Abstract:
In accordance with the invention an optical fiber communication system comprising a source of optical signals and an optical fiber transmission line is provided with one or more multiple-order distributed Raman effect amplifiers downstream of the source for amplifying the transmitted signals. As compared with a communication system using conventional first order Raman amplifiers, multiple-order amplifier systems can have reduced noise, longer fiber span lengths and reduced nonlinearities. In a preferred embodiment the system uses signal wavelengths in the range 1530-1570 nm, first order Raman pumping at 1430-1475 nm and second order pumping at about 1345 nm. Advantageously, the second order pump light is copropagating with the signal light and the first order pump is counterpropagating with the signal.
Abstract:
The performance of optical fiber Raman devices can be increased by substitution of a broadband reflector (typically a multilayer dielectric mirror) for some of the narrowband reflectors (typically fiber Bragg gratings) that are conventionally used to define the optical cavities of the device. The device exemplarily is a Raman laser or amplifier, and in preferred embodiments a broadband reflector reflects all the Stokesshifted wavelengths, such that the cavities are defined by the single broadband reflector and by a multiplicity of appropriately selected narrowband reflectors. Optionally the broadband reflector also serves to reflect the pump radiation.
Abstract:
In an optically amplified multi-wavelength optical fiber communication system (e.g., 80), deleterious effects due to channel addition/removal can be reduced or avoided if the optical amplifiers (80) are "overpumped", that is to say, the system is selected such that at least 70%, preferably 90% or more, of the pump power that is introduced into the amplifier fiber is unabsorbed in the amplifier fiber.
Abstract:
An optical communication system comprising a light source, a cladding pumped fiber laser (10) having a pump cladding (14), an optical fiber (20) attached to the cladding pumped fiber laser, the optical fiber having a cladding (24) and a protective coating (26). and an expedient that prevents substantial damage to the protective coating of the optical fiber upon transmission of at least 1 watt of residual light out of the pump cladding. Such an expedient may be the material of the protective coating, which may comprise a metal, such as gold, aluminium or copper, or a high refractive-index polymer such as a polyimide, polyetheretherketone, polytetrafluoroethene or an epoxide. Alternatively, or in addition, the expedient may comprise an article disposed at the attachment of the laser to the fiber and capable of conducting and dissipating heat produced by the residual light, for example, a metal block having a groove that supports the laser, the fiber or both.
Abstract:
The optical waveguide system (100) comprises a mode discriminating coupler (10) and reflective mode coupling means (e.g., 34 and 35). These components can be combined in a variety of ways to perform a variety of functions. Among them are drop multiplex devices (30), add multiplex devices (60), add/drop multiplex devices (70), and power combiners. The device combinations can have low loss as well as high reliability, the latter due to the robust structure of the devices.
Abstract:
An optical fiber communication system (40) according to the invention comprises an optical fiber filter that can be manufactured at low cost and that can be conveniently incorporated into the system, substantially like a conventional fiber jumper. The filter comprises a length L of axially uniform optical fiber selected to have substantially no loss (e.g., 1 , and to have relatively high loss (e.g.,> 20dB) at a wavelength λ 2 . The length L will typically be less than 100 m. In one embodiment the optical fiber is a single mode optical fiber at λ 1 (e.g., 1.3µm) that does not have a guided mode at λ 2 (e.g., 1.55µm). In another embodiment the fiber contains a dopant that does substantially not absorb radiation of wavelength λ 1 , but substantially absorbs at λ 2 . In the second embodiment, λ 1 can be greater than λ 2 . Fiber filters according to the invention can be advantageously used in a variety of communication systems, and exemplary systems are disclosed.
Abstract:
A low noise optical fiber Raman amplifier with integral Raman laser (FRA) is disclosed. The FRA typically comprises a fiber ring with at least two amplifier stages (21, 22), with strictly counter-propagating pump radiation. Relatively short wavelength (e.g., 1060 nm) pump power is provided to the Raman laser portion of the fiber ring. Appropriately selected and placed Bragg gratings (e.g., 204) provide one or more optical cavities in the fiber ring, such that the input pump radiation is converted to the desired amplifier pump radiation (e.g., 1240 nm, suitable for amplification of 1310 nm signal radiation). The FRA can, for instance, advantageously serve as power amplifier in digital or analog fiber communication systems, or it can serve as pre-amplifier or in-line amplifier.