conceptual design review
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Conceptual Design Review. Stray Light Rob Hubbard Systems Engineering. Definition of Terms. Stray light is unwanted light Most problematic when observing faint objects near the sun. Possible causes include Scatter from optical or mechanical surfaces Ghost reflections - PowerPoint PPT PresentationTRANSCRIPT
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Conceptual Design Review
Stray LightRob Hubbard
Systems Engineering
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Definition of Terms
• Stray light is unwanted light• Most problematic when observing faint objects
near the sun
•Possible causes include
–Scatter from optical or mechanical surfaces
–Ghost reflections–Edge scatter or “glints”–Diffraction around edges
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The Science Requirement
…The total instrumental scattered light (dust plus mirror roughness) shall be 25 millionths or less at 1000 nm and at 1.1 radii. Values larger than these levels require longer integration times to achieve the desired signal to noise levels.
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Relevant Studies Performed
• Some Stray-Light Reduction Design Considerations for ATST (Andrew Buffington and Bernard V. Jackson, UCSD)
• M1 Microroughness and Dust Contamination (Rob Hubbard, ATST Systems Engineering)
• Further Stray-Light Reduction Design Considerations for ATST (Andrew Buffington, UCSD)
• Advanced Technology Solar Telescope (ATST) Stray and Scattered Light Analysis (Scott Ellis, Richard N. Pfisterer, Photon Engineering, LLC)
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• “Sunlight reflected from the heat shield/coronagraph occulter does not need to be absorbed nearby, and can be safely dumped into the interior of the building; and…”
• “Except maybe close to the M1 mirror mount, the building interior can be typical black or even gray paint, without generating significant stray light in the FOV.”
• “Specifying, manufacturing, testing and certifying M1 could prove a significant challenge for ATST.”
• “ATST’s success as a coronagraph probably requires aggressive contamination control, even if a low-dust site is found…”
Some Stray-Light-Reduction Design Considerations for ATST(July 2002)
Buffington and Jackson
Conclusions:
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Extending the Analysis
• Can we make additional assumptions that will allow us to better quantify the scattering due to M1 microroughness?
• Can we refine the dust contamination predictions so that they can be compared to scatter due to M1 microroughness?
• How frequently will the ATST primary mirror need to be cleaned to maintain acceptable coronagraphic performance?
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ATST Technical Note No. 0013
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1.11.52.0
Sample Positions
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Typical scatter versus angle for a clean, polished glass surface
The Scatter Model
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…In direction-cosine space
Plotting log10 | sin – sin 0 | versus log10 BSDF
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Figure courtesy of Gary Peterson, Breault Research Organization; measurement by James Harvey.
S
bBSDF
01.0
)sin()sin( 0
2
1002
SbTIS
S
Harvey Model
= 0.57º
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Even and small angles?
1.11.52.0
1.6 arcmin
sin 0.0005
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Power Spectral Density
Church, Eugene L.,” Fractal Surface Finish,” (Applied Optics 27, No. 8, 15 April 1998.)
~40 arcsec (from grating equation)
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Profile of a Star
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The Profilometer and Roughness
22
2
1L
LL
Lim z x z dxL
!
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2
1002
42
SbTIS
S
Microroughness and Harvey
The single RMS roughness parameter () contains insufficient information to completely characterize the BSDF of the polished surface, even assuming a power-law relationship.
