Lecture04 - Optical Alignment
description
Transcript of Lecture04 - Optical Alignment
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Alignment of Optical Systems
Robert E. Parks
Optical Perspectives Group, LLC5130 N. Calle la Cima
Tucson, AZ 85718
www.optiper.com
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Outline of talk
• What do we mean by alignment? – An example
• How is alignment done as an after-thought?
• How should alignment be done with fore-thought?
– In theory
– In practice, generally in two steps, coarse and fine
• Techniques for alignment
• Examples of aligning systems
• Talk really applies to prototype/high performance systems
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What is alignment all about?
• Points and lines – centers of curvature & axes
• Physical realizations of points and lines
• Their relative locations in 3-D space
• How to measure their locations
–Tools for alignment
–Methods
•Relative – such as reversal
•Absolute – with fixtures or stages
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What is optical alignment all about?
• Intrinsic alignment properties of lenses and mirrors
– How are centers of curvature and axes defined
– How are they located in practice
• Extrinsic alignment properties of optical systems to objects
and images
– How are C’s of C & optical axes aligned to mechanical
axes
– How do optical systems behave relative to their location
between object and image
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2
3
5
6
7 8 9
Surf Type Comment Radius Thickness Glass Diameter
OBJ STANDARD Source at ∞ Infinity Infinity 0
1 STANDARD Start of rays Infinity 5 0
2 STANDARD Front of corr. -11.78675 0.8307299 K5 12
3 STANDARD Back of coor. -12.51825 0 12
4 STANDARD Dummy surface Infinity 15.75064 0.002
STO STANDARD Primary mirror -39.67921 -15.75064 MIRROR 10.65653
6 STANDARD Sec. mirror -12.51825 16.08293 MIRROR 2.444401
7 STANDARD Front ff -6.645839 0.332292 K5 0.3703107
8 STANDARD Back ff Infinity 3.398446 0.3485696
IMA STANDARD Image plane Infinity 0.01195214
A typical example of an optical system
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1) Far points determine telescope axis – align to collimator
2) Align primary to left most point, align ff to 33.365 point, align corrector to 11.310 point
3) Light from collimator will focus at far right point and have good image quality
4) (Alignment order set by tooling and interference with already aligned optics)
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What is typically done for alignment?
• Satisfactory optical design produced by lens designer
• Designer does Monte Carlo tolerance analysis
– Every surface is perturbed – spacing, decenter(2), and tilt(2)
– Often done without thinking – one element is reference
• Tolerances used to make optical element & barrel drawings
– Tight tolerances lead to higher costs
– May be impossible due to thermal concerns
• Put parts together mechanically and test optically
– Take test results and analyze for what could produce observed errors
– Take apart, try to correct and re-assemble
– Do optical test again
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Drawing of corrector element
1) Edge diameter – affects decenter
2) Wedge – affects tilt and decenter
3) Seat – affect tilt and decenter
4) All must mate with barrel
5) Allowance for thermal excursion
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What should be done about alignment?
• Satisfactory optical design produced by lens designer
• Do tolerance analysis using some surface as a reference
– Perturb balance of surfaces – spacing, decenter(2), and tilt(2)
• Develop an alignment plan in concert with optical designer
– Barrel should have exterior datum features concentric with bores
– Establish reasonable tolerances along with alignment plan
• True barrel on rotary table
– Assemble each element so centers of curvature located within tolerance
• Use shims or intermediate cells and adjustment screws
– Simultaneously check element spacings and thicknesses
• Do optical test aligned to collimator or target
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Practical alignment
• Do coarse alignment to find center of curvature
• Set up autostigmatic microscope on return image
– Point microscope toward center of aperture or pupil
• Find center of field of microscope with cat’s eye
– Focus on a surface and mark location of return image in field of view
• Move microscope in 3 translations to center return image
– Return reflection should lie on top of cat’s eye return
– Return image should be as small as possible (in focus)
• Focus of microscope is now at the center of curvature of the
spherical surface
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Why should we have to think about this?
