Polarization scrambler and optical network using the same
View Patent ↗To generate light with the degree of polarization zeroed and the spread of an optical spectrum suppressed even with temporal overlapping between optical pulses each of which is polarized orthogonally to the succeeding pulse, a polarization scrambler includes an optical pulse generator that generates optical pulses with an intensity waveform repetition period T/2 and an electrical field repetition period T in which the same intensity waveform is repeated every repetition period T/2 and in which phase is inverted every repetition period T/2, and an orthogonal polarization delay unit which receives each of the optical pulses, separates the optical pulse into two optical pulses with orthogonal states of polarization, and relatively shifts the temporal position of one of the two optical pulses from that of the other optical pulse by (2n−1)T/4 (n is a natural number) to generate light in which each pulse is polarized orthogonally to a succeeding pulse.
1. A polarization scrambler comprising:
an optical pulse generator that generates optical pulses with an intensity waveform repetition period T/2 and an electrical field repetition period T in which the same intensity waveform is repeated every repetition period T/2 and in which phase is inverted every repetition period T/2; and
an orthogonal polarization delay unit which receives each of said optical pulses, separates the optical pulse into two optical pulses with orthogonal states of polarization, and relatively shifts the temporal position of one of the two optical pulses from that of the other optical pulse by (2n−1)T/4 (n is a natural number) to generate light in which each pulse is polarized orthogonally to a succeeding pulse.
2. A polarization scrambler according to claim 1 , wherein said optical pulse generator comprises a light source that generates a continuous wave and an optical intensity modulator which has an input signal φ(t) (t denotes time) and such a transmission characteristic that for a particular input signal φ 0 , output electrical fields are expressed by:
E (φ( t )−φ 0 )=− E (−φ( t )−φ 0 )
the optical intensity modulator being driven by the input signal φ(t) having such a repetition period T that:
φ( t )−φ 0 =φ( t−T )−φ 0 =−φ( t−T/ 2)−φ 0 (≠0),
the optical pulse generator modulates uses said input signal φ(t) of the repetition period T to modulate said continuous wave to generate optical pulses with an intensity waveform repetition period T/2 and an electrical field repetition period T which provide electrical fields expressed by:
E ( t )= E (φ( t )).
3. A polarization scrambler according to claim 2 , wherein said optical intensity modulator has a periodic transmission characteristic for the input signal.
4. A polarization scrambler according to claim 3 , wherein said optical intensity modulator is a Mach Zehnder type optical intensity modulator and subjects paths into which optical power is split, to phase modulation using sinusoidal signals with opposite phases which have a time average difference φ 0 and cause a phase difference π on a peak-to-peak basis.
5. A polarization scrambler according to claim 4 , wherein when a data signal bit rate is defined as B, a signal input to said optical intensity modulator has a repetition period T=2/mB (m is a natural number), and a phase of a data signal bit rate clock is synchronized to a phase of the input signal to said optical intensity modulator.
6. A polarization scrambler according to claim 2 , wherein when a data signal bit rate is defined as B, a signal input to said optical intensity modulator has a repetition period T=2/mB (m is a natural number), and a phase of a data signal bit rate clock is synchronized to a phase of the input signal to said optical intensity modulator.
7. A polarization scrambler according to claim 3 , wherein when a data signal bit rate is defined as B, a signal input to said optical intensity modulator has a repetition period T=2/mB (m is a natural number), and a phase of a data signal bit rate clock is synchronized to a phase of the input signal to said optical intensity modulator.