The optical frequency is extremely high, as high as hundreds of tera-hertz (1 tera-hertz (=THz) =1012 Hz), and cannot be converted directly to electrical signals. For the conversion, optical beat measurements are used. When two optical beams of frequency (f1) and (f2) are mixed, optical beat occurs at a frequency (f1 - f2) and is observed if (f1 - f2) is adequately low. The optical frequency is measured in combination with the optical beat measurements.
An ultra-short pulse train generated from a mode-locked laser contains fine spectral lines spaced by a frequency interval determined by repetition frequency (frep) as illustrated in Fig. 1. As the spectral lines seem like a comb, the spectrum is named "optical frequency comb". The optical frequency comb has lines spaced at precisely uniform interval, and if the intervals are stabilized to the frequency based on the cesium atomic clock, the optical frequency comb can be used as a optical frequency ruler. Particularly, in case of optical comb of greater span than an octave (double frequency), it may be possible to set frequencies of comb lines to multiples of (frep), by selecting conditions appropriately. In this condition, all the frequencies of the optical frequency comb are the integral multiples of the repetition frequency (frep). Where n is a large integer. Finally, a laser frequency to be measured (flaser) can be determined as flaser = n·frep + fbeat, by measuring an optical beat (fbeat).
In order to convert stable signals of atomic clock into optical signals (n·frep) in the optical comb, the following steps are traced: (1) microwave frequency synthesis of frep from a microwave frequency generated from an atomic clock (Process A), (2) control of optical comb (Process B), and (3) n-time multiplication by optical comb (Process C). The MIJ-AIST has studied the bottleneck steps, Process A and Process B, and improved these. Consequently, improved system could measure the most stable laser in NMIJ/AIST by using the most stable atomic clock as the reference. That is, this "optical frequency ruler" is confirmed not to degrade the signal.
In addition, signal-to-noise (S/N) ratio of the optical beat is of great significance. The optical system has been optimized so that the S/N ratio is stabilized for a long time by increasing adjusting points, and by selecting optical components of reduced loss. Besides, the accuracy for measuring signals of lower S/N ratio has been improved by checking the frequency behavior.
The absolute frequency of a laser can be determined from 500 nm to 1064 nm as far as an optical frequency comb exits. Therefore, laser of any wavelength, and of any type, semiconductor, solid-state and others can be used technically as a standard laser for length.
The provision of the calibration service will upgrade the reliability of lasers for length standard, and make it possible to use various kinds of laser as reference for precise length measurement, such as green gas laser, which has not been calibrated so far, and semiconductor lasers of various colors. Consequently, it is expected that compact and lower-price laser-interferometers will appear.