• Design programs are too much help
• Elements and systems appear pre-aligned
• Most optical systems are axi-symmetric
• Split in responsibility between optics and mechanics
– Relatively few opto-mechanical and test engineers
– Few have sufficient overlapping skills
– Lens designers held in too exalted regard
– No one likes to start over on any design
• Designs and drawings are a means of communication
– They are not sacred objects written in stone
– A jumping off point for more ideas
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Need for thinking about alignment now obvious
Have to establish an axis and C of C for each
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C’s of C easy to find optically
Edges define other end of axes
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1) Far points determine telescope axis – align to collimator
2) Align primary to left most point, align ff to 33.365 point, align corrector to 11.310 point
3) Light from collimator will focus at far right point and have good image quality
4) (Alignment order set by tooling and interference with already aligned optics)
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Why this exercise?
• Makes the alignment problem obvious at the design stage
• Like giving a print to a machinist –
– Person making part is quick to spot missing dimensions
– Same true for alignment – steps and equipment needed more obvious
• Center of curvature can be found very accurately
– With proper tooling to 1 part in 105 to 106 angle wise
– Center of curvature placement is critical for optical performance
– Aperture placement less important – uniform illumination
• Control of C of C by element edge is difficult
– Wrong end of lever arm
– Problem with tolerance build up
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Coarse alignment
• Find return (reflected) spot from surface in question
– Measure to find approximate axial location
– Use bright light source – optical fiber is good source
– Dim room lights and white paper around source
• Axial distance (focus) important
– 1 mW, 5 um spot at best focus in f/10 cone
– 10 uW when 1 mm from focus
– 100 nW when 10 mm from focus
– 1 nW when 100 mm from focus
• Set up translucent sheet at return spot for fine location
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Finding the C of C of a CC sphere
• Helpful if mirror has a reflective coating
• Helpful if approximate radius is known
• Move in close to mirror, right side up – inside C of C
• Close one eye, center eye, back away, eye blows up
• Place pointed object here, look for inverted reflection
• Helps to illuminate object from side
• Line up points, now have lateral location
• Scan head across mirror, motion of points, no focus
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Finding the C of C, first step
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Finding C of C, second step
Object inside C of C, image appears to
move as eye moves sideways
Object outside C of C, object appears to
move as eye moves sideways
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Autostigmatic microscope
• Microscope with an internal “point” light source at the long
focus of the microscope objective
• Microscope with an internal beamsplitter so reflected return
image of light source can be viewed in eyepiece
– Metalographic or reflected light microscope
• For ease of use should have a video camera to view image and
a means of varying light source intensity and camera
sensitivity
• The Point Source Microscope (PSM) is a commercial version
as is the Gamma Scientific Model 700-10-1A
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What is in the PSM?
Two internal light sources, lenses, beamsplitters and a mirror
Externally mounted are a digital CCD camera and a commercial objective
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How is the autostagmatic microscope used?
• Point microscope toward center of surface being located
• Focus microscope on the target from coarse alignment
• Turn on internal light source, focus to find cat’s eye reflection
• Mark center of focused return spot on video monitor screen or
in software display – this is the centering reference
– Best focus or smallest spot gives axial reference
• Move ASM to focus on the center of ball marking the desired
location of the center of curvature of the surface
– Center return spot on previously marked reference
– Remove ball and adjust surface under test so its return is centered and
well focused on reference
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How does the PSM work; at Cat’s eye?
A Cat’s eye reflection is gotten when focused on a surface
The return image is always centered; may not be in focus
Useful for calibration, set up and radius measurement
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Finding the C of C of a concave sphere
Locates two
lateral co-
ordinates, x,y
Locates axial
coordinate, z
For three
altogether
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Autostigmatic microscope
• Microscope illuminated with a point source of light via a beamsplitter
• Sometimes referred to as a Star tester for looking at images
• PSM is a commercial autostigmatic microscope with full field imaging
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Balls
• Balls are convex mirrors with a specific radius
• Bearing balls of grade 3 and 5 are optically good
• SiN bearing balls are better than chrome steel
– Better finish and roundness
– Better durability, they are harder
– More useful reflectivity for most alignment
– Diameter certified to 25 nm
• Either kind of ball is quite inexpensive
• Balls are the workhorses of alignment
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Finding the C of C of a convex sphere
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How does PSM work at center of curvature?