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1.E-05
1.E-04
1.E-03
1.E-02
1.E-01
1.E+00
1.E+01
1.E+02
1.E+03
0.0001 0.0010 0.0100 0.1000 1.0000
S = -1.5
S = -1.6
S = -1.7
S = -1.8
Slope Ranges
Angle (Degrees)
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Microroughness – 20 Ångstrom s=-1.5
0.0E+00
2.0E-06
4.0E-06
6.0E-06
8.0E-06
1.0E-05
1.2E-05
1.0 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2.0 2.1
Distance from Sun Center (solar radii)
Rat
io t
o O
n-D
isk
Irra
dia
nce
20 A -1.5
= 1.0 Micrometer
The 20 Ångstrom Finish
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Two Sample Polishes
0.0E+00
2.0E-06
4.0E-06
6.0E-06
8.0E-06
1.0E-05
1.2E-05
1.0 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2.0 2.1
Distance from Sun Center (solar radii)
Rat
io t
o O
n-D
isk
Irra
dia
nce
20 A -1.5
12 A -1.5
= 1.0 Micrometer
The Likely Finish
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R/Rsun S = –1.5 = 12 Å
S = –1.5 = 20 Å
S = –1.8 = 12 Å
S = –1.8 = 20 Å
1.1 3.93×10-6 10.9×10-6 10.5×10-6 29.3×10-6
1.2 3.20×10-6 8.90×10-6 8.03×10-6 22.3×10-6
1.3 2.72×10-6 7.55×10-6 6.51×10-6 18.1×10-6
1.4 2.36×10-6 6.57×10-6 5.45×10-6 15.2×10-6
1.5 2.08×10-6 5.77×10-6 4.63×10-6 12.9×10-6
1.6 1.85×10-6 5.14×10-6 4.01×10-6 11.1×10-6
1.7 1.67×10-6 4.64×10-6 3.53×10-6 9.82×10-6
1.8 1.52×10-6 4.21×10-6 3.13×10-6 8.71×10-6
1.9 1.38×10-6 3.84×10-6 2.80×10-6 7.79×10-6
2.0 1.27×10-6 3.53×10-6 2.52×10-6 7.02×10-6
Range of values
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Figure courtesy of Gary Peterson, Breault Research Organization.
Dust Contamination
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The number of particles per square foot with diameters greater than s microns is given by:
log(n) = 0.926 [ (log(c))2 - (log(s))2 ]
s = particle diameter (m)c = cleanliness leveln = number of particles per square-foot with diameters greater than s
n 500 s( )
n 300 s( )
n 100 s( )
s1 10 100 1 10
31
10
100
1 103
1 104
1 105
1 106
1 107
# of Particles Over a Given Diameter
Particle Diameter
Num
ber
of P
arti
cles
Courtesy of Gary Peterson, Breault Research Organization.
MIL-STD 1246C
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0.001 0.01 0.1 1 10 100Scattering A ngle, D egrees
1E -006
1E -005
1E -004
1E -003
1E -002
1E -001
1E +000
1E +001
1E +002
1E +003
1E +004
1E +005
1E +006
1E +007
1E +008
BR
DF
(p
er s
tera
dia
n)
AB g = 2.5 e-6, 1 e-13, 3
AB g = 2.5 e-6, 1 e-9, 3
AB g = 2.5 e-6, 1 e-5, 3
AB g = 4 e-5, 1 e-8, 2
AB g = 4 e-5, 1 e-4, 2
S pyak an d W olfe (1992), 0.6 n m(3 m on th s exposu re)
Buffington and Jackson
• Measurements are only available to within a degree of the specular direction.
• We know the linear relationship cannot go on indefinitely and retain a finite TIS.
• The roll-off will likely occur right in our angular domain, so knowledge of the position of the “knee” is critical to dust analysis.
