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🔬 ASME B89.1.8-2011 (Reaffirmed 2016) is the American National Standard for the performance evaluation of displacement-measuring laser interferometers, prepared by Project Team B89.1.8 under the ASME B89 Dimensional Metrology Committee and approved by ANSI on July 15, 2011. Laser interferometry has become the preferred way to evaluate the linear-displacement accuracy of machine tools and coordinate measuring machines (CMMs) and serves as the core incremental radius-measuring device in systems such as laser trackers. The Standard helps users evaluate the accuracy of laser interferometer systems: it includes a folded common-path comparison test that lets users functionally compare systems even when the lasers use different wavelengths or measurement techniques, provides a measurement uncertainty table for judging an individual measurement or comparing competing systems, and includes best-practice appendices.
The body comprises scope, definitions, general considerations for system performance evaluation, test procedure (laser interferometer comparison test), verification of test performance and bias estimation with result uncertainty, measurement evaluation, and references. The definitions section highlights the Abbe offset (schematically shown in Figure 2-1): when the laser measurement axis is laterally offset from the displacement direction, any angular drift is magnified into a displacement error. The test procedure chapter gives recommended target positions (Table 4.2-1), sensitivity coefficients associated with the length difference error LDE (Table 4.7.2-1), and the air-refractive-index wavelength-correction method (Tables 4.8-1 to 4.8-3 for low/medium/high humidity air, with combinations in Table 4.8-4).
Section 3 states the general principles: evaluation should separate the instrument’s intrinsic errors (predictable by the manufacturer) from errors introduced by the use environment, and it emphasizes the effect of the structural loop — the mechanical connection among the laser head, optics, and retroreflector forms the measurement loop, and any thermal or mechanical drift enters the measurement. It also warns that when different interferometers use different wavelengths or techniques (AC vs. DC interferometers, see Appendix E), comparing raw readings directly may mask systematic differences, so the folded common-path test is recommended for functional comparison.
The comparison test is the core procedure: two or more laser interferometer systems are arranged on a shared folded path, the target mirror is moved to the recommended positions of Table 4.2-1, and each system’s reading at every position is recorded. The test should cover the typical range and sampling density of the system under test, and the contributions of components such as the length difference error (LDE) are assessed using the sensitivity coefficients of Table 4.7.2-1. During measurement, temperature, pressure, and humidity are recorded synchronously and the wavelength is corrected per Tables 4.8-1 to 4.8-4. Results are reported in the forms of 4.10-1 to 4.10-3 (intercomparison results, sensor calibration results, and overall result).
| Environmental Variable | Typical Sensitivity (Ref., 10⁻⁶ order) | Correction Note |
|---|---|---|
| Air temperature | ≈ −0.9 to −1.0 ppm/°C | Higher temperature lowers refractive index, lengthens wavelength; correct the displacement reading |
| Atmospheric pressure | ≈ +0.35 ppm/mmHg | Higher pressure raises refractive index, shortens wavelength |
| Relative humidity | Low (25 %RH) to high (75 %RH) differ ≈ 0.2–0.3 ppm | Water vapor lowers refractive index; Tables 4.8-1–4.8-3 give values |
| CO₂ content | ≈ 0.15 ppm / 100 ppm CO₂ | Secondary correction for high-accuracy measurement |
Section 5 requires verifying the test itself: estimate the test bias through repeated measurements and confirm the test system is in control, then evaluate the result per the uncertainty table. Section 6 (Measurement Evaluation) gives two sample budgets: Table 6-1 for errors predictable by the manufacturer, and Table 6-2 combining the manufacturer’s reported uncertainty with additional sources (environment, Abbe offset, alignment error, etc.) for a metrology laboratory. Appendix A gives a complete uncertainty budget for interferometric length measurement; Appendix B describes methods for comparing two interferometer systems; and Appendix C collects best procedures and practices for accurate linear measurement with a laser interferometer.