摘要:
An apparatus for creating an optical noise of a predetermined bandwidth uses an optical amplifier (2,20,50) which amplifies optical noise components and produces unpolarized optical noise by spontaneous emission, a mirror (32,52,98) to reflect the optical noise components back to the optical amplifier (2,20,50) and a filter (4,32,34,56,80) that filters out optical noise components outside the predetermined optical bandwidth. The filter (4,32,-34,56,80) is located so that optical noise components passed by the filter are amplified in the optical amplifier (2,20,50) during an additional amplification. Optionally, a pollarizer and Faraday rotator (30,54,96) are used in the apparatus. The optical noise created in the optical amplifier is polarized in the polarizer (34,36,58,60,84,100) after 2 amplifications, rotated in the Faraday rotator (30,54,96) then is amplified two more times before leaving the apparatus.
摘要:
An optical circulator having first, second, and third ports. The optical circulator includes a beam splitter and a plurality of Faraday stages. The beam splitter is connected to the first and third ports and separates a first light signal entering the first port into first and second outgoing light signals. The beam splitter also separates a second light signal entering the third port into third and fourth outgoing light signals. The first, second, third, and fourth outgoing light signals are spaced-apart from one another. The first and second outgoing light signals include, respectively, orthogonal polarization components from the first light signal, and the third and fourth outgoing light signals include, respectively, orthogonal polarization components from the second light signal. The Faraday stages, including a first Faraday stage and a last Faraday stage, being arranged in series. The first Faraday stage receives light from the beam splitter, and the last Faraday stage is positioned so as to provide light to the second port. The second port and the walk-off directions and directions of rotation of the Faraday stages are chosen such that light entering the first port exits the second port, light entering the second port exits the third port, and light entering the third port is prevented from exiting the first and second ports.
摘要:
In a laser that generates blue light, two reflectors (34 & 40; 52 & 56; 61 & 62), one or both of which may be fiber-Bragg gratings, define a laser cavity which contains an optical fiber (39; 51; 60) doped with praseodymium. An energy source (32; 55; 64 & 65) provides input light to the optical fiber. A portion of the optical fiber (39) may be doped with ytterbium. Another reflector (37) defines a second, shorter laser cavity within the first laser cavity. The energy source (32) provides energy with a wavelength of about 850 nanometers which provides cross relaxation pumping, resulting in the generation of blue light. There may be two separate cavities, one for the praseodymium-doped fiber (51) and one for an ytterbium-doped fiber (50). An energy source (55) of about 835 nanometers is used. The ytterbium-doped fiber may not be used, in which case two energy sources, one (64) at 1017 nanometers and one (65) at 835 nanometers, are provided.
摘要:
Apparatus (300) and method for measuring the change in a dimension of a structure operate by measuring the distance between the plurality of reflective markers (11-15) located along an optical fiber (22). The optical fiber (22) is attached to the structure in such a manner that a change in the dimension in question results in a change in the optical delay of the fiber (22) between at least two of the markers (11-15). The fiber (22) is illuminated with low coherence light. Each marker (11-15) reflects a portion of a light signal traversing the fiber from a first end thereof. The markers (11-15) are located at predetermined distance from the first end. Light reflected from the markers (11-15) is collected and introduced into an autocorrelator (30,310) that measures the coherent sum of a first signal comprising the collected light and a second signal comprising the collected light delayed by a variable time delay. The coherent sum is measured as a function of said variable time delay. Various embodiments of the present invention utilize different methods for identifying the specific markers (11-15). For example, the markers (11-15) may be constructed such that each pair of markers (11-15) reflects light of a characteristic wavelength. In a second embodiment, the distance between each pair of markers (11-15) is used to identify the pair of markers (11-15). In a third embodiment. the reflectivity of each marker (11-15) is used to identify the markers (11-15).
摘要:
A channel selection method and apparatus accommodate the dynamic reconfiguration of channels that are passed through parallel waveguides by selectively tuning Bragg gratings along the waveguides. In the preferred embodiment, the waveguides are output optical fibers connected to an optical splitter (94) having an input of a wavelength division multiplexed (WDM) optical signal. The number of channels in the WDM signal is equal to the number of output fibers (74, 76, 78, 80, 82), which is in turn equal to the number of tunable Bragg gratings (84, 86, 88, 90, 92) along each of the output fibers. The series of Bragg gratings on a particular output fiber is structurally identical to the other series, with each tunable Bragg grating being dedicated to passing or rejecting one of the channels of the WDM signal. Thus, the series of Bragg gratings along a particular output fiber may be tuned to isolate any of the channels or may be tuned to pass two or more channels. In addition to use in a demultiplexing application, the method and apparatus may be used in a multiplexing application to enable channel selection along each of a number of different input waveguides.
