observation of beam halo with corona graph. objective lens magnifier lens opaque disk to block glare...
TRANSCRIPT
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Observation of beam halo
with corona graph
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Objective lens
Magnifier lens
Opaque disk to block glare of central image
Observation with normal telescope
1. Diffraction fringes vs. beam tail (halo)
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Diffraction fringes makes tail surrounding from the central beam image.
Intensity of diffraction tail is in the range of 10-2 -10-3 of the peak intensity.
The diffraction tail disturb an observation of week object surrounding from bright central beam
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Diffraction fringesGaussian beam profile
Convolution between diffraction fringes and beam profile
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Diffraction fringesGaussian beam profile
Convolution between diffraction fringes and beam profile
Blocked by opaque disk
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2. The coronagraph to observe sun corona
Developed by B.F.Lyot in 1934 for a observation of sun corona by artificial eclipse.
Special telescope having a re-diffraction system to eliminate a diffraction fringe.
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Optical system of Lyot’s corona graph
Objective lens
Field lens
Baffle plate (Lyot stop)
Relay lens
Opaque disk
Anti-reflection disk
Baffle plates to reduce reflection
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3. Re-diffraction optics system to eliminate the diffraction fringe
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Opaque disk
Lyot stop
Re-diffraction optics systemOpaque disk
Field lens
Objective lens
Re-diffraction Re-diffraction optical systemoptical system
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Opaque disk
Lyot stop
Re-diffraction optics systemOpaque disk
Field lens
Objective lens
Re-diffraction Re-diffraction optical systemoptical system
Function of the field lens : make a image of objective lens aperture onto Lyot stop
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Opaque disk
Lyot stop
Re-diffraction optics systemOpaque disk
Field lens
Objective lens
Re-diffraction Re-diffraction optical systemoptical system
Function of the field lens : make a image of objective lens aperture onto Lyot stop Blocking diffraction fringe by
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Observation of the sun corona by coronagraph
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Front view of the coronagraph
4. Photographs of coronagraph
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Objective lens with anti-reflection disk to block reflected light from opaque disk
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Field lens
Lyot’s stop
View from the back side
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Fast gated camera set on the final focusing point
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Zoom up of opaque disk.
Shape is cone and top-angle is 45º
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Opaque disk assembly
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5. Background sources
1.Scattering by defects on the lens surface (inside) such as scratches and digs.
2. Scattering from the optical components (mirrors) near by coronagraph.
3. Reflections in inside wall of the coronagraph. Cover the inside wall with a flock paper (light trapping material).
4. Scattering from dust in air. Use the coronagraph in clean room.
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5-1. Scattering by defects on the lens surface such as scratches and digs.
With normal optical polishing, for example S&D 60/40 scattered light intensity : about 10-3 times of input light intensity.
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S&D 60/40 surface of the glass
5mm
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Result of careful optical polishing for the objective lens
5mm
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5-2. Scattering from the optical components (mirrors) near by coronagraph
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29401100
SR beam
electron beam orbit
Set up of SR monitor at the Photon factory
mirror
mirror
2900
source point
Scattering from Be-mirror is about 5x10Scattering from Be-mirror is about 5x10-7-7
Scattering from the mirror which set at 2m in Scattering from the mirror which set at 2m in front of coronagraph is aboutfront of coronagraph is about 6x106x10-5-5
coronagraph
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Low scattering noise mirror for optical path
To escape from scattering noise from mirrors in the optical path, we used back-coated mirror with well polished optical flat having a small wedge angle.
The wedge angle is necessary to separate surface reflection
Optical axis reflected by back Al coating
Optical axis of surface reflection
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6. Observation of beam tail (halo) at the Photon Factory, KEK
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Beam profile
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Beam tail
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Intentionally spread some dust on the mirror in 2m front of the coronagraph
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Lyot’s stop
Entrance pupil is intentionally rotated by 30º to recognize diffraction tail easily.
30°
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Move the opaque disk slightly to show the edge of central beam image (diamond ring!)
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65.8mA 61.4mA 54.3mA
45.5mA 35.5mA396.8mA
Multi-bunch bunch current 1.42mA
Beam tail images in the single bunch operation at the KEK PF measured at different current
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Single bunch 65.8mA
Exposure time of CCD : 3msec
Exposure time of CCD : 100msec
Intensity in here : 2.05x10-4 of peak intensity
2.55x10-6
Background leavel : about 6x10-7
Far tail
Observation for the more out side
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Strong tail in RF bucket
Weak tail in outside of RF bucket
1 101 201 301 401 501
RF bucket
1 101 201 301 401 501
x 33
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7. Conclusions• The coronagraph was designed and constructed for
the observation of weak object (such as tail and halo) surrounding from central glare of the beam.
• Optical polish of the objective lens is key point to realize good S/N ratio, and we reached ratio of background to peak intensity 6x10-7.
• Spatial resolution is about 50m• By using the coronagraph, we observe beam tail at
the photon factory storage ring. As results; 1. a strong beam tail was observed in inside of RF bucket 2. a weak, and wide-spread tail is observed in outside of RF bucket.
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Comments for possibility of SR monitor in LHC
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PF bend 2.5GeV 0.45A
LHC bend 7TeV 0.2A
Visible SR
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total
component
component
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Visible SR at 7TeV is ten times stronger than PF!
1. Stationary and dynamical beam profile observation via normal focusing method with fast gated camera.
2. Beam size measurement via SR interferometer with the spatial resolution better than few m.
3. Beam halo observation via coronagraph.
4. Temporal beam profile observation via streak camera.
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d
f
x2iexp)(F
fi
1)x(u
2
1
Intensity distribution on Lyot’s stop by
re-diffraction system is given by;
In here, F(is disturvance of the light on field lens
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The integration performs 1 and
: radius of
field lens
: radius of
opaque disk
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Geometrical image of the aperture of objective lens
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Block the re-diffraction fringes
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10-5
0.0001
0.001
0.01
0.1
0 2 4 6 8 10 12 14
holizontal beam size in
Diffraction tail
Bam tail
Comparison between beam tail and diffraction tail