Mode-locked fiber lasers
A mode locked fiber laser, with a ring-shaped
resonator composed of optical fibers and an erbium-doped fiber
gain medium, can generate ultra-short pulses. Passive mode locking,
which takes advantage of nonlinear optical effects, makes it possible
to generate femto-second optical pulses but the repetition rate
is limited to about 10 MHz, whereas active mode locking based
on high-speed optical modulators can increase the repetition rate
to about 10 GHz but the pulse width cannot be decreased below
the pico second level. As an example of an actively mode locked
laser, Fig. 1 shows the configuration of a regeneratively and
harmonically mode locked fiber laser, and Fig. 2 shows the output
waveform. Since fiber lasers generate nearly transform-limited
pulses with their pulse width ranging from ps to fs, their expected
light source applications may include optical communication as
well as signal processing, measurement, and spectroscopy.

Fig. 1 Regeneratively and harmonically mode-locked fiber
laser.

Fig. 2 Output waveform
Distribution of frequency standards by fibers
The linewidth of the longitudinal
mode in a laser output spectrum is below 1 kHz. This exceptionally
stable regeneratively mode locked laser is used for frequency
measurement with extremely high precision by employing the equally-spaced
longitudinal modes as a "ruler" (Fig. 3). Furthermore,
a laser driven by a 9.1926 GHz signal generated from a Cs atom
as a clock provides optical signals with a frequency of 9.1926
GHz, namely an "optical atomic clock". This frequency
standard in optical communication band can be distributed directly
to photonic networks. The application of these stable mode-locked
lasers to frequency standards is a goal of our research.

Fig. 3 Providing frequency standards through optical fibers

Fig. 4 Cesium optical atomic clock
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