Lightwave Electronics Corporation

Sunpower Corporation

Jds Uniphase Corporation

Mobius Photonics, Inc.

Ipg Photonics Corporation

Frank J Adams

David L Klein

Werner H Wiechmann

Mark Alan Arbore

Jeffrey Dellert Kmetec

Manuel J Leonardo

William M Grossman

Melvin Chan

Henry G Plaessman

Output pulses from an optical system having a seed source and an optical amplifier coupled to the seed source may be controlled by controlling a power of a seed signal from the seed source. The seed signal may be varied between a minimum value and a maximum value in a way that the seed signal exhibits one or more pulse bursts. Each pulse burst may contain one or more pulses. During an inter-pulse period between successive pulses within a pulse burst or between successive pulse bursts, the power of the seed signal may be adjusted to an intermediate value that is greater than the minimum value and less than the maximum value. The intermediate value is chosen to control a gain in the optical amplifier such that a pulse or pulse burst that follows the period exhibits a desired behavior.

Tailored pulse burst

Power consumption at a site is monitored. An electrical load is connected to a power source by an electrical conductor. A fuel-less energy producing device is electrically connected to a junction along the electrical conductor. A current sensor is electromagnetically coupled to the electrical conductor at a sensing position between the power source and the junction to create a current sensor signal. Sensed current and voltage signals are produced from the current sensor signal. A sensed phase relationship between the sensed signals is determined and compared to a baseline phase relationship to determine the direction of current flow through the conductor. A power source signal, based on the current flowing through the conductor at the sensing position, is created. With some examples a Rogowski type differential current sensor is used. In some examples a single current sensor is used.

Method for enabling monitoring of power consumption

Methods and apparatus for managing thermal loads on a laser gain medium and for boosting the output power of a diode pumped laser are disclosed. The short-term average pumping power to the gain medium is increased, to provide a burst of pumping energy to the laser gain medium. A subsequent short-term reduction in the average pumping power then allows the gain medium to cool to a desired state steady level. The average pumping power is then increased to maintain this steady state level until the next burst is desired. For example, a pulse of current may be applied to a laser diode at a first current level Ifor a first time interval &#x394;t, where Iexceeds a nominal current value Iby an amount &#x394;I. The current to the laser diode is reduced to a second current level Ifor a second time interval &#x394;t, where Iexceeds Iby an amount &#x394;I. To balance the thermal load on the diode an integral of &#x394;Iover the time &#x394;tis approximately equal in magnitude to an integral of &#x394;Iover the time &#x394;t. After applying the pulse of current at the first current level I, and before or after reducing the current to the second level I, the nominal current is applied to the laser diode for a third time interval &#x394;t.

Laser burst boosting method and apparatus

Methods and apparatus for calibrating a frequency difference between two or more lasers over an extended frequency range as well as optical signal generators that employ such an apparatus or method are disclosed. The lasers are tuned in coordination with respect to one or more readily characterized narrow frequency ranges to characterize one or more tuning parameters of each of the lasers over the extended frequency range. The apparatus may include first and second tuning controllers respectively coupled to the first and second lasers, an optical coupler optically coupled to the first laser and the second laser, a frequency detector coupled to the optical coupler and a controller coupled to the frequency detector and the temperature controllers. The controller may include a processor and a memory containing processor executable instructions for calibrating the two lasers in accordance with the method described above. Such a frequency calibration apparatus may be incorporated with the lasers into a signal generator apparatus.

Calibrating a frequency difference between two or more lasers over an extended frequency range

An intracavity frequency converted, Q-switched laser and method for operating such laser to obtain high output power in secondary pulses at a converted frequency. The secondary pulses are generated by a intracavity frequency conversion element from primary pulses at the fundamental wavelength. In accordance with the invention, after the primary and secondary pulses are generated the Q-switch is turned back on before the gain is fully depleted in the generation of the primary pulse. In particular, the Q-switch is turned back on such that a certain amount of energy of the primary pulse is retained in the laser, but late enough so that a majority of the secondary pulse is out-coupled from the laser. The Q-switched laser is well-suited for use at pulse repetition rates larger than 1/&tgr;, where &tgr; is an upper state lifetime (fluorescence lifetime) of the laser. Specifically, the laser can be operated at repetition rates of 10 kHz and higher, e.g., 30 kHz and higher to obtain significant increases in output power of the secondary pulses. Furthermore, the method and laser of the invention are compatible with various types of frequency conversion elements and processes including second harmonic generation, third harmonic generation, fourth harmonic generation, difference frequency generation, sum frequency generation, parametric amplification and parametric generation.

Method for operating Q-switched lasers with intracavity frequency conversion

Pulse recovery times are reduced in a pulsed intracavity frequency-converted laser by operating the laser in a continuous-wave (c.w.) mode before operation in a Q-switched mode. C.w. light locally optically heats the frequency-conversion optics of the laser to facilitate phase-matching at the beginning of Q-switched operation. C.w. operation also reduces the amplitude of the first pulse of the subsequent firing sequence by expending population inversion accumulating in the gain medium. Operation in c.w. mode is initiated by ramping up the net optical gain in the laser cavity when the time elapsed since the latest emitted pulse exceeds 110% of the interpulse spacing prior to the latest pulse. Initiation of c.w. operation does not require external signals other than optionally a pulse trigger sequence from the user. Cavity optical losses may be increased immediately prior to the first pulse, for accumulating population inversion and increasing the first pulse to a desired level. Frequency doubling and tripling lithium triborate (LBO) crystals were used with a Nd-YAG solid state medium to generate ultraviolet light at 355 nm from infrared light at 1064 nm.

Pulse amplitude control in frequency-converted lasers

Method and apparatus for stabilization of pulse energies produced by a continuously pumped, Q-switched, solid-state or gas laser, through control of the optical power delivered by an optical pump to the laser, in order to limit the energy emitted in any single laser pulse as a result of Q-switching. The laser pump is driven at full strength for a selected initial refresh time t.sub.r. If a Q-switch trigger signal is received by the laser before the elapsed time .DELTA.t has reached the refresh time t.sub.r, the laser emits a pulse with the reduced energy stored in the laser at that time. If the elapsed time reaches or exceeds the refresh time t.sub.r, the optical pump power subsequently delivered to the laser is reduced to a lower level, which may be time-dependent, that is sufficient to maintain the net energy stored in the laser at a predetermined value so that the energy in a subsequently emitted laser pulse does not exceed a selected limit. Numerous techniques for controlling the optical pump power delivered are disclosed.

Growing community of inventors

Los Altos, CA, United States of America

Frank J Adams