If the objective focus is
precisely at the center of
curvature of the spherical
mirror, the reflected light will focus to a tight spot in
the center of the detector
If the objective focus is
not at the center of
curvature the reflected
spot will, in general, not
be centered or in focus.
PSM Align© tells how far
from center and how big is the spot diameter.
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Using the PSM
• In many ways like the alignment telescope
• Focus on a surface to get a Cat’s eye return
• Set reference crosshair on the Cat’s eye return
• Move PSM so it is focused at the C of C of an alignment datum
– Usually the center of a ball, sometimes axis of a cylinder
– Focus will control 3 degrees of freedom when centered and focused in
crosshair
• Remove ball or cylinder
• Adjust lens or mirror until light is centered and focused on crosshair
• Done; move on to next surface
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Example of return image
With crosshair centered on cat’s eye
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Main use of first PSM
• Align centers of curvature of a series of lenses, toroids and
mirrors to a common axis as they were installed
Uses the functional aspect of the optical element; the optical surface
Eliminates mechanical tolerance build up
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Aligning a fixture with the PSM
Display
Fixture
Ball
Metering rod
PSM
X-y-z stage
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Aligning prisms
Prisms Prism cage Ball to mark focus PSM
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Spectrometer example
Entrance slit
Exit slit
Fold mirror
Grating
Fold mirror
Entrance slit
Entrance
collimator
Exit
decollimator
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Alignment of a grating spectrometer
Entrance slit
Exit slit
Grating
Collimating
mirrorsFold mirrorCenters of curvature
of collimating mirrors
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First alignment step
Entrance slit
Exit slit
Center of rotation of grating
C of C of entrance collimator
C of C of exit decollimator
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Second alignment step
Grating
Ball conjugate with
entrance slit
Ball at entrance slit
Ball at exit slit
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Final alignment step
Ball at entrance slit
Ball at exit slit
Fold mirror
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Tools for alignment
• Autocollimators
• Alignment telescopes
• Autostigmatic microscopes
• Stands for holding the above
• Rotary tables with tilt and decenter stages
• Sine plates, angle gauge blocks, optical squares
• Plug gauges and balls
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Autocollimating alignment telescopes
• Focus from about 0.5 m to infinity
• Project crosshairs – useful as an autocollimator
• Establishes a line of sight over focus range
– Position, angle and distance – 5 DoF
– Good for setting non-optical targets in a line
– Can align centers of curvature
– Have fairly narrow field of view
• Most have 2.25” barrels to fit standard mounts
• Davidson, Bronson, K&E, Taylor-Hobson
• Used instruments - www.bscoptics.com/tooling1.htm
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AutocollimatorsJust work at infinity focus
• Nikon 6B/6D and stand
– 2 translations and 3 angle adjustments
– Objective focuses, 70 mm aperture
– 0.5 second resolution
• Davidson D-660 and stand
– 2.25” barrel and 1.7” aperture
• Electronic autocollimators
– PSM without the objective
– 6 mm aperture
www.davidsonoptronics.com/poa.htm
Information on how to use an auto-
collimator to make various kinds of
angular measurements
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Using autocollimatorsMeasuring angles between two plane surfaces
• Locate the return reflection off surface one
– May need bright light in eyepiece and dim room lights to find reflection
• Find reflection off surface two
– May need sine plate or angle blocks if angle difference large
• In general, angle off in two directions
– Rotate one surface until crosshairs are aligned in one direction
