Abstract: An intracavity laser absorption infrared spectroscopy system for detecting trace analytes in vapor samples. The system uses a spectrometer in communications with control electronics, wherein the control electronics contain an analyte database that contains absorption profiles for each analyte the system is used to detect. The system can not only detect the presence of specific analytes, but identify them as well. The spectrometer uses a hollow cavity waveguide that creates a continuous loop inside of the device, thus creating a large path length and eliminating the need to mechanically adjust the path length to achieve a high Q-factor. In a preferred embodiment, the laser source may serve as the detector, thus eliminating the need for a separate detector.

Abstract: In a gas phase analyte testing method a laser beam is generated using a laser beam from a laser gain medium located within an external laser cavity. A gain parameter of the laser gain medium is changed so that the laser gain medium emits across a range of wavelengths in response to the change. The beam is passed through a test sample as the gain parameter is changed, the test sample being positioned inside the external laser cavity. A change in the spatial or spectral mode distribution or dynamics of the laser emission spectrum is detected. It is then determined whether the change in the spatial or spectral mode distribution or dynamics of the laser emission spectrum is caused by the test sample.

Abstract: An intracavity laser absorption infrared spectroscopy system for detecting trace analytes in vapor samples. The system uses a spectrometer in communications with control electronics, wherein the control electronics contain an analyte database that contains absorption profiles for each analyte the system is used to detect. The system can not only detect the presence of specific analytes, but identify them as well. The spectrometer uses a hollow cavity waveguide that creates a continuous loop inside of the device, thus creating a large path length and eliminating the need to mechanically adjust the path length to achieve a high Q-factor. In a preferred embodiment, the laser source may serve as the detector, thus eliminating the need for a separate detector.