Multi-wavelength laser source
AssigneeLucent Technologies Inc.
InventorsJohn J. Veselka, Steven K. Korotky
Life of this patent
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AssigneeLucent Technologies Inc.
InventorsJohn J. Veselka, Steven K. Korotky
Estimating the term…
A light source for generating many precisely spaced wavelength channels, based on the periodic modulation of light. CW light is periodically amplitude modulated and then coupled to a non-linear fiber where it undergoes additional modulation by the process of self-phase modulation or other non-linear effects. In a general embodiment of the multi-wavelength source (MWS), an optical modulator driven by a periodic electromagnetic signal imposes periodic amplitude modulation on light from a single longitudinal mode CW laser. The light is then coupled to a non-linear medium with an intensity dependent refractive index where it generates higher order spectral sidebands by the process of self-phase modulation and/or other non-linear effects. The frequency spacing between the spectral components is equal to the repetition rate of the modulation. The shape of the spectrum (i.e. the relative amplitudes of the spectral components) can be modified by adjustments to: the amplitude modulated waveform; the optical power of the waveform when coupled to the non-linear medium; and/or characteristics of the non-linear medium such as the non-linear refractive index, the length and the dispersion.
A multi-wavelength light source for producing laser light having a plurality of wavelengths, comprising:
A multi-wavelength light source for producing laser light having a plurality of wavelengths, comprising:
A multi-wavelength light source for producing laser light having a plurality of wavelengths, comprising:
A multi-wavelength light source for producing laser light having a plurality of wavelengths, comprising:
A multi-wavelength light source for producing laser light having a plurality of wavelengths, comprising:
A multi-wavelength light source for producing laser light having a plurality of wavelengths, comprising:
A method of producing a plurality of light signals of spaced-apart wavelength, the wavelength being related to the frequency of a periodic signal, comprising the steps of:
A method of producing a plurality of light signals of spaced-apart wavelength, the wavelength being related to the frequency of a periodic signal, comprising the steps of:
A wavelength division multiplex transmitter comprising:
Dependencies are inferred from the claim text.
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Laser transmitters: using external modulation
Based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect: operation of the cell; Circuit arrangements
Frequency conversion, i.e. wherein a light beam is generated with frequency components different from those of the incident light beams: four-wave…
Structural aspects: multiwavelength transmitters
Term ended 13 Feb 2017 (estimated)
USPTO file history isn’t available for this patent, so only indexed dates are shown.
The invention pertains to the field of laser light sources. More particularly, the invention pertains to sources of multiple wavelengths of coherent light for Wavelength Division Multiplexed (WDM) optical communications systems.
Wavelength-Division-Multiplexing (WDM) is an attractive option for providing increased capacity in light wave transmission systems and routing capability within optical networks. For example, high capacity transport systems that carry as many as eight wavelengths per fiber have been developed and are currently being deployed. Presently in these systems, each transmitter includes a laser that is intended to operate at only one of the allowed wavelength channel frequencies. The lasers are engineered to operate within the channel specifications for the life of the system by both tight control of the laser fabrication and its operating environment. To plan for the event of a failure, an inventory of transmitters for each wavelength channel must also be maintained. As undoubtedly the demand for the number of wavelengths in transport and local systems will increase to 32 or more in the not too distant future, new technological capabilities and designs for transmitters and receivers will be required to minimize the complexity and cost of the use of such large numbers of wavelengths.
Several approaches to address the channel stabilization and inventory issues are being considered. One solution to the inventory problem is to use a tunable laser that can be adjusted to the desired channel within each transmitter. However, tunable lasers are more complicated than fixed frequency lasers, will naturally drift over a wider range, and will require stabilization of the operating wavelength for each of a large number of channels. A very attractive solution to the inventory and stabilization dilemma is to use a wavelength selectable laser. In this case, each photonic source chip includes several fixed frequency lasers, which the desired channel may be selected from. Wavelength selectable source chips that can reach 4-6 channels have been reported (see M. G. Young, U. Koren, B. I. Miller, M. Chien, T. L. Koch, D. M. Tennant, K. Fedder, K. Dreyer, and G. Raybon, "Six wavelength laser array with integrated amplifier and modulator," Electron. Lett., vol. 31, no.21, pp. 1835-1836, Oct. 12, 1995), however reaching larger numbers would presumably present significant yield and packaging issues.
FIG. 1 shows a block diagram of the invention in its most general form.
FIG. 2 shows a more specific block diagram of the invention.
FIG. 3a shows the spectrum of the light at the input to the DSF as measured by a Fabry-Perot spectrometer.
A general embodiment of the multi-wavelength source (MWS) is shown in FIG. 1 and operates as follows.
An optical modulator (3) driven by a periodic signal (4) imposes periodic amplitude modulation on light (2) from a single longitudinal mode CW laser (1). The light is then coupled to a non-linear medium (5) with an intensity dependent refractive index where it generates higher order spectral sidebands by the process of self-phase modulation. The frequency spacing between the spectral components is equal to the repetition rate of the modulation. The shape of the spectrum (i.e. the relative amplitudes of the spectral components) can be modified by adjustments to: the amplitude modulated waveform; the optical power of the waveform. when coupled to the non-linear medium; and/or characteristics of the non-linear medium such as the non-linear refractive index, the length and the dispersion.
The basic configuration of a practical MWS is shown in FIG. 2. A similar configuration has been used by others to generate optical soliton pulses for use in a soliton transmission system (E. A. Swanson and S. R. Chinn, "40-GHz Pulse Train Generation Using Soliton Compression of a Mach-Zehnder Modulator Output," IEEE Photon. Technol. Lett., vol. 7, no. 1, pp. 114-116, January 1995). The present invention comprises the use of this arrangement as a multi-wavelength source, an effective and novel system for generating a plurality of spaced-apart wavelength coherent light signals from a single laser source. Two alternative methods to attain the periodic amplitude modulated optical signal are described.