Abstract:
An external cavity semiconductor laser system (100) is disclosed wherein multiple segments of semiconductor material are excited with an array of pump sources (20). In one embodiment, a laser beam is reflected in a pattern to pass through multiple excited segments on a wafer of semiconductor material (12). On another embodiment, a series of wafers disposed in a laser cavity are excited. This pumping system spreads out the thermal load while providing a high power, high quality, laser beam.
Abstract:
A control circuit for a laser system having a first and a second power supply (10, 26) connected in parallel. A mode selector (50) is available to the laser operator to change the operational mode of the laser system from continuous to pulse mode or vice versa, and any combination of the modes. In the pulse mode, a series of short-time voltage pulses is superimposed on a low power level laser mode using the circuit control characteristic of the thyratron tube (36) to sharply increase the laser output for the duration of the individual pulses.
Abstract:
A laser assembly includes a lasing medium (12), associated reflector components (14, 16) defining a resonance cavity, and means (16) for outputting laser pulses therefrom. Means (18) is provided to pump the lasing medium with pulses of predetermined energy. There is a pumping circuit (20) for activating the pump means, and control means (22, 34, 35) associated with said pumping circuit for determining the energy of the pumping pulses.
Abstract:
Described is a laser system comprising a laser (10), which can be switched between at least two power levels, and a power supply (1 + 2) for the laser which is connected up to the mains supply which applies the input voltage. The invention is characterized by the fact that the laser power supply has a distributing unit (1) the input terminal of which is connected to the mains voltage and which is connected to a laser power supply unit (2) and to a charging unit (4) for an accumulator unit (5) in such a way that, while the laser is being operated at low power, the charging unit is also powered, in addition to the laser power supply unit, from the mains, and that, while laser is being operated at high power, the output terminal of the accumulator unit is connected to the laser power supply unit.
Abstract:
A method and apparatus for generating an inverted population in a gas are provided. Gas is excited at one pressure, so as to give a portion of the gas the energy of a higher electronic state. The gas is then expanded to a lower pressure, so as to concentrate that portion of the gas into a reduced number of energy levels in the higher electronic state. This concentrated population should then produce an inverted population relative to a lower electronic state. Inverted populations can then be used for stimulating emission, in a variety of laser devices, or in an amplifier. A lower curve (1) represents the ground state of energy and a middle curve (3) represents the first excited electronic state energy; an upper curve (5) represents the upper electronic energy states. To generate a population inversion unexcited atoms in the flat portion (13) are excited into flat portion (15) or the upper flat portions (17).
Abstract:
The invention is applied to N2, CO2, eximer and other lasers and can be used in any installation based on volumetric self-sustained discharge. The invention facilitates the formation of volumetric self-sustained discharge where there is significant non-homogeneity in the density of gas mixtures and a high pulse repetition rate of volumetric self-sustained discharge. The system comprises at least two electrodes (1, 2) made from separate plates (5, 6). Each plate of the first (1) and second (2) electrodes is electrically connected to two other plates (5, 6), through spark (9) gaps, to the plate (5, 6) proximate to its own electrode, and through its separate section (3) of the container tank, to the plate (5, 6) of the other electrode (1, 2) lying on the same plane. In any of the electrically connected plate pairs, one of the plates (5) is linked, through a stabilising inductance (7, 10), with the common collection bar (8, 11) of its own electrode (1, 2), while the other (6) is not connected to the common collection bar (8, 11). Between all the plates (5, 6) there are dielectric elements forming a gas flow with a velocity route perpendicular to the working edge of the plates (5, 6).
Abstract:
In a free electron laser system with energy recovery, the system having an electron gun (110) to supply a beam of electrons; a wriggler array (114) to supply a spatially alternating magnetic field to the electron beam whereby a microwave beam (118) is generated; separating means (115) to spatially separate the microwave beam and the electron beam emerging from the wriggler array; electron collection means to receive the separated electron beam; and a high voltage, low current supply (122) and a low voltage, high current supply (124) connected in series to supply the gun (110); the high voltage supply also being connected between the electron collection means (120) and the gun (110); any instabilities are sensed by sensing the current through the high voltage supply (122); comparing the sensed current with a preset value; and disconnecting the EHT supply (122) from the gun (110) when the preset value is exceeded.
Abstract:
In an AVLIS process, Zr is selectively removed from natural zirconium by a three-step photoionization wherein Zr atoms are irradiated by a laser beam having a wavelength lambda 1, selectively raising Zr atoms to an odd-parity E1 energy level in the range of 16000-19000 cm , are irradiated by a laser beam having a wavelength lambda 2 to raise the atoms from an E1 level to an even-parity E2 energy level in the range of 35000-37000 cm , and are irradiated by a laser beam having a wavelength lambda 3 to cause a resonant transition of atoms from an E2 level to an autoionizing level above 53506 cm . lambda 3 wavelengths of 5607, 6511 or 5756 ANGSTROM will excite a zirconium atom from an E2 energy state of 36344 cm to an autoionizing level; a lambda 3 wavelength of 5666 ANGSTROM will cause an autoionizing transition from an E2 level of 36068 cm ; and a lambda 3 wavelength of 5662 ANGSTROM will cause an ionizing resonance of an atom at an E2 level of 35904 cm .
Abstract:
A waveguide filter (22, 24) is incorporated into a cavity resonator (20) for a free-electron laser or the like by coating a material layer (24) on the inner peripheral surface of a hollow waveguide member (22). A high pass filter configuration is provided when the conductivity of the material layer (24) is higher than that of the waveguide member (22), such that electromagnetic signals having wavelengths longer than the skin depth of the material layer (24) pass into and are affected by the lower conductivity waveguide member (22). Reversing the conductivities produces a low pass filter configuration in which signals having wavelengths shorter than the skin depth are affected by the material layer (24). A bandpass filter configuration is provided by adding an additional material layer (32) of low conductivity to a high pass filter, whereas a band exclusion filter configuration is produced by adding an additional material layer (32) of high conductivity to a low pass filter.
Abstract:
Free electron laser apparatus, for producing coherent electromagnetic radiation within a spectral range extending from millimeter to visible wavelenghts, includes elements for generating an electron beam (14) and for directing the beam to move over the surface of a diffraction grating (16) thereby producing electromagnetic radiation. Optical or quasi-optical elements confine the electromagnetic radiation, including bound surface mode radiation, to generate feedback, resulting in stimulated, coherent emission. Methods are disclosed for increasing the electron beam current above a certain value so as to provide sufficient feedback of the electromagnetic radiation for producing stimulated, coherent emission.