IPBSM response to non-Gaussian beam 20130211 K. KUBO.
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Transcript of IPBSM response to non-Gaussian beam 20130211 K. KUBO.
![Page 1: IPBSM response to non-Gaussian beam 20130211 K. KUBO.](https://reader036.fdocuments.net/reader036/viewer/2022083009/5697bf731a28abf838c7ee72/html5/thumbnails/1.jpg)
IPBSM response tonon-Gaussian beam
20130211 K. KUBO
![Page 2: IPBSM response to non-Gaussian beam 20130211 K. KUBO.](https://reader036.fdocuments.net/reader036/viewer/2022083009/5697bf731a28abf838c7ee72/html5/thumbnails/2.jpg)
Motivation of this study
• We sometimes observe apparent discrepancies between beam sizes measured with different IPBSM crossing angles (different modulation pitches)
• May come from systematic errors of IPBSM• But, may come from non-Gaussian beam shape, because
beam size is evaluated assuming Gaussian beam.– How IPBSM measurement depends on beam shape?
![Page 3: IPBSM response to non-Gaussian beam 20130211 K. KUBO.](https://reader036.fdocuments.net/reader036/viewer/2022083009/5697bf731a28abf838c7ee72/html5/thumbnails/3.jpg)
What IPBMS measures
)/2cos(12
),( hyaA
yp
Interference of two laser beams: photon density is
Scanning the phase , “modulation” is
For electron density (y), signal height is
dyhyyadyhyya
dyyG
)/2sin()(sin)/2cos()(cos
)()(
dyy
dyhyiya
GG
GGM
)(
)]/2(exp[)(
maxmax
maxmax
Modulation is, basically, amplitude of Fourier transformation of electron density.
1+a
1-a
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2
2
2exp)(
yy
2
222exp
haM
M
ah ln
2
1
For Gaussian beam
For two Gaussians beam
2
2
2
2
2exp
2exp)(
TC
yT
yCy
TC
hT
hC
aM
TC
2
22
2
22 2exp
2exp
Cannot tell beam size and beam shape.Effect of tail is different for different fringe pitch (crossing angle).But, only important if T is comparable with C.
![Page 5: IPBSM response to non-Gaussian beam 20130211 K. KUBO.](https://reader036.fdocuments.net/reader036/viewer/2022083009/5697bf731a28abf838c7ee72/html5/thumbnails/5.jpg)
Modulation for beam of sum of two Gaussians
0
0.2
0.4
0.6
0.8
1
0 1 10-7 2 10-7 3 10-7 4 10-7 5 10-7
30 deg174 degCalc for 174 deg from 30 deg modulation
Mod
ulat
ion
sigma of 2nd part of beam (m)
Calculated modulations as functions of sigma of 2nd part (tail) of the beam. Population of 1st and 2nd part =1:1Dashed line: Modulation with 174 deg, calculated from the modulation with 30 deg, assuming a single Gaussian beam.
Sigma of 1st part =37 nm
![Page 6: IPBSM response to non-Gaussian beam 20130211 K. KUBO.](https://reader036.fdocuments.net/reader036/viewer/2022083009/5697bf731a28abf838c7ee72/html5/thumbnails/6.jpg)
Rectangular beam
)(0
)(1)(
by
byy
)/2(
)/2sin(
hb
hbaM
0
0.2
0.4
0.6
0.8
1
0 100 200 300 400 500 600
Gauussian bunch, 7 deg modeGauussian bunch, 30 deg modeGauussian bunch, 174 deg modeRectangular bunch, 7 deg modeRectangular bunch, 30 deg modeRectangular bunch, 174 deg modeM
odu
lati
on
RMS (nm)
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Tracking simulation of ATF2 beam line IPBSM modulation
0
0.2
0.4
0.6
0.8
1
0 0.001 0.002 0.003 0.004 0.005 0.006
174 deg.
30 deg
Mod
ula
tion
sigma_E/E
Set very large energy spread might simulate large non-linear effects (?) large tail
0
1000
2000
3000
4000
-2 10-6 -1 10-6 0 1 10-6 2 10-6
sigmaE/E=0.5%
Cou
nts
y (m)
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Tracking simulation of ATF2 beam line IPBSM modulation
Set strong transverse wakefield
0
200
400
600
800
1000
-5 10-7 -4 10-7 -3 10-7 -2 10-7 -1 10-7 0 1 10-7
MREF3FF 1.6 mm offsetemity 12 pm
Cou
nt
y (m)40
60
80
100
120
140
160
0.1
0.2
0.3
0.4
0.5
0.6
0.7
-0.002 -0.0015 -0.001 -0.0005 0 0.0005 0.001 0.0015 0.002
sigmay (nm) modulation
sigm
ay
(nm
) modu
lation
MREF3 offset
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Conclusion
We should keep in mind that
•IPBSM is not necessarily measuring sigma or RMS beam size.
•Modulation is not necessarily monotonic function of RMS, or sigma of core part of the beam.
•Evaluated beam size from modulation assuming Gaussian beam can be different for different crossing angle on leaser beams.
If electron beam shape is far from Gaussian.
No conclusion about the actual beam size and beam shape.
Here, only possibilities are shown.