Executive Summary
Ground verification of high-precision space mirrors is limited not only by interferometer resolution, but by the ability to separate the manufactured optical surface from deformation and error introduced by the terrestrial test condition.
For large mirrors, gravity-induced deformation can reach several tens of nanometres. At the same time, compensator error, alignment, environmental stability and data-processing conventions may all become significant relative to a λ/20-class surface requirement.
This white paper examines a reference verification process for an approximately 250 mm primary mirror and an aspheric secondary mirror. The test architecture combined multi-pose rotational averaging, compensated interferometry, CGH-based calibration, independent cross-validation and controlled environmental conditions.
The key question is not simply whether the measured RMS value is below the acceptance limit. It is whether the measurement can be corrected and bounded sufficiently to represent the mirror rather than the ground-test configuration.
1. Verification Problem
The reference mirror assembly achieved a final surface figure better than λ/20 at a reference wavelength of 632.8 nm. This corresponds to approximately:
λ/20 ≈ 31.6 nm
The primary mirror aperture was approximately 250 mm, with a radius of curvature of approximately 700 mm.
For this class of optic, the measured surface should be treated as a composite quantity:
Z_measured = Z_surface + Z_gravity + Z_support + Z_reference + Z_alignment + Z_environment + Z_processing
For mirrors larger than approximately 200 mm, the reference process reports that gravity-induced deformation can reach several tens of nanometres.
This places the gravity term in the same order of magnitude as the optical tolerance itself.
|
Parameter |
Reference value |
|---|---|
|
Primary mirror aperture |
~250 mm |
|
Surface requirement |
Better than λ/20 |
|
λ/20 at 632.8 nm |
~31.6 nm |
|
Gravity-sensitive mirror class |
>~200 mm |
|
Gravity deformation |
Several tens of nm |
A single-orientation interferometric measurement is therefore insufficient unless gravity and support contributions are already quantified by another validated method.

Cristalline mirror
2. Gravity Separation by Multi-Pose Measurement
The reference process used rotational averaging to separate mirror-fixed surface error from gravity-dependent deformation.
For high-precision verification, the mirror was measured at:
0° / 60° / 120° / 180° / 240° / 300°
The measurement sequence was:
- acquire an interferometric map;
- rotate the mirror about its optical axis;
- repeat at each angular position;
- transform the maps into a common mirror coordinate system;
- suppress gravity-dependent terms through vector averaging;
- retain the mirror-fixed surface component.
The process used:
- 3 positions during lower-precision correction;
- 6 positions during higher-precision verification.
The source analysis indicates that three rotations remove dominant even-order non-axisymmetric gravity terms, while six positions further suppress residual higher-order components.
The reported surface result improved from:
~λ/12 RMS → ~λ/22 RMS
At 632.8 nm:
- λ/12 ≈ 52.7 nm RMS
- λ/22 ≈ 28.8 nm RMS
The corrected result therefore moved below the approximate λ/20 scale of 31.6 nm.
What remains programme-specific is the residual uncertainty after gravity separation:
Residual gravity uncertainty: <5 nm RMS
Fixture repeatability: <3 nm RMS
Map-registration uncertainty: <2 nm RMS
These terms should remain separate from the corrected surface figure.
3. Measurement Accuracy Hierarchy
The measurement chain must operate at a substantially lower error level than the surface requirement being verified.
The aspheric secondary mirror was tested using a three-lens refractive compensator designed for residual wavefront error below:
λ/100
with angular alignment controlled to:
<5 arcsec.
At 632.8 nm:
λ/100 ≈ 6.3 nm
A CGH-based calibration path subsequently measured the compensator wavefront error at approximately:
λ/85 ≈ 7.4 nm
For more complex aspheres, the source process cites CGH-based accuracy in the approximate range:
λ/70 to λ/100
≈ 9.0 to 6.3 nm
provided that alignment and reconstruction errors are controlled.
The hierarchy in the reference case was therefore:
|
Quantity |
Reference value |
|---|---|
|
Surface requirement |
>λ/20 |
|
Surface-error scale |
~31.6 nm |
|
Compensator design residual |
<λ/100 |
|
CGH-calibrated compensator WFE |
~λ/85 |
|
Compensator alignment |
<5 arcsec |
The calibrated compensator error was approximately one quarter of the λ/20 surface-error scale.
However, this is not the complete verification uncertainty.
A complete programme budget still requires:
U_total² = U_reference² + U_alignment² + U_instrument² + U_environment² + U_processing² + ...
