Abstract:
Aspects of the disclosure relate generally to a circuit for sustaining an radio frequency (RF) modulated optical signal. The circuit may comprise a self injection locking component having a fiber optic delay line over which a portion of the optical signal propagates. The circuit may also comprise a self phase locked loop component having at least two fiber optic cables having different lengths and over which another portion of the optical signal propagates and a phase detector coupled to the at least two fiber optic cables and configured to determine a phase difference between the signals propagating over one of the respective fiber optic cables. The circuit may further comprise a voltage controlled oscillator configured to generate a stable oscillating signal in response to signals generated by each of the self injection locking and self phase locked loop components, the stable oscillating signal being configured to sustain the optical signal.
Abstract:
An adjustable array includes a plurality of optical devices. Each adjustable array device has an optical light output therefrom and is configured whereby the corresponding optical lights of the plurality of optical devices have a predefined nonequivalent relationship relative to one another with respect to an output parameter. In response to a drive signal, the plurality of optical devices are further configured to adjust the corresponding optical lights with respect to the output parameter while substantially maintaining the predefined nonequivalent relationship.
Abstract:
The invention relates to a mirror arrangement for guiding a laser beam in a laser system having at least one first end mirror (1) and one second end mirror (2), wherein said end mirrors (1, 2) define a resonator having an optical resonator axis (OA), wherein the laser beam is guided into the resonator as an input laser beam (ES) and is guided out of the resonator again after multiple reflection at the first and second end mirrors (1, 2) as an output laser beam (AS). The sequence of reflections at the first and the second end mirror (1, 2) thereby determines a direction of rotation between the first and second end mirror, defined as an axis of rotation relative to the resonator axis, whereby a first beam path is defined and the laser beam circulates in a direction of rotation between the first and second end mirrors in the resonator defined as an axis of rotation relative to the resonator axis (OA). The resonator is designed such that the direction of rotation is reversed at a reversing point and the laser beam in the resonator passes through at least partially in a direction of rotation opposite to the first beam path, whereby a second beam path is defined.
Abstract:
An optical pulse source 30 comprising a DPSS pump laser 31, a photonic crystal fibre (PCF) 35 and acousto-optic modulator (AOM) gating means 33. The pump pulses are coupled through lenses 32 to the AOM 33, synchronised to the pump laser 31 and operable to gate the pump pulses to a reduced repetition rate Rr = Rf/N, where Rf is the pump laser fundamental frequency. The pulses from the AOM 33 are injected via optics 34 into the PCF 35. Propagation through the PCF 35 causes the pulses to broaden spectrally to produce supercontinuum pulses. An optical pulse source comprising the optical pulse source 30 and an acousto-optical tunable filter (AOTF) operable to convert supercontinuum pulses into wavelength variable output pulses is also provided. A method of scaling the energy of the optical supercontinuum pulses is also provided.
Abstract:
Presented is a laser resonator cavity comprising at least one gain medium (16A,16B) and end reflectors (12A,12B,14) which define together longitudinal modes of light in the cavity, the resonator cavity further comprising: (1) a beam coupler assembly (320) configured to split tight impinging thereon into a predetermined number of spatially separated light channels (C1, C2), and to cause phase locking and coherent combining of the light channels, having common longitudinal and transverse modes, in a double pass through the beam coupler assembly, to thereby produce an output combined light channel, the beam coupler assembly being configured for polarization coupling of the light channels and comprising two polarizers (322A,322B) accommodated in a spaced-apart relationship along an axis of the cavity; and an optical element (323) configured as a half wave retardation plate or 45° polarization rotator accommodated between the two polarizers; and an aperture arrangement (318A,318B) configured to select in at least one of the light channels a predetermined transverse mode content that is desired at the cavity output (14).
Abstract:
A grating (16) based line narrowing unit with bi-directional beam expansion for the narrowing lasers. In a preferred embodiment a beam from the chamber of the laser is expanded in the horizontal direction with a three-prism beam expander (8, 10, 12) and is expanded in the vertical direction with a single prism (60). A narrow band of wavelengths in the expanded beam is reflected from a grating in a Littrow configuration back via the two beam expanders into the laser chamber for amplification.
Abstract:
A smart laser having automatic computer control (24A) of pulse energy, wavelength, and bandwidth using feedback signals from a wavemeter (22). Pulse energy is controlled by controlling discharge voltage. Wavelength is controlled by very fine and rapid positioning of an Rmax mirror in a line narrowing module. Bandwidth is controller by adjusting the curvature of a grating in the line narrowing module. Preferred embodiments include automatic adjustment of a prism plate on which beam expander prisms are located and automatic adjustment of the Rmax tilt. Other preferred embodiments include automatic adjustment of the horizontal position of the laser chamber (3) within the resonance cavity. In preferred embodiments, feedback signals from a wavelength monitor are used to position the Rmax mirror. In other embodiments a separate laser beam reflected off the Rmax mirror on to a photodiode array is used to position the mirror.
Abstract:
A smart laser having automatic computer control (24A) of pulse energy, wavelength, and bandwidth using feedback signals from a wavemeter (22). Pulse energy is controlled by controlling discharge voltage. Wavelength is controlled by very fine and rapid positioning of an Rmax mirror in a line narrowing module. Bandwidth is controller by adjusting the curvature of a grating in the line narrowing module. Preferred embodiments include automatic adjustment of a prism plate on which beam expander prisms are located and automatic adjustment of the Rmax tilt. Other preferred embodiments include automatic adjustment of the horizontal position of the laser chamber (3) within the resonance cavity. In preferred embodiments, feedback signals from a wavelength monitor are used to position the Rmax mirror. In other embodiments a separate laser beam reflected off the Rmax mirror on to a photodiode array is used to position the mirror.
Abstract:
The invention relates to a method for operating a laser light source, more particularly, for scanning in a confocal laser scan microscope, whereby the laser light source (3) is supplied with power by means of a power unit. In order to enhance service life of the laser light source (3) and reduce operating costs, the laser light source (3) is operated with the required power almost exclusively during effective beam utilization time, preferably during data capture. By using a pulsating laser light source, effective beam utilization time, especially data capture, is synchronized (14) substantially with the emission cycle of the laser light source.