Abstract: A modulated reflectance measurement system includes three monochromatic diode-based lasers. Each laser can operate as a probe beam or as a pump beam source. The laser outputs are redirected using a series of mirrors and beam splitters to reach an objective lens. The objective lens focuses the laser outputs on a sample. Reflected energy returns through objective and is redirected by a beam splitter to a detector. A lock-in amplifier converts the output of the detector to produce quadrature (Q) and in-phase (I) signals for analysis. A Processor uses the Q and/or I signals to analyze the sample. By changing the number of lasