the machined immersion grating - inafhires modes” volume 9908, ground-based and airborne...
TRANSCRIPT
The workshop on Dispersing Elements for Astronomy 2017 in Milan
The machined immersion grating for the absolute and simple solution of the
downsizing concept
in the high-precision infrared Spectroscopy
Takashi. Sukegawa
Oct 10,20171/33
Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
Outline
• Introduction First History in Canon
Original Machine capability
Conventional grating for IR
Image slicer
• Immersion grating
InP
Germanium
CdZnTe
• Conclusions
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Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
Introduction
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Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
What is first motivation in Canon?
There is the Key Device for our semiconductor business.
There was only one vendor for this device in 2010. We thought this
situation was one of the restrictions for our business cost.
Echelle Grating with the length of 360mm
General Requirement
Grooved pitch : FSR > 1nm @193.4nm
Grooved area : Length > 350mm Width > 55mm
Wavefront Error : < 30nmRMS 100nmPV (Flat or Concave)
Absolute Diffraction Efficiency : > 60%@193.4nm Required robustness against 193nm
Although we started the difficulty at not knowing first, at the end, it succeeded.
We learned and experienced a lot from this development.
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Original Machine potential
Free Form Mechanical Cutting tool
• High precision- Placement Error : < 2nm(RMS)
- Surface roughness : < 1nm(RMS)
50,000 grooves/mm
20nm/pitch
SEM
Machined Area
300mm x 200mm x 300mm
A machining with the accuracy
of UV grating is possible in 3D.
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Performances of UV grating by 3D machining
Direction of Grooving
56m
mMaster #1 Master #26nm RMS 32nm PV
85mm (355mm)
6nm RMS 33nm PV
Wavefront Error ( 31th-order at 632.8nm by Zygo interferometer)
Flatness of Diffraction Efficiency
90%
100%
110%
0 50 100 150 200 250 300 350
au (
vs a
vera
ge)
Position(mm)
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Micro Slicer for 2D spectrograph in SPACE
Designed by Suematsu-san (NAOJ)
Suematsu, et al. “Development of compact metal-mirror image slicer unit for optical telescope
of the SOLAR-C mission” SPIE 9904, Space Telescopes and Instrumentation 2016:
Optical, Infrared, and Millimeter Wave, 990411 (29 July 2016);
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Machined by CANON
Micro Slicer for 2D spectrograph in SPACE
July 2012 Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
9/33Micro Slicer for 2D spectrograph in SPACE
Machined by CANON
Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
Machined potential - 3D machining ~ e.g.②
Surface roughness 0.61nm RMS
200um
1mm
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Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
UV VL IRVUV
Reflective
Transmittance
Immersion
An Immersed grating is the absolute and simple solution of the
downsizing concept in the high-precision infrared Spectroscopy.
for Astronomy
The types of Grating currently offered by Canon
for Astronomy
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Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
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Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
A B
Before
Coating
After
Ag Coating
High Blazed echelle Grating for mosaicking
Grooved Length:198mm
Grooved width : 58mm Blaze angle: 79.3°
Apex angle: 88°Depth:
Pitch: 90.4um
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High Blazed echelle Grating for IR
Polarization A B
Absolute
Maximum
Diffraction
Efficiency
Average
TM 60.9% 61.3%
TE 76.2% 76.2%
Variation
(3 points ±65mm)
TM 1.9% 1.1%
TE 1.1% 1.2%
Surface Flatness
Area of 90%
PV 54.1nm 45.4nm
RMS 5.6nm 6.0nm
These performances are very close in manufactured individually.
Otsubo et al, “First high-efficiency and high-resolution (R=80,000) NIR spectroscopy with high-blazed Echelle grating: WINERED
HIRES modes” Volume 9908, Ground-based and Airborne Instrumentation for Astronomy VI; 990879 (2016)
Please refer to the following paper about the spectrograph (WINERED) which mounted the reflection
gratings by Canon.
