Abstract:
A wavemeter and method for measuring bandwidth for a high repetition rate gas discharge laser having an output laser bean comprising a pulsed output of greater than or equal to 15 mJ per pulse, sub-nanometer bandwidth tuning range pulses having a femptometer bandwidth precision and tens of femptometers bandwidth accuracy range, for measuring bandwidth on a pulse to pulse basis at pulse repetition rates of 4000Hz and above, is disclosed which may comprise a focusing lens having a focal length; an optical interferometer creating an interference fringe pattern; an optical detection means positioned at the focal length from the focusing lens; and a bandwidth calculator calculating bandwidth from the position of interference fringes in the interference fringe pattern incident on the optical detection means, defining a DID and a DOD, the respective distances between a pair of first fringe borders and between a pair of second fringe borders in the interference pattern on an axis of the interference pattern, and according to the formula Δλ= λ0 [DOD2 _ DID2] / [8f2-D02] where λ0 is an assumed constant wavelength and D0 = (DOD - DID)2, and f is the focal length.
Abstract:
A method and apparatus for measuring bandwidth of light emitted from a laser (12) is disclosed which may comprise: a first (30) and second (34) wavelength sensitive optical bandwidth etalon detectors providing, respectively, an output (32, 36) representative of a first parameter indicative of the bandwidth of the emitted light as measured respectively by the first anal second bandwidth detectors, and an actual bandwidth calculation apparatus (40) adapted to utilize these two outputs as part of a multivariable linear equation employing predetermined calibration variables specific to either the first or the second bandwidth detector, to calculate a first actual bandwidth parameter (FWXM) or a second actual bandwidth parameter (EX).
Abstract:
There is described a system and method for the in vivo determination of lactate levels in blood using Near-Infrared Spectroscopy (NIRS)and/or Near-infrared Raman Spectroscopy (NIR-RAMAN). The method teaches measuring lactate in vivo comprising: optically coupling a body part (14) with a light source (10) and a light detector (18) the body part having tissues comprising blood vessels; injecting near-infrared (NIR) light at one or a plurality of wavelengths in the body part; detecting, as a function of blood volume variations in the body part, light exiting the body part at at least the plurality of wavelengths to generate an optical signal (20); and processing the optical signal as a function of the blood volume variations to obtain a lactate level in blood.
Abstract:
A simple, reliable, easy to use method for calculating bandwidth data of very narrow band laser beams based on bandwidth data obtained with a spectrometer in circumstances where the laser bandwidths are not large compared to the slit function of the spectrometer. The slit function of the spectrometer is determined (20). Spectral data of the laser beam is measured with the spectrometer to produce a measured laser beam spectrum which represents a convolution of the laser beam spectrum and the spectrometer slit function (76). This measured laser spectrum is then mathematically convolved with the slit function of the spectrometer to produce a doubly convolved spectrum. Bandwidth values representing true laser bandwidths are determined from measured laser spectrum and the doubly convolved spectrum. Preferably the true laser bandwidths are calculated by determining the difference between 'twice a measured laser bandwidth' and a corresponding 'doubly convolved bandwidth.' This method provides an excellent estimate of the true laser bandwidth because 'twice the measured laser bandwidth' represents two laser bandwidths and two spectrometer slit function bandwidths and the 'doubly convolved bandwidth' represents one laser bandwidth and two spectrometer slit function bandwidths. Thus, the difference is a representation of the true laser bandwidth. In a preferred embodiment the bandwidth parameters measured are the full width half-maximum bandwidth and the 95% integral bandwidth.
Abstract:
A computer implemented method for matching paint on a vehicle, having the steps of receiving in a central computer, from a remote terminal, vehicle identifying information relating to a specific vehicle and a first set of paint color data from a portion of the body of the vehicle. The central computer includes a database with vehicle identifying information for a plurality of vehicles, associated with paint color data and their paint formulations. A first process determines a first best match paint formulation which relates submitted vehicle identifying information and submitted paint data to a paint formulation. The latter is transmitted to the remote terminal. The central computer receives a second set of paint color data from the remote terminal representing a surface of the specific vehicle painted with the first best paint formulation and compares by a second process the second paint color data to the first paint color data so as to establish accuracy data. The accuracy data is applied to the first process so as to be implemented in subsequent paint formulation identifications.
Abstract:
The present invention provides an excimer laser capable of producing a high quality pulsed laser beam at pulse rates of about 4,000 Hz at pulse energies of about 5mJ or greater. A preferred embodiments is an ArF excimer laser specifically designed as a light source for integrated circuit lithography. An improved wavemeter with special software monitors output beam parameters and controls a very fast PZT driven tuning mirror and the pulse power charging voltage to maintain wavelength and pulse energy within desired limits. In a preferred embodiment two fan motors drive a single tangential fan which provides sufficient gas flow to clear discharge debris from the discharge region during the approximately 0.25 milliseconds between pulses.
Abstract:
The method and apparatus of the present invention provides a system wherein light-emitting diodes (LEDs) (162) can be tuned within a given range by selecting their operating drive current in order to obtain a precise wavelength. The present invention further provides a manner in which to calibrate and utilize an LED probe (150), such that the shift in wavelength for a known change in drive current is a known quantity. In general, the principle of wavelength shift for current drive changes for LEDs is utilized in order to allow better calibration and added flexibility in the use of LED sensors, particularly in applications when the precise wavelength is needed in order to obtain accurate measurements. The present invention also provides a system in which it is not necessary to know precise wavelengths of LEDs where precise wavelengths were needed in the past. Finally, the present invention provides a method and apparatus for determining the operating wavelength of a light-emitting element such a light-emitting diode.
Abstract:
In order to decrease errors in spectral measurement, the data measured at sampling wavelength intervals smaller than the wavelength sampling intervals are changed to data of wavelength sampling interval of spectral effective curve. If the wavelength half-bandwidths to be measured are different from the wavelength sampling intervals, the spectral data at wavelengths in correspondence with the wavelength sampling intervals are obtained with interpolation. In a spectroradiometer, wavelength scale is calibrated with use of a plurality of line spectra of specified wavelengths, and the photoelectric outputs are integrated with use of the addresses of elements as a weight factor.
Abstract:
A photometric light absorption measuring apparatus includes a central processing unit sending generator frequency data to a high power generator that pulses a light source intermittently to irradiate a liquid sample contained in a transparent receptacle. The intermittent light beams pass through optical guides, focusing lenses, light amplifiers and a slit aperture. A diffraction grating disperses the light beams and a light detector receives the spectral components and generates corresponding intensity signals which are passed through an amplifier and supplied to an arithmetical unit which receives frequency power generation signals from the central processing unit. A misfire detector sends signals to the arithmetical unit when the light source fails to flash. The arithmetical unit preselects two spectral components and calculates the concentration of a corresponding preselected constituent of the liquid sample from the average mean value of the intensity differences between the two preselected spectral components corrected to eliminate intensity data corresponding to non-flashes of the light source.