Abstract:
A pumping source is provided for the Raman amplification of an optical wavelength division multiplex signal, wherein the pumping source has a number of pumping lasers with, in each case, different pumping wavelengths. Modules for the angle and/or amplitude modulation of pumping signals of the pumping lasers are connected to the pumping lasers, such that by appropriate adaptation of the modulation of the pumping signals mixing products from four-wave mixing between the pumping signals are suppressed.
Abstract:
A pump source for a fiber Raman amplifier used in a WDM optical communication system is formed to generate an RF-modulated pump signal (as opposed to the prior art CW signals). The modulation frequency and index of the RF-modulated pump signal are controlled to impart a sufficient degree of nullrandomnessnull to the presence of the pump signal at each wavelength, thus minimizing cross talk between the signals and improving the transfer of power from the pump signal to the plurality of optical input signals.
Abstract:
This invention relates to a new diode pumped solid state laser which has a miniature Q-switching device in the cavity. Nd:YAG, Nd:YLF or Nd:YVO4 are useful solid state laser materials for Q-switching. A compact thermo-electric (TE)cooled diode laser unit is used as a pump source, and high-speed switching of the drive current driver is provided for the precise pump energy control. By using the variable high-speed switching pump source, the energy of each Q-switched output pulse from the laser can be controlled precisely and the usual “giant pulse” from the Q-switch can be eliminated. Also, the pulse energy can be controlled precisely independent of the repetition rate or switching speed of the Q-switch without using other feedback components. The Q-switch is synchronized to open at the end of each diode pump pulse.
Abstract:
The present invention relates to a laser light-source apparatus and a method of producing a laser beam, and particularly to a laser light-source apparatus capable of generating intermittent pulse light having a predetermined flickering time and emphasizing the brightness of its peak by a Bartley effect. A timing circuit forms a timing signal so as to allow an excitation type laser light source to produce the intermittent pulse light having the predetermined flickering time. A pumping laser pumps the excitation type laser light source based on the signal outputted from the timing circuit. The intermittent pulse light is flickering slower than a flicker value of a normal person in cycle. The time required to put out the intermittent pulse light is set to a time or so required to restore the sensitivity of each of human eyes to the maximum sensitivity after the human eyes have felt brightness since light has been launched into the human eyes.
Abstract:
An apparatus for pumping an optical gain medium, such as a fiber gain medium, comprises a pump source having a plurality of different spatially separate or multiple wavelengths or wavelength bands which are all coupled into the fiber gain medium and provide at least one or more wavelengths to fall within the absorption band of fiber gain medium producing gain despite wavelength shifts in the pump source multiple wavelengths due to changes in the operating temperature of the pump source. At least one or more of the pump wavelengths will overlap the gain spectrum of the fiber gain medium sufficiently to continually provide high input power for pumping of the fiber gain medium.
Abstract:
A switched cavity laser system which includes a resonant cavity, a gain medium within the resonant cavity, a cavity switch and an output coupler. A controllable pump energy source delivers pump energy to the gain medium in response to an energy control signal. A detector is coupled with the gain medium and generates a detector signal in response to the amount of population inversion exhibited by the gain medium. A control circuit is coupled to the detector and controllable pump energy source for generating the energy control signal in response to the detector signal. As the switching rate of the Q-switch is varied, the energy control signal varies to ensure a constant level of population inversion between each pulse. In this matter, a prespecified pulse energy is achieved for each pulse independent of the switching rate of the Q-switch.
Abstract:
A light detection and ranging (LiDAR) system in which multiple pump lasers are operated in polyphase fashion at a single pumping stage is disclosed. In some embodiments, the multiple pump lasers are operated by controllers that generate current pulses through the multiple pump lasers. The current pulses powering at least two of the pumping lasers have different phases. In some embodiments, the phase differences are such that there is no timing overlap in the current pulses through the pump lasers. In some embodiments, the phase difference between successive current pulses is greater than the pulse width such that the sum of the duty cycles of all the current pulses is less than one. In some embodiments, junction temperatures of pump lasers are monitored and temperature information from the monitoring is used to dynamically select which pump laser will be utilized at a given time. Further details of these and other embodiments are disclosed herein.
Abstract:
A pump light generation unit of an optical amplifier pumping device outputs pump light with a single wavelength or a plurality of wavelengths from a plurality of output ports. A pump light multiplexing unit polarization-multiplexes or wavelength-multiplexes the plurality of pieces of pump light which has been output from the pump light generation unit. A polarization scrambler collectively polarization-scrambles the polarization-multiplexed or wavelength-multiplexed pump light which has been output from the pump light multiplexing unit and outputs the polarization-scrambled pump light to an optical waveguide for pump light. The optical waveguide for pump light inputs the pump light which has been polarization-multiplexed or wavelength-multiplexed by the pump light multiplexing unit to the pump light superimposition unit. A pump light superimposition unit multiplexes the polarization-multiplexed or wavelength-multiplexed pump light and signal light. A pump light output port superimposes the pump light on the signal light by outputting the pump light from the pump light superimposition unit to the gain medium so that the pump light propagates in the same direction as the signal light.
Abstract:
Systems, devices, and methods of the present invention provide for the effective generation of high-speed modulated light using difference frequency generation (DFG). Modulated light in the mid-IR region may be generated in an optical resonator with a DFG device and having a Q factor greater than about 50 for a signal light with a wavelength in the range between 1350 and 1550 nm. A DFG device may generate the modulated mid-IR light by collinear passage of the intracavity signal light and a modulated pump light having a wavelength in the range between 1000 and 1100 nm through the DFG device. The modulated pump could be used for pumping both a signal lasing media and a DFG device at the same time.
Abstract:
Example ultra narrow linewidth Brillouin lasers are disclosed that are pumped by pump lasers that are controlled via optimal control schemes in order to stabilize the Brillouin laser output frequency and minimize the Brillouin output linewidth. The control schemes are based on feedback loops to match the pump laser frequency to the optimum Stokes shift on the one hand and to line-narrow the pump laser linewidth on the other hand via comparing the linewidth of the pump laser with the linewidth of the Brillouin laser. The feedback loops in the control schemes can be partially or fully replaced with feedforward control schemes, allowing for larger bandwidth control. Provision for simultaneous oscillation of the Brillouin lasers on two polarization modes allows for further line-narrowing of the Brillouin output. The ultra-narrow linewidth Brillouin lasers can be advantageously implemented as pumps for microresonator based frequency combs, and can also be integrated to the chip scale and be constructed with minimal vibration sensitivity. The ultra-narrow linewidth Brillouin lasers can be widely tuned and a frequency readout can be provided via the use of a frequency comb. When phase locking a frequency comb to the Brillouin laser, ultra-stable microwave generation can be facilitated.