A low wavelength infrared Super Continuum (SC) signal from a master oscillator introduces two or more seeds into an amplifier that supports the Raman effect. A counter-propagating, high-power, continuous wave, or quasi-continuous wave quantum cascade lasers pump (amplifies) a first optical seed creating a cascading amplification of subsequent optical seeds forming two or more tunable wavelength coherent optical pump sources.

A fiber laser device includes a pumping light source, an amplifying fiber, an input side fiber fusion-spliced on an input side of the amplifying fiber and formed with a HR-FBG, an output side fiber fusion-spliced on an output side of the amplifying fiber and formed with an OC-FBG having a reflectivity smaller than that of the HR-FBG, an output end, and a mode filter, wherein the input side fiber or an intermediate fiber disposed between the amplifying fiber and the input side fiber is fusion-spliced with the amplifying fiber via a fusion splice portion, and at least a portion of the mode filter is disposed in a region between the fusion splice portion and a position separated from the fusion splice portion by a coherence length of beating caused by mode interference of signal light propagating in the amplifying fiber.

A fiber-based optical amplifier for operation at an eye-safe input signal wavelength λ.sub.S within the 2 μm region is formed to include a section of Holmium (Ho)-doped optical gain fiber. The pump source for the fiber amplifier is particularly configured to provide pump light at a wavelength where the absorption coefficient of the Ho-doped optical gain fiber exceeds its gain coefficient (referred to as an “absorption-dominant pump wavelength”), and is typically within the range of 1800-1900 nm. The selection of an absorption-dominant pump wavelength limits the spontaneous emission of the pump from affecting the amount of gain achieved at the higher wavelength end of the operating region. The amount of crosstalk between the signal wavelength and pump wavelength is also reduced (in comparison to using the conventional 1940 nm pump wavelength).

The present disclosure relates to optical fiber amplifying systems having operability at a wide variety of ambient temperatures and to methods for using them. One aspect of the disclosure is an optical fiber system configured to provide amplified radiation. The system includes an active optical fiber; a plurality of grating-locked pump sources, each having an output optically coupled to the active optical fiber; one or more temperature sensors, configured to measure a temperature associated with one or more of the grating-locked pump sources; and a control system configured to accept measurements from the one or more temperature sensors and, for a desired total pump power output, to provide to one or more of the grating-locked pump sources a set of drive currents suitable to provide the desired total pump power output.

A broadband optical amplifier for operation in the 2 μm visible wavelength band is based upon a single-clad Ho-doped fiber amplifier (HDFA). A compact pump source uses a combination of discrete laser diode with a fiber laser (which may be a dual-stage fiber laser) to create a pump output beam at a wavelength associated with creating gain in the presence of Ho ions (an exemplary pump wavelength being 1940 nm). The broadband optical amplifier may take the form of a single stage amplifier or a multi-stage amplifier, and may utilize a co-propagating pump and/or a counter-propagating pump arrangement.

A method of providing in-line Raman amplification in an optical fiber sensing system, including the procedures of generating a probe light having a probe wavelength, transmitting the probe light into an optical fiber, generating at least one Raman pump light at a respective pump wavelength, the pump wavelength being shorter than the probe wavelength, generating at least one Raman seed light at a respective seed wavelength, the seed wavelength being between the pump and probe wavelengths, transmitting the Raman pump light into the optical fiber, transmitting the Raman seed light into the optical fiber and propagating the Raman pump light, the Raman seed light and the probe light along the optical fiber to achieve distributed Raman amplification of signal light produced by the probe light as it propagates along the optical fiber.

A power semiconductor waveguide optical amplifier (P-SWA) may include an amplifier waveguide with an invertible core formed from one or more undoped heterogeneous semiconductor layers and one or more cladding layers surrounding one or more sides of the invertible core formed as one or more undoped semiconductor layers. Pump light may be coupled into the amplifier waveguide to induce the population inversion in the invertible core. Signal light may further be coupled into the amplifier waveguide and may be amplified as it propagates through the amplifier waveguide. The signal light may then exit the amplifier waveguide as amplified signal light.

An opposing pump structure for twin 980-nm pump lasers in an EDFA, the structure comprising erbium-doped optical fiber, two 980-nm pump lasers, two signal/pump combiners, and anti-interference structures. Two 980-nm pump lasers output first pump light and second pump light, respectively, and first pump light and second pump light are injected into erbium-doped optical fiber in forward direction and reverse direction, respectively. Optical transmission path of first pump light and optical transmission path of second pump light are separately provided with anti-interference structures. Anti-interference structures are two fiber Bragg gratings or two optical filters. The invention improves optical paths of opposing pump structure for twin 980-nm pump lasers, and adds fiber Bragg gratings or optical filters to serve as anti-interference structures, so as to prevent residual pump light from either direction from entering opposite direction, thereby eliminating mutual interference between two opposing 980-nm pumps, and avoiding damage to tube cores.

A light source for Raman amplification to Raman-amplify signal light includes: plural incoherent light sources that output incoherent light; plural pumping light sources that output second-order pumping light; an optical fiber for Raman amplification to Raman-amplify the incoherent light with the second-order pumping light, and outputs the amplified incoherent light; and an output unit connected to the optical transmission fiber, receiving the amplified incoherent light, and outputting the amplified incoherent light as first-order pumping light having a wavelength that Raman-amplifies the signal light to the optical transmission fiber.

This optical amplification module includes a light source that outputs light of a predetermined wavelength as excitation light, a first optical coupler that splits the excitation light into first excitation light and second excitation light such that an optical power ratio becomes a predetermined ratio, and then couples the first excitation light with a first optical signal and outputs the result, and outputs the second excitation light to a different path from the first optical signal and a first optical amplifier that amplifies and outputs the first optical signal.