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Roll-off in the IR (10 microns)
From Spyak and Wolfe, Scatter from particulate-contaminated mirrors, Part 3
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Harvey 1 Harvey 2b b0 l s %TIS 1 b b0 l s % TIS 2 % Sum
7.000E-02 0.156739 0.007 -2.26 0.0135 0.00754 2.5014E-05 0.59 -1.4 0.004569 0.0180
The Mie Model for 0.01% Coverage (Level 230)
Harvey Fit to Mie Data
1.E-06
1.E-05
1.E-04
1.E-03
1.E-02
1.E-01
1.E+00
0.0001 0.0010 0.0100 0.1000 1.0000
Sine Theta
BS
DF
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Mie at 0.01% Compared to Microroughness
0.0E+00
1.0E-06
2.0E-06
3.0E-06
4.0E-06
5.0E-06
6.0E-06
7.0E-06
8.0E-06
9.0E-06
1.0E-05
1.0 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2.0
Distance from Sun Center (solar radii)
Ra
tio
to
On
-Dis
k I
rra
dia
nc
e
0.01% coverage
12 A Microroughness
Mie at 0.01% Compared to Microroughness
0.0E+00
1.0E-06
2.0E-06
3.0E-06
4.0E-06
5.0E-06
6.0E-06
7.0E-06
8.0E-06
9.0E-06
1.0E-05
1.0 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2.0
Distance from Sun Center (solar radii)
Ra
tio
to
On
-Dis
k I
rra
dia
nc
e
0.01% coverage
12 A Microroughness
Dust results at 1 Micron
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Dust accumulation
UKIRT Emissivity versus Time
y = 0.0011x + 0.2
0.0000
0.5000
1.0000
1.5000
2.0000
2.5000
3.0000
3.5000
0 500 1000 1500 2000 2500
Hours
Rel
ativ
e E
mis
sivi
ty
UKIRT Emissivity versus Time
y = 0.0011x + 0.2
0.0000
0.5000
1.0000
1.5000
2.0000
2.5000
3.0000
3.5000
0 500 1000 1500 2000 2500
Hours
Rel
ativ
e E
mis
sivi
ty
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Scatter with Accumulation
0.0E+00
2.0E-05
4.0E-05
6.0E-05
8.0E-05
1.0E-04
1.2E-04
1.4E-04
1.6E-04
1.8E-04
1.0 1.2 1.4 1.6 1.8 2.0
Distance from Sun Center (solar radii)
Ra
tio
to
On
-Dis
k I
rra
dia
nc
e
Microroughness
0.01% Coverage
1 Day (0.063%)
1 Week (0.38%)
Accumulation with time
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Apache Point Accumulation Rates
0
0.01
0.02
0.03
0.04
0.05
0.06
0.07
0.08
0.09
0.1
0 20 40 60 80 100 120 140 160 180 200
Hours
Fra
ctio
nal
Co
vera
ge
Rate of change ≈ 0.04% per hour!
40 Times faster at Apache Point
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Kitt Peak Dust Experiment
• At what rate does dust accumulate in the McMath-Pierce tunnel?
• What is the distribution of particle sizes?
• What affect does an air knife have on dust accumulation rates?
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A Large Compressor!
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The Experiment
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The Air Knife and Samples
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Super Air Knife by Exair
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24-Hour Accumulation
330 m
200 Magnification
10 m
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The Need for Clean Air
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Dust Scatter vs. Wavelength
Dust BSDF at 1, 3, and 10 microns
-6
-5
-4
-3
-2
-1
0
-3.0 -2.5 -2.0 -1.5 -1.0 -0.5 0.0
Log(Beta)
Lo
g(B
SD
F)
1 Micron
3 Microns
10 Microns
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Other Stray Light SourcesREFLECTED LIGHT FROM THE SUN (YELLOW)
WHAT THE GREGORIAN FOCUS SEES (BLUE)
REFLECTED LIGHT FROM THE SUN (YELLOW)
WHAT THE GREGORIAN FOCUS SEES (BLUE)
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Relative Contributions
Scattered Power - Gregorian Focus
0
0.005
0.01
0.015
0.02
0.025
0.03
0.035
0.04
0.045
0.05
Primary Mirror(M1)
Secondary Mirror(M2)
Everything Else
Po
we
r @
Co
ud
e Im
ag
e
With Dome
No Dome
Rel
ati
ve
Co
ntr
ibu
tio
n
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Conclusions from the Reports
“Scattering due to dust contamination of the primary mirror would appear to be the most serious stray-light concern for coronagraphic observations. The accumulation of dust on the primary quickly overwhelms the effects of surface microroughness from the polishing process.”
Mie at 0.01% Compared to Microroughness
0.0E+00
1.0E-06
2.0E-06
3.0E-06
4.0E-06
5.0E-06
6.0E-06
7.0E-06
8.0E-06
9.0E-06
1.0E-05
1.0 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2.0
Distance from Sun Center (solar radii)
Rat
io t
o O
n-D
isk
Irra
dia
nce
0.01% coverage
12 A Microroughness
M1 Microroughness and Dust Contamination:
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Dust Dominates
• In situ washing is already part of the baseline plan.
• Operational procedures will have to be developed (as with any telescope) that establish criteria for “safe exposure” of the telescope to high winds in high-dust situations.