Title: SSRF Long Trace Profiler with an innovative design
1SSRF Long Trace Profiler with an innovative
design
Shanghai Symposium on Intermediate-energy Light
Source 2426/9/2001
Tiqiao XIAO and Shaojian XIA
Shanghai National Synchrotron Radiation
Center Shanghai Institute of Applied Physics, CAS
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What for?
SSRF Beamline Construction
- 2-30keV hard X-ray widely used
- grazing angle 2.56mrad is required
- strip like mirror around 1 meter long
- precision for surface profile reach 1mrad
- widely use of bent mirror
- dynamic measuring of mirrors under different
moment - dynamic measure the effect of gravity compensation
- mirrors with large size and high precision
- difficult to control the quality for suppliers in
the world
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Table 1. Long mirrors for the first set of
beamline at SSRF
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laser beam
scanning
surface under test
mirror
gravity
compensator
compensator
Figure 1. Setup for measurement to the
compensation of mirror gravity
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Requirements on metrology instrument
- Large scanning range 12 m
- high repeatability 1mrad
- high resolution 0.1?0.2mrad
- applicable for measurement on mirrors with
different surface profile
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- Available commercialized instruments,such as
WYKO,ZYGO et al.,their characteristics - wide beam,in principle size of elements measured
equals to beam size - applicable for regular profile measurement
generally - expensive for large caliberF152 (1 million RMB)
-
F600(1 million USD)
Blind alley!
Pave a different way
Scan with a pencil beam LTP
7Table 2. Some of LTP in the world
Shanghai Symposium on Intermediate-energy Light
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During RD of SSRF, we wanted to do something.
We decided to develop a long trace profiler by
ourselves.
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Goal
Preliminary scanning range 1.2m
repeatability 1.0mrad resolution
0.1mrad
In fact scanning range 350mm
repeatability 3.0mrad resolution
0.5mrad
develop an LTP on the basis of successful solve
of some key techniques
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- Key techniques to be solved
- f-q system based on phase plate diffraction
- compensate to system errors employing area array
CCD - approaches to reduce the effect of environmental
noises, such as temperature shift, air
turbulence et al. - software amend to system errors
- data collection and processing
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Principle for measuring minute profile change
with pencil beam
detector
q
P
2q
d
P
q d/2l
Set d9mm,l 10m, detectable maximum change
0.45mrad correspondent minimum radius 2.3km
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- The supreme problem is how to measure d value
precisely
- Factors that affect
- sourcefrequency,polarization,spatial mode
- light transmit mediaair turbulence,temperature
shift - mechanic stabilityvibration,inertial stress
release - optical elementsmaterial uniformity, process
quality - detectorssignal-to-noise ratio,dynamic range
- approaches for data processing
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Schematic diagram proposed by Bieren
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ppLTP by Qian Shinan et al.
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Disadvantages of ppLTP
- Sensitive to environmental noises, such as
temperature shift, air turbulence - strict requirements on the light source stability
in frequency, spatial mode, polarization et al
We have to keep cautious to every step during
measuring
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BS
x
z
PP
y
f
FT Lens
Focal Plane
SUT
Diode Laser
Optical fiber
Schematic diagram for the innovative design of
SSRF LTP
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Advantages of our design
- Restricts on light source greatly decreased
- Effect of environmental factors on precision
greatly reduced,insensitivity to noises improved - Instrument structure simplified
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Results
Repeatability
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Nominal parameters for SSRF LTP
Scanning range10350mm Accuracy 0.5mrad Static
stability0.1mrad/200s Acceptance
8mrad maximum measurable mirror
length1200mm Profilearbitrary
Measuring environment Room with no air
condition and with 1-2 person in
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Future plan
Develop a Long Trace Profiler with 1.5 meters
scanning range, employing the phase-plate
diffraction based f-q system
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Acknowledgement
Fruitful discussion with Dr. A.K.Freund, Dr.
O.Hignette from ESRF are highly appreciated
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Thanks!