 6 turn by turn data sets, RD-000652, 653, 654, 655, 656, 657Normalized so that average at each BPM of 4 gains is unityStandard deviation, eliminating all points with gain errors greater than 50% is =4.3%

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Data from December 19, 2009

Turn by turn data RD-000908.dat, RD-000909.dat

Immediately followed by measurement of phase.8607 and ac_eta.165

1.Use turn by turn data to determine gains

2.Use fitted gains to correct coupling and eta measurements

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Examples of fits for various BPMs

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Summary of fitted gains

σ = 4.6%

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Coupling without gain correction

Coupling with gain correction

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Dispersion without gain correction

Dispersion with gain correction