Abstract: A system and method are disclosed for gas sensing over a wide tunable wavelength range provided by one or more quantum cascade lasers. A laser beam is generated within the wide tunable wavelength range, which is given by the sum of the wavelength ranges from the individual lasers. Gas sensing or detection is achieved by obtaining an infrared absorption spectrum for a sample contained in one or more cells having different path lengths for the laser beam.

Abstract: A system and method are disclosed for gas sensing over a wide tunable wavelength range provided by one or more quantum cascade lasers. A laser beam is generated within the wide tunable wavelength range, which is given by the sum of the wavelength ranges from the individual lasers. Gas sensing or detection is achieved by obtaining an infrared absorption spectrum for a sample contained in one or more cells having different path lengths for the laser beam.

Abstract: A system and method are disclosed for gas sensing over a wide tunable wavelength range provided by one or more quantum cascade lasers. A laser beam is generated within the wide tunable wavelength range, which is given by the sum of the wavelength ranges from the individual lasers. Gas sensing or detection is achieved by obtaining an infrared absorption spectrum for a sample contained in one or more cells having different path lengths for the laser beam.

Abstract: The penetration depth of surface acoustic wave scales with wavelength. To measure thinner films using impulse stimulated thermal scattering (ISTS) it is advantageous to reduce the measurement wavelength to on the order of 1 micron. One way to reduce the measurement wavelength is to employ a high numerical aperture lens to converge an excitation and probe laser beam in an optical system at wider angles. While doing this, the increased optical/mechanical tolerances can be reduced by fine-tuning the phase between an excitation laser pattern and a probe laser pattern by adjusting either a neutral-density filter or matching plate for a particular wavelength. Blocking unwanted diffraction order beams generated by the optical system with a specialized design beam block plate is needed to retain the long wavelength capability.

Abstract: The invention represents an improved method of measuring trenches on semiconductor wafers with optical spectroscopy. According to the described method, it is possible to characterize not only depth but also shape of the trench. The advancement is achieved by improved Effective Medium Approximation-based modeling of the optical response of trench structures.

Abstract: The penetration depth of surface acoustic wave scales with wavelength. To measure thinner films using impulse stimulated thermal scattering (ISTS) it is advantageous to reduce the measurement wavelength to on the order of 1 micron. One way to reduce the measurement wavelength is to employ a high numerical aperture lens to converge an excitation and probe laser beam in an optical system at wider angles. While doing this, the increased optical/mechanical tolerances can be reduced by fine-tuning the phase between an excitation laser pattern and a probe laser pattern by adjusting either a neutral-density filter or matching plate for a particular wavelength. Blocking unwanted diffraction order beams generated by the optical system with a specialized design beam block plate is needed to retain the long wavelength capability.

Abstract: The invention represents an improved method of measuring trenches on semiconductor wafers with optical spectroscopy. According to the described method, it is possible to characterize not only depth but also shape of the trench. The advancement is achieved by improved Effective Medium Approximation-based modeling of the optical response of trench structures.

Abstract: Structures are characterized by exposing a sample to optical radiation, measuring a spectrum associated with the exposure, detecting at least one characteristic parameter in the measured spectrum, and computing at least one structural parameter based on the at least one characteristic parameter.

Abstract: In an opto-acoustic measuring device for thin films and solid surfaces, the probe beam is split into a first probe beam portion and a second reference beam portion. The splitting of the probe beam is achieved using a phase mask that also splits the excitation beam. The probe beam is aligned using a retro-reflector on a motorized stage to control the beam angle. Excitation and probe/reference beams are overlapped at the sample surface. The first probe beam portion gets diffracted by material disturbances generated by excitation beams. The diffracted part of the first probe beam portion is collinear with the second reference beam portion, resulting in heterodyning. The heterodyne signal measured by the detector is analyzed in order to determine thickness and/or other properties of a thin film or solid surface. The invention improves magnitude and reproducibility of the opto-acoustic signal which results in enhanced precision of measurements.

Abstract: In an opto-acoustic measuring device for thin films and solid surfaces, the probe beam is split into a first probe beam portion and a second reference beam portion. The splitting of the probe beam is achieved using a phase mask that also splits the excitation beam. The probe beam is aligned using a retro-reflector on a motorized stage to control the beam angle. Excitation and probe/reference beams are overlapped at the sample surface. The first probe beam portion gets diffracted by material disturbances generated by excitation beams. The diffracted part of the first probe beam portion is collinear with the second reference beam portion, resulting in heterodyning. The heterodyne signal measured by the detector is analyzed in order to determine thickness and/or other properties of a thin film or solid surface. The invention improves magnitude and reproducibility of the opto-acoustic signal which results in enhanced precision of measurements.