Convolution method for measuring laser bandwidth
AssigneeCymer, Inc.
InventorsSteven F. Haas, Richard L. Sandstrom, Thomas Hofmann, Alexander I. Ershov
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AssigneeCymer, Inc.
InventorsSteven F. Haas, Richard L. Sandstrom, Thomas Hofmann, Alexander I. Ershov
Estimating the term…
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. 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. 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.
A method for using a spectrometer defining a slit function to make bandwidth measurements of a light source having bandwidths which are not large compared to corresponding bandwidths of the spectrometer slit function, said method comprising the steps of:
Dependencies are inferred from the claim text.
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Generating the spectrum; Monochromators: using multiple reflection, e.g. Fabry-Perot interferometer, variable interference filters
Spectrometry; Spectrophotometry; Monochromators; Measuring colours: details
Details: control of working procedures of a spectrometer; Failure detection; Bandwidth calculation
Spectrometry; Spectrophotometry; Monochromators; Measuring colours: generating the spectrum; Monochromators
Term ended 20 May 2020 (estimated)
Spectrometers are well known devices for measuring the spectra of laser beams (i.e., the intensity of light in the beam as a function of wavelength). Ultraviolet laser light sources used for modem integrated circuit lithography are required to have very narrow bandwidth and operate within tight bandwidth specifications. Spectrometers used to measure the spectra of these lasers can be divided into two main categories: diffraction grating based spectrometers and Fabri-Perot etalon based spectrometers.
A description of a typical KrF excimer laser used for lithography is provided in U.S. Pat. No. 5,991,324 which is incorporated herein by reference. There are two spectral bandwidth characteristics of these lasers which are referred to extensively in microlithography applications. These are the spectral bandwidth of the laser measured at 50 percent of the peak intensity, called its full width at half maximum bandwidth (abbreviated FWHM), and the spectral bandwidth, which contains 95% of laser energy called the 95% integral bandwidth (abbreviated 95% I). It is very important that the laser is always operating within specifications during microlithography chip manufacturing because spectral broadening causes blurring of the integrated circuit features being printed on silicon wafers which would result in yield problems. Therefore, it is very important to provide continuous accurate monitoring capabilities for the laser spectrum.
A measure of the quality of a spectrometer is its slit function. This is the spectrum which is recorded by the spectrometer when measuring a very very narrow spectrum. For a spectrometer to accurately measure the spectrum of a laser beam, the slit function bandwidth of the spectrometer itself should be substantially smaller than the laser bandwidth.
FIG. 1 is a flow chart showing the principal steps for practicing a preferred embodiment of the present invention.
FIG. 2A is a drawing showing the principal components of a prior art spectrometer.
FIG. 2B is a graph of the slit function of a prior art diffraction grating spectrometer.
A preferred embodiment of the present invention may be described by reference to the drawings.
Equipment
This first preferred embodiment is preferably used to measure the bandwidths of a lithography gas discharge laser such as a line narrowed KrF laser, a line narrowed ArF laser or an F2 laser. A preferred spectrometer is a grating spectrometer known as the ELIAS spectrometer (an acronym for Emission Line Analyzing Spectrometer) which is supplied by Lasertechnik Berlin—GmbH with offices in Berlin, Germany. Preferably a personal computer running with Windows NT and a special algorithm described herein is used to calculate bandwidth parameters.