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Immersion Grating
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Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
Characteristics of three materials for immersion
InP Ge CdZnTe
Refractive index 3.2 4.0 2.7
Practical Wavelength(Attenuation coefficient(α)<0.1/cm-1)
1.4μm~8μm 2μm~11μm 5μm~20μm
Low temperature operation
Size availability at the Blaze angle 75
~120mm
(85mm)~200mm ~85mm
not yet
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Potential of three materials for immersion
105
104
103
102
R(λ/Δλ)
1 5 10 20μm2
Assumption conditions
Blaze angle:75°Maximum Length
InP 85mm
Ge 200mm
CdZnTe 85mm
22,000
140,000100,000
CdZnTeGeInP
88,000
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CdZnTe immersion grating
2012 SPIE Astronomical Telescopes +Instrumentation Sukegawa et al
Applied Optics 2015 Ikeda et al
22mm
80mm
New View 3D
Surface roughness
3.2nm RMS
Mag : x30
Mag : x300
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Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
Germanium immersion grating with the length of 155㎜
x10.000
X500
5μm
42mm155mm
Groove Pitch 91.74um
Blaze Angle 75°
Apex Angle 85°
Machinability of germanium is the best for us currently. There are also almost no restrictions of
material.⇒ Today, introducing “EGIG” , “GRISM”
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Test of Low temperature operation
3980 3985 3990 3995 4000
Effi
cie
ncy
(1
DV
= 5
%)
Before(TM)After(TM)
Temperature cycle x 3times
Cooling speed : 250K/9h
Minimum 25K Ge immersion grating⇒No efficiency change
We did also a same test
for InP immersion grating.
⇒ No change
Other Reference
Sarugaku et.al,“Cryogenic Performance of High-
efficiency Germanium Immersion Grating” SPIE astronomical telescopes and instrumentation(2016)
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Grooved pitch : 476um for 3-5um Blaze angle : 75 degrees
Maximum Absolute Diffraction Efficiency : 78%@ 4um
EGIG : Extremely High-order Germanium Grating
Tani, et al. “Extremely-high-order Ge Immersion Grating-based Spectrometer for Offset-free
Precision Spectroscopy in the Mid-infrared Region” CLEO®/Europe-EQEC 2017
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Germanium Grism (GG)
Grooved pitch : 2.174um
Blaze angle : 19.19 degrees
Effective Size : Φ30mm
Mag : x10,000
5μm
Since one groove is machined each by each, an device like grism with a small pitch is extremally high cost.
Notice !!
Wavefront Error : 9nmRMS 47nmPV
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Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
InP immersion grating
x1000
X500050mm
Groove Pitch 47.3um
Blaze Angle 72°
Apex Angle 86°
20mm
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Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
Performance of InP immersion grating
+100nm
-100nm
Ruled Direction
(in an area 14.7 mm×18.9 mm)
Gro
ove
Dire
ctio
n
RMS 12.1nm
PV 53.5nm
50%
55%
60%
65%
70%
75%
80%
85%
1546 1547 1548 1549 1550 1551 1552Ab
solu
teD
iffr
acti
on
Eff
icie
ncy
(%
)
Wavelength(nm)
TM
TE
Max : 80%
Max : 70%
Order = 180th
Wavefront Error
Absolute
Diffraction
Efficiency
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Conclusions
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Items
Reflection(L200x60)
CdZnTe(L80x20)
Germanium(L112x32)
InP(L50x20)
Surface Flatnessin grooved areaby Littrow condition
6nm RMS
54nm PV
6nm RMS
40nm PV
7nm RMS
54nm PV
12nm RMS
54nm PV
Maximum AbsoluteDiffraction Efficiency
76%(TE)61%(TM)@1.5um
74%(TE)74%(TM)
@4um(189th)
80%(TE)75%(TM)
@4um(178th)
80%(TE)70%(TM)@1.5um(180th)
Typical Performances of our gratings
Copyright 2017 CANON INC. all rights reserved The workshop on Dispersing Elements for Astronomy 2017 in Milan
Commercial Availability of immersion
Item Typical performance
Size/Resolution ~200,000
Efficiency >70%
Wavefront Error < 20nm RMS
Scatter and Ghost < 10-4
Delivery Time < 1year
Cost ExpensiveWe consider that it is reasonable enough for its total cost of system miniaturization by immersed effect.
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Conclusions
• Canon succeeded in fabricating 3 types of
completed immersion echelle grating.
• Canon could also a reflective grating.
Canon’s grating is expected
small surface flatness ( <20nm RMS)
and high efficiency (60 to 80%).
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Major risk in “ made in JAPAN “
Earthquakes during processingAlthough it has several safety counter measures in our factory,
it is difficult to respond to the direct type earthquake.
In this case,
fortunately there was no
problem in practical use
and it was used for actual
spectroscopy
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