MIKES fibre-coupled differential dynamic line scale interferometer

An instrument developed for high accuracy calibration of line scales up to 1.16 m is described. The instrument is based on an earlier design from the early 1990s. Since then, in order to improve performance and achieve smaller uncertainty, large portions of software, mechanics and optics have been redesigned and several uncertainty components better characterized. The software has been developed to be less sensitive to imperfections of the line mark. In order to decrease noise and deformation coupling in interferometric measurement, the interferometer operating principle has been designed to use a fibre-coupled laser light, interferometer optics have been improved for better phase adjustment and detection and a differential interferometer principle has been taken into use. In order to minimize the effects due to deformations of the stone table rail with moving heavy carriage, a separate bed has been designed under line scale supports. The bed with fixed differential reflector prevents deformations of the table from affecting the line scale versus interferometer position. The main properties of the instrument are described and an uncertainty estimate is presented. The expanded uncertainty (k = 2) for line distance calibration of high-quality low-thermal-expansion line scale is U = [(4.5 nm)2 + (43 × 10−9 L)2]½, where L is the measured length. The results of international comparisons support the uncertainty estimate.

[1]  K P Birch,et al.  The effect of variations in the refractive index of industrial air upon the uncertainty of precision length measurement. , 1993 .

[2]  Hirokazu Matsumoto,et al.  Automatic Recording Laser Interferometer for Line Standards up to 2 m , 1980 .

[3]  Kyuwon Jeong,et al.  The dynamic compensation of nonlinearity in a homodyne laser interferometer , 2001 .

[4]  J. S. Beers,et al.  Interferometric measurement of length scales at the National Bureau of Standards , 1982 .

[5]  Akira Takahashi,et al.  An experimental verification of the compensation of length change of line scales caused by ambient air pressure , 2010 .

[6]  Jens Fluegge,et al.  Status of the nanometer comparator at PTB , 2001, Lasers in Metrology and Art Conservation.

[7]  B. Edĺen The Refractive Index of Air , 1966 .

[8]  G. B. nsch,et al.  Measurement of the refractive index of air and comparison with modified Edl?n's formulae , 1998 .

[9]  Harald Bosse,et al.  SUPPLEMENTARY COMPARISON: Final report on CCL-S3 supplementary line scale comparison Nano3 , 2003 .

[10]  F. Zernike,et al.  Accurate laser wavelength measurement with a precision two-beam scanning Michelson interferometer. , 1981, Applied optics.

[11]  Yuichi Takigawa,et al.  Error contributor of defocus and quadratic caustic in line scale measurement , 2011 .

[12]  I. Tiemann,et al.  An international length comparison at an industrial level using a photoelectric incremental encoder as transfer standard , 2003 .

[13]  Harald Bosse,et al.  An international length comparison using vacuum comparators and a photoelectric incremental encoder as transfer standard , 2008 .

[14]  Felix Meli,et al.  Calibration of a 2D reference mirror system of a photomask measuring instrument , 2001, Lasers in Metrology and Art Conservation.

[15]  Masaji Sawabe,et al.  A new vacuum interferometric comparator for calibrating the fine linear encoders and scales , 2004 .

[16]  Antti Lassila,et al.  Design and performance of an advanced metrology building for MIKES , 2011 .

[17]  Harald Bosse,et al.  A revised treatment of the influence of the sample support on the measurement of line scales and the consequences for its use to disseminate the unit of length , 2009 .

[18]  Paul G Shekelle,et al.  Results and Conclusion , 2009 .

[19]  A Lassila,et al.  Interferometer for calibration of graduated line scales with a moving CCD camera as a line detector. , 1994, Applied optics.

[20]  Bojan Ačko Final report on EUROMET Key Comparison EUROMET.L-K7: Calibration of line scales , 2012 .