• Angle between surfaces is read off separated crosshairs
– Factor of two in reflection is accounted for in scale reading
– Wedge opens parallel to single crosshair
• Tip surface to find direction of angle
– Kill back surface reflection on optical flat with contact paper
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Sine plate and angle gauge blocks
• Single axis and compound sine plates – used with Jo blocks
• Angle gauge blocks – wrung up like Jo blocks
– Set angles to 1 second with few blocks
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Using alignment telescopes
• Focused at ∞, alignment telescope is an autocollimator
• Focuses like camera on near targets
– Illuminating target helps seeing target
– If target is polished, will see centered reflected crosshair
• This is cat’s eye reflection – it can be confusing
• If AC on flat, then focus on flat, will see centered crosshairs
• Reflected cross should lie on top of crosshair in eyepiece – check
• For long radius spheres may get crosshair from center of curvature of sphere
– can align to eyepiece crosshair
– Good way to get centers in a line
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Using alignment telescopes 2Axis defined by normal to flat and point
• Focus at ∞ and tip-tilt AT mount to autocollimate off of flat
• Focus on point and translate mount to center point on crosshairs
• If AT did not tip-tilt during translation – done
• Focus at ∞ and check autocollimation – touch up if needed
• Then focus on point and translate if needed
• Done when aligned at both focus positions
• If flat can be tipped, procedure can be reversed
– Align first on point and then adjust flat to AT
– Axis of AT is then the axis of the setup
• This mode (point and normal) of alignment is the easiest to do
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Using alignment telescopes 3Axis defined by two points
• Order is important, rotate to align on far point, translate to near
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Mechanical tooling
• Good mechanical tooling is inexpensive
– Also optically as good as most optics
– SiN balls – better finish and roundness than metal
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Alignment using aberrations
• Spheres and spherical (stigmatic) wavefronts have no aberrations
– Spheres propagate as spheres; they don’t change shape
– Can fold inputs & outputs of optical systems
• Aspheres & many wavefronts inside optical systems are aspheric
– These wavefronts have axes and change shape
– Axes must go through centers of curvature, or get aberrations
• These aberrations can be used for alignment purposes
– Moving correctly if aberrations get smaller
– Often hard to tell if seriously misaligned
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R-C telescope model for alignment
750 mm diameter telescope, 4500 mm focal length, f/6 system, f/2.5 primary
Primary and secondary are both hyperboloids, primary is almost a paraboloid
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Alignment of primary mirror
Put microscope in mechanical
center of telescope tube
Point telescope until image
centered on microscope
Decenter primary and point
telescope until image is symmetric
(Spots 3.2 mm off axis or 0.18)
Spot large because hyperbola 230
µm diameter
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Secondary mirror alignment
Place PSM at mechanical
center of field
Tilt secondary to get light
centered on PSM
While keeping spot
centered, tilt and decenter
secondary to make
symmetric image
There should be symmetry
in field if no error in mirrors
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How well does the telescope image?
Image quality is symmetric about center of field
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What about misalignment?
Here’s what happens for a 0.1 mm secondary decenter
Spot is now one pixel big, any defocus throws light outside pixel
Asymmetry is the same direction for all points in the field
Shadow of secondary is obviously decentered
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What does an off-axis mirror look like?
