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Journal of the Optical Society of America

Journal of the Optical Society of America

  • Vol. 43, Iss. 10 — Oct. 1, 1953
  • pp: 853–859

Optics InfoBase > JOSA > Volume 43 > Issue 10 > Precision Measurement of Wavelengths with Echelle Spectrographs

Precision Measurement of Wavelengths with Echelle Spectrographs


JOSA, Vol. 43, Issue 10, pp. 853-859 (1953)

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<p>Echelles of the type now produced by the Bausch & Lomb Optical Company lie intermediate in dispersive properties between ordinary diffraction gratings and such interferometers as the Fabry-Perot etalon. When crossed with a concave grating in a stigmatic mount of the type recently described (Harrison, Archer, and Camus, J. Opt. Soc. Am. <b>42</b>, 706 [1952]) an echelle might be expected to give wavelength precision between the approximately one part in 10<sup>6</sup> of which the grating is capable and the one part in 25×10<sup>6</sup> of the etalon. We find precision to about 1 part in 5×10<sup>6</sup> attainable with the echelle.</p><p>Identification of the order of interference <i>m</i> of any cycle on an echellegram can be made quickly and exactly by use of a standard plate or scale, which can be marked uniquely after photography of two or three known lines. A horizontal fiducial line of constant <i>m</i>λ<sub>0</sub> is recorded on the spectrogram by reflecting light from a mirror which can be swung into position in front of the echelle. The exact <i>m</i>λ<sub>0</sub> value for the plate is determined from the two or three standard lines photographed on it. Wavelength reduction is most conveniently made in terms of <i>m</i>λ, using the <i>m</i>λ<sub>0</sub> line as a reference. The vertical <i>m</i>λ dispersion is first assumed constant over the entire plate, and an approximate <i>m</i>λ value is determined for each line in terms of its distance <i>l</i> from <i>m</i>λ<sup>0</sup>. A small correction ≪ is then added for each line, values of ≪ for the entire fixed focal surface having been determined in advance with some complex spectrum having many known lines, such as thorium. Values of ≪ are found to not exceed 0.050 <i>m</i> order-angstroms with our instrument. This range includes empirical corrections for error of coincidence, nonuniformity of dispersion along a cycle, variable magnification of the spectrograph, and all other deviations from vertical linearity or horizontal constancy of <i>m</i>λ.</p><p>On division by three-figure integral values of <i>m</i>, wavelengths can be obtained to within about 0.001A throughout the visible and ultraviolet spectrum, with little added complexity beyond that required for reducing grating spectrograms, and with greater precision, compactness, and spectrum coverage on a single plate.</p><p>A discussion of the so-called “error of concidence” is included, as this phenomenon, which has been principally of historical importance since the early days of spectroscopy, now affects the accuracy attainable with a single fiducial line and two or three Hg 198 lines, when substituted for the large number of standard lines needed for precision wavelength determinations with concave gratings.</p>

GEORGE R. HARRISON, SUMNER P. DAVIS, and HUGH J. ROBERTSON, "Precision Measurement of Wavelengths with Echelle Spectrographs," J. Opt. Soc. Am. 43, 853-859 (1953)

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