摘要:
A cross-coupler[20, 100, 200] for connecting a first optical network running on a first optical channel[10] to a second optical network running on a second optical channel[12]. The optical couplers are inserted into the first and second optical channels at an insertion point in each of the optical channels. Broadly, the coupler includes a first interface[21] inserted into the first optical channel[10], a second interface[22] inserted into the second optical channel[12], and an optical connecting channel connecting the first and second interfaces for transferring light of a selected wavelength from the first optical channel[10] to the second optical channel[12]. The first and second interfaces preferably include variable frequency Bragg reflectors (VFBR) for reflecting light of a selected wavelength traveling in the optical channels. The selected wavelength is alterable by applying a selection signal to the first VFBR[24, 104]. In embodiments in which light signals are transferred both from the first optical channel[10] to the second optical channel[12] and vice versa, a second optical connecting channel[118] is utilized for transferring light between the second optical channel[12] and the first optical channel[10]. The device preferably utilizes optical circulators for interfacing the various light signals to, and from, the connecting channels. Embodiments in which fixed frequency Bragg reflectors are used in place of the VFBRs may also be constructed.
摘要:
An optical system such as an add and/or drop WDM multiplexer allows the wavelength fluctuation of an optical carrier to be tracked so that a corresponding fiber Bragg grating (FBG) can be responsively tuned. The preferred embodiment of the wavelength tracking system in an optical system such as an add and/or drop module includes a three-port optical circulator (22), three optical fibers (12, 26, 28), a series of tunable FBGs (30, 32, 34, 36, 38 and 40), a source of a broadband optical noise signal (48), an optical spectrum analyzer (OSA) (50), and an FBG tuner (44). In operation, an LED generates modulated probe lightwaves that are inserted into a drop module (20). The LED lightwaves and the optical carriers propagating through the drop module are monitored by an OSA. The monitoring procedure determines the conditions, in terms of target wavelengths of the FBGs, and the stability or instability of the optical carriers. The FBGs are then tuned in response to the FBG and optical carrier information. In another embodiment, the wavelength of an optical carrier is tracked using a modulated tracking grating (94) and an FBG (102) is adjusted in response to the tracking information.
摘要:
A channel selection method and apparatus accommodate the dynamic reconfiguration of channels that are passed through parallel waveguides by selectively tuning Bragg gratings along the waveguides. In the preferred embodiment, the waveguides are output optical fibers connected to an optical splitter (94) having an input of a wavelength division multiplexed (WDM) optical signal. The number of channels in the WDM signal is equal to the number of output fibers (74, 76, 78, 80, 82), which is in turn equal to the number of tunable Bragg gratings (84, 86, 88, 90, 92) along each of the output fibers. The series of Bragg gratings on a particular output fiber is structurally identical to the other series, with each tunable Bragg grating being dedicated to passing or rejecting one of the channels of the WDM signal. Thus, the series of Bragg gratings along a particular output fiber may be tuned to isolate any of the channels or may be tuned to pass two or more channels. In addition to use in a demultiplexing application, the method and apparatus may be used in a multiplexing application to enable channel selection along each of a number of different input waveguides.
摘要:
Apparatus (300) and method for measuring the change in a dimension of a structure operate by measuring the distance between the plurality of reflective markers (11-15) located along an optical fiber (22). The optical fiber (22) is attached to the structure in such a manner that a change in the dimension in question results in a change in the optical delay of the fiber (22) between at least two of the markers (11-15). The fiber (22) is illuminated with low coherence light. Each marker (11-15) reflects a portion of a light signal traversing the fiber from a first end thereof. The markers (11-15) are located at predetermined distance from the first end. Light reflected from the markers (11-15) is collected and introduced into an autocorrelator (30,310) that measures the coherent sum of a first signal comprising the collected light and a second signal comprising the collected light delayed by a variable time delay. The coherent sum is measured as a function of said variable time delay. Various embodiments of the present invention utilize different methods for identifying the specific markers (11-15). For example, the markers (11-15) may be constructed such that each pair of markers (11-15) reflects light of a characteristic wavelength. In a second embodiment, the distance between each pair of markers (11-15) is used to identify the pair of markers (11-15). In a third embodiment. the reflectivity of each marker (11-15) is used to identify the markers (11-15).