The line narrowed laser apparatus configured to perform a plurality of burst oscillations including a first burst oscillation and a second burst oscillation next to the first burst oscillation to output a pulse laser beam. The line narrowed laser apparatus comprises a laser resonator, a chamber provided in the laser resonator, a pair of electrodes provided in the chamber, an electric power source configured to apply a pulsed voltage to the pair of electrodes, a wavelength-selecting element provided in the laser resonator, a spectral width varying unit provided in the laser resonator, a wavelength variable unit configured to change a selected wavelength selected by the wavelength-selecting element, and a controller. The controller is configured to control the wavelength variable unit based on an amount of control of the spectral width varying unit in a period from a time of ending the first burst oscillation to a time of starting the second burst oscillation.

A method of identifying the material and determining the physical thickness of each layer in a multilayer structure is disclosed. The method includes measuring the optical thickness of each of the layers of the multilayer object as a function of wavelength of a light source and calculating a normalized group index of refraction dispersion curve for each layer in the multilayer structure. The measured normalized group index of refraction dispersion curves for each of the layers is then compared to a reference data base of known materials and the material of each layer is identified. The physical thickness of each layer is then determined from the group index of refraction dispersion curve for the material in each layer and the measured optical thickness data. A method for determining the group index of refraction dispersion curve of a known material is also disclosed.

An example laser system includes a laser source to transmit a source light generated based on optical feedback provided by a laser cavity. The laser system further includes a beam-splitter to split the source light into a reference light and a split source light. The laser system further includes a modulator to modulate the split source light's frequency. The modulated light may be transmitted towards and reflected from a target. The modulator and beam-splitter may receive, frequency-modulate, and pass the reflected light to the laser cavity. The laser cavity amplifies the reflected light and transmits the amplified light toward the beam-splitter, such that the amplified light follows a same path as the reference light. The laser system further includes a detector to receive the reference light and amplified light, and detect a beating frequency as an indication of presence of the reflected light. Related methods and devices are also disclosed.

The excimer laser device receives data on a target value of pulse energy from an external device and outputs a pulse laser beam. The excimer laser device includes a master oscillator, at least one power amplifier including a chamber provided in an optical path of the pulse laser beam outputted from the master oscillator, a pair of electrodes provided in the chamber, and an electric power source configured to apply voltage to the pair of electrodes, and a controller configured to control the electric power source of one power amplifier of the at least one power amplifier to stop applying the voltage to the pair of electrodes based on the target value of the pulse energy.

Methods and systems wherein laser induced refractive index changes by focused femtosecond laser pulses in optical polymeric materials or optical tissues is performed to address various types of vision correction.

A ring laser gyroscope comprises a laser block that includes a resonant internal cavity defined by a plurality of surfaces of an optical closed loop pathway, and a plurality of electrodes coupled to the laser block. The electrodes are configured to generate a pair of counter-propagating laser beams from a lasing gas in the optical closed loop pathway. The ring laser gyroscope also includes a field reducer shield comprising an electrically conductive material, with the field reducer shield located completely within the laser block. The field reducer shield is configured to modify an electric field generated by the plurality of electrodes to substantially prevent ions in the laser block from migrating toward the plurality of surfaces of the optical closed loop pathway.

Methods and systems wherein laser induced refractive index changes by focused femtosecond laser pulses in optical polymeric materials or optical tissues is performed to address various types of vision correction.

The excimer laser device receives data on a target value of pulse energy from an external device and outputs a pulse laser beam. The excimer laser device includes a master oscillator, at least one power amplifier including a chamber provided in an optical path of the pulse laser beam outputted from the master oscillator, a pair of electrodes provided in the chamber, and an electric power source configured to apply voltage to the pair of electrodes, and a controller configured to control the electric power source of one power amplifier of the at least one power amplifier to stop applying the voltage to the pair of electrodes based on the target value of the pulse energy.

In an inertial containment fusion (ICF) system which uses a KrF laser, it is beneficial to perform pulse compression of the laser output to produce a higher-power, higher-intensity laser pulse at the target. Such pulse compression involves counter-propagating laser pump and seed beams. A short-pulse seed beam is amplified as energy is extracted from a long-pulse pump beam. Because such energy extraction is invariably incomplete, a fraction of the pump energy will exit the compression cell in the same direction as the optics used to create the seed beam. The invention involves a gas consisting of a noble gas such as neon or argon which may be excited by an electron beam to enhance absorption. By proper choice of gas, cell length, electron-beam excitation, and time delay, the residual pump beam may be absorbed almost entirely with less than 0.01% transmitted laser energy through the invention.

An intracavity plasma solid state laser with an emission line radiation source of determined wavelength seeding a semiconductor laser gain medium providing a high power laser beam of the determined wavelength. A plasma cell generates a determined wavelength based on an atomic emission line that is received by the semiconductor laser or laser diode having a broadband output encompassing the determined wavelength received from the plasma cell. The laser diode locks on to the determined wavelength and emits a high powered laser beam of the determined wavelength. The intracavity plasma solid state laser creates a laser beam of narrow linewidth comparable to the natural Voight or Doppler linewidth of atomic transition and higher power in a smaller size than previously possible. The intracavity plasma solid state laser is easily manufactured and suitable for placement in an array for targeting a predetermined area.