OPTICAL PULSE SOURCE GENERATING RETURN-TO-ZERO PULSE AT WAVELENGTH lambda

    公开(公告)号:JP2002344389A

    公开(公告)日:2002-11-29

    申请号:JP2002070749

    申请日:2002-03-14

    Abstract: PROBLEM TO BE SOLVED: To provide an RZ pulse source which has high power and is jitter-free, compact (inexpensive) and power efficient. SOLUTION: The modulated RZ pulse source has a modulated light source optically and a optical trap coupled to a stabilized Bragg grating filter. The light source is modulated in power and frequency, and has an adjusted channel wavelength λ. The Bragg grating filter has a reflective bandwidth having a high slope reflective cutoff, and is preferably tunable. By a feedback arrangement responsive to the taps, the source channel wavelength λ is kept on the edge of the reflective bandwidth and RZ pulses are shaped. When the Bragg grating is stabilized, the feedback system maintains λ at a value linked to the grating reflective edge, and converts the light source modulated by overlapping at least one part of the optical spectrum of the source, into RZ pulses with high extinction ratio.

    OPTICAL DIFFRACTION GRATING DEVICE HAVING ADJUSTABLE CHIRP

    公开(公告)号:JP2000137197A

    公开(公告)日:2000-05-16

    申请号:JP30793299

    申请日:1999-10-29

    Abstract: PROBLEM TO BE SOLVED: To obtain an optical diffraction grating device having an adjustable chirp. SOLUTION: The optical waveguide diffraction grating having an adjustable chirp includes a waveguide diffraction grating thermally brought into contact with an electrically controllable heat converting substrate whose temperature is changed along the length of the diffraction grating (A). The heat converting substrate can generate heat on a fiber, or remove heat from the fiber, and temperature slope can be generated along the diffraction grating. In an execution example, the heat converting substrate is constituted as a resistance film whose local resistance is changed along the length of the diffraction grating (B). Currents running through the thin film can generate the temperature slope along the diffraction grating almost proportional to the local resistance of the thin film, and the size of the chirp can be adjusted by the currents. Thus, this obtained device can be made simple, compact, and efficiently power.

    DEVICE INCLUDING OPTICAL PULSE RE-SHAPING MEANS

    公开(公告)号:JP2000298296A

    公开(公告)日:2000-10-24

    申请号:JP2000071393

    申请日:2000-03-15

    Abstract: PROBLEM TO BE SOLVED: To provide an all-optical means applicable to re-shaping of pulse by selecting an optically nonlinear material and periodic variations, so that a re-shaped optical output pulse becomes an optical output pulse substantially limited in conversion. SOLUTION: A WDM (a system having one or more operating wavelengths) signal from a transmitter 11 is propagated downstream to an amplifier 15, and demultiplexed by a conventional demultiplexer 17. Next, the demultiplexed channels are supplied to each BSPR(Bragg soliton pulse re-shapers) 161-169. Each BSPR is adjusted to a proper wavelength. Next, the reshaped pulses are multiplexed by a conventional multiplexer 18 and propagated downstream to a using means. The BSPR to be used consists of a Bragg diffraction grating formed in a waveguide showing nonlinearity with respect to the electric field of the pulse propagated via the BSPR. Furthermore, the BSPR is selected so that the nonlinearity of the waveguide substantially averages the dispersion, a fixed distorted pulse is substantially limited in conversion.

    OPTICAL WAVEGUIDE GRATING DEVICE HAVING ADJUSTABLE OPTICAL SPACING PROFILE

    公开(公告)号:JP2002277650A

    公开(公告)日:2002-09-25

    申请号:JP2001081811

    申请日:2001-03-22

    Abstract: PROBLEM TO BE SOLVED: To provide an optical waveguide grating device having an adjustable optical spacing profile. SOLUTION: The optical waveguide grating having the adjustable optical spacing profile is provided with a waveguide grating coming into thermal contact with one or more resistive film coatings. The coating is extended along the length direction of the grating and its local resistance is changed in accordance with the length of the grating. Since a plurality of overlapping coatings are chosen in a certain example, the variation values of respective resistance values are made different and various heat generation profiles are influenced by the control of each individual coating. Different heat generating profiles successively and proportionally change the geometric spacing and local refractive index of the grating along the length direction of the grating, so that a required adjustable optical spacing profile can be provided. In another example, a resistance film is used on the basis of heating variation to be suddenly or periodically changed.

Patent Agency Ranking