The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.

The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.

Date of Patent:
Jul. 22, 2003

Filed:

Feb. 22, 2001
Applicant:
Inventors:

Matthias Kramer, Goettingen, DE;

Marcus Serwazi, Gleichen, DE;

Assignee:

Lambda Physik AG, Goettingen, DE;

Attorney:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
G01B 9/02 ;
U.S. Cl.
CPC ...
G01B 9/02 ;
Abstract

A first method for determining the relative wavelength shift of a laser beam away from a known reference line, such as an absorption line of a gas in an opto-galvanic cell or a reference line of reference laser uses a monitor etalon. The FSR of the etalon used to calculate the wavelength shift is determined based on a calculated gap spacing between the etalon plates, or etalon constant. The gap spacing is determined based on a fit to measured values of wavelength deviations of the FSR as a function of the relative wavelength shift. The FSR used to calculate the wavelength shift is also based on the wavelength shift itself. A second method for measuring the absolute bandwidth and spectral purity of a tunable laser beam uses an opto-galvanic or absorption cell. The laser beam is directed to interact with a gas in the cell that undergoes an optical transition within the spectral tuning range of the laser. The beam is tuned through the optical transition line of the gas in the cell, and the opto-galvanic or absorption spectrum of the line is measured. The measured bandwidth and spectral purity are convoluted or broadened by the bandwidth of the laser beam used in the measurement. The bandwidth and spectral purity of the laser beam are determined based on the bandwidth and spectral purity, respectively, of the measured spectrum and a known correspondence between the measured convoluted bandwidth and spectral purity and the bandwidth and spectral purity, respectively, of the laser beam.


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