parabola
sphere
vR
zdr
h
a
r
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Off-axis conic mirrors - math
x = x’ + h and y = y’
x’ = ax” and y’ = ay” so that x”^2 + y”^2 = ρ2 where 0≤ρ≤1
K+=8
43rc
z vκδ
( ) ( )[ ]22"2"3
8ayhax
cz v ++=
κδ
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Off-axis mirrors – math results
48
430
4
acb vκ
=
6
331
3
hacb vκ
=
4
223
2
2
hacb vκ
=
( )16
4 42230
2
ahacb v +
=κ
( )3
23 3331
1
haahcb v +
=κ
( )24
63 42243
0
0
ahahcb v ++
=κ
(spherical aberration)
(coma)
(astigmatism)
(focus)
(tilt)
(piston)
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Off-axis mirrors – contour maps
-1 0 1-1
-0.5
0
0.5
1Delta z over full aperture
a 0,0=-8.000a -1,1= 0.000a 1,1= 0.000a -2,2= 0.000a 0,2=-12.00a 2,2= 0.000a -3,3= 0.000a -1,3= 0.000a 1,3= 0.000a 3,3= 0.000
-1 0 1-1
-0.5
0
0.5
1sub-aperture, h = .6, a = .4
a 0,0=-2.026a -1,1= 0.000a 1,1=-3.583a -2,2= 0.000a 0,2=-1.024a 2,2=-0.921a -3,3= 0.000a -1,3= 0.000a 1,3=-0.410a 3,3= 0.000
-1 0 1-1
-0.5
0
0.5
1Piston and tilt removed
a 0,0= 0.000a -1,1= 0.000a 1,1= 0.000a -2,2= 0.000a 0,2=-1.024a 2,2=-0.921a -3,3= 0.000a -1,3= 0.000a 1,3=-0.410a 3,3= 0.000
-1 0 1-1
-0.5
0
0.5
1Piston, tilt & power removed
a 0,0= 0.000a -1,1= 0.000a 1,1= 0.000a -2,2= 0.000a 0,2= 0.000a 2,2=-0.921a -3,3= 0.000a -1,3= 0.000a 1,3=-0.410a 3,3= 0.000
-1 0 1-1
-0.5
0
0.5
1Astigmatism also removed
a 0,0= 0.000a -1,1= 0.000a 1,1= 0.000a -2,2= 0.000a 0,2= 0.000a 2,2= 0.000a -3,3= 0.000a -1,3= 0.000a 1,3=-0.410a 3,3= 0.000
-1 0 1-1
-0.5
0
0.5
1Astigmatism & coma removed
a 0,0= 0.000a -1,1= 0.000a 1,1= 0.000a -2,2= 0.000a 0,2= 0.000a 2,2= 0.000a -3,3= 0.000a -1,3= 0.000a 1,3= 0.000a 3,3= 0.000
![Page 58: Lecture04 - Optical Alignment](https://reader031.fdocuments.in/reader031/viewer/2022020111/563dbb99550346aa9aae99b9/html5/thumbnails/58.jpg)
Alignment of off axis mirrors
• Two steps to alignment – crude and fine
• Crude done from center of curvature
• Aberration seen from C of C is astigmatism and coma
• Image looks like a fish with tail pointing toward optical axis
• Correct azimuthal orientation and position C of C
• Then set up autocollimation test for fine adjustment
• Off-axis mirror angle is correct following crude alignment
• Locate autostigmatic microscope at correct focus
• Adjust autocollimating mirror for autocollimation
• Adjust off axis mirror while keeping image center in PSM
![Page 59: Lecture04 - Optical Alignment](https://reader031.fdocuments.in/reader031/viewer/2022020111/563dbb99550346aa9aae99b9/html5/thumbnails/59.jpg)
Representative images for crude alignment
![Page 60: Lecture04 - Optical Alignment](https://reader031.fdocuments.in/reader031/viewer/2022020111/563dbb99550346aa9aae99b9/html5/thumbnails/60.jpg)
Representative images for fine alignment
![Page 61: Lecture04 - Optical Alignment](https://reader031.fdocuments.in/reader031/viewer/2022020111/563dbb99550346aa9aae99b9/html5/thumbnails/61.jpg)
System to be alignedAdaptive optics for atmospheric wavefront correction
Gemini Adaptive Optics Bench
Telescope Focal Plane
LGS WFS (provided by others)
Pick-off mirror (provided by Gemini)
AOB Fold Flat (provided by Gemini)
Entrance Shutter
Exit Shutter
Focal Plane
NGS SS LGS SS
Deploy into beam
Fold Flat #1
OAP #1
DM0
DM1
DM2
Tip-tilt
Science ADC
Fold Flat #2
OAP #2
OAP #3
NGS Flat #1NGS ADC NGS
Flat #2
NGS Field Corrector
NGSFocal Plane
LGSBeamSplitter
NGSBeamSplitter
![Page 62: Lecture04 - Optical Alignment](https://reader031.fdocuments.in/reader031/viewer/2022020111/563dbb99550346aa9aae99b9/html5/thumbnails/62.jpg)
Simplified view of same systemRays in center of field only
Telescope focus
Conjugate telescope focus
OAP #2 OAP #1