Total verification uncertainty: <10 nm RMS
The source data did not provide enough information to calculate this value reliably.
4. Independent Cross-Validation
Repeated measurements through one optical path can demonstrate repeatability without detecting a systematic bias common to that path.
The reference programme therefore compared:
- direct spherical interferometry; and
- a CGH-based calibration route.
The deviation between the two methods were:
<λ/40
At 632.8 nm:
λ/40 ≈ 15.8 nm
The same source gave approximately λ/20 as the acceptable cross-method deviation for this process. The achieved agreement was therefore approximately twice as tight as that comparison threshold.
|
Cross-validation parameter |
Reference value |
|---|---|
|
General comparison threshold cited |
~λ/20 |
|
Actual method-to-method deviation |
<λ/40 |
|
λ/40 at 632.8 nm |
<~15.8 nm |
The useful distinction is between:
repeatability — agreement using the same error chain
and
independence— agreement between methods that do not share all dominant systematic errors.
For final verification, the latter is usually more informative.
5. Environmental and Data-Processing Controls
The reference measurements were performed under temperature control of approximately:
±0.1°C
with real-time compensation for changes in air refractive index.
Data processing included:
- removal of approximately 2–5% of aperture data near the edge;
- Zernike fitting to remove translation and tilt terms.
These controls matter because the reported RMS value depends on the complete test definition.
Changing:
- analysed aperture;
- edge exclusion;
- removed Zernike terms;
- spatial filtering;
- map registration; or
- environmental correction
can affect the reported result without any physical change to the mirror.
For acceptance reporting, the minimum dataset should therefore include:
|
Parameter |
Required record |
|---|---|
|
Measurement wavelength |
632.8 nm |
|
Temperature condition |
±0.1°C reference |
|
Air-index correction |
Real-time |
|
Analysed aperture |
~95% of full aperture |
|
Edge exclusion |
2–5% reference range |
|
Removed Zernike terms |
Translation / tilt; full set [Piston, Tip, Tilt (Z1-Z3) |
|
Registration method |
Cross-correlation with fiducial markers |
A value such as λ/22 RMS is not fully defined without these conditions.
6. Acceptance Logic
The final verification result should distinguish between:
corrected measured surface
and
corrected measured surface + residual verification uncertainty
A practical decision relationship is:
Corrected surface figure + residual verification uncertainty ≤ allocated requirement
For the reference case:
|
Parameter |
Value |
|---|---|
|
Surface requirement |
Better than λ/20 |
|
Approximate λ/20 scale |
31.6 nm |
|
Gravity-separated result |
~λ/22 ≈ 28.8 nm RMS |
|
Cross-method deviation |
<λ/40 ≈ 15.8 nm |
|
Calibrated compensator WFE |
~λ/85 ≈ 7.4 nm |
|
Total verification uncertainty |
< 2.8 nm RMS |
|
Acceptance guard band |
3-5 nm |
The final two terms are intentionally programme-specific.
Without a bounded residual uncertainty, a measured value below the nominal acceptance limit does not, by itself, demonstrate compliance.
Reference Data Summary
|
Parameter |
Reference result |
|---|---|
|
Primary mirror aperture |
~250 mm |
|
Primary radius of curvature |
~700 mm |
|
Final surface figure |
Better than λ/20 |
|
λ/20 at 632.8 nm |
~31.6 nm |
|
Gravity deformation |
Several tens of nm |
|
Rotational positions |
3 or 6 |
|
Six-pose interval |
60° |
|
Gravity-separated result |
~λ/12 → λ/22 RMS |
|
Compensator design residual |
<λ/100 |
|
Compensator alignment |
<5 arcsec |
|
CGH diffraction efficiency |
>30% |
|
CGH-calibrated compensator WFE |
~λ/85 |
|
Cited CGH accuracy |
~λ/70–λ/100 |
|
Cross-validation result |
<λ/40 |
|
Test temperature stability |
±0.1°C |
|
Edge-data exclusion |
~2–5% |
These values are specific to the reference verification process and should not be interpreted as universal qualification limits.
Review a Ground-to-Orbit Verification Requirement
For high-precision space mirrors, the limiting issue is often not nominal interferometer resolution, but how gravity, support conditions, reference-wavefront error, alignment, environment and residual uncertainty are treated in the acceptance result.
If your optical hardware is approaching nanometre-level surface or wavefront tolerances, submit the relevant aperture, optical requirement, test configuration and available error budget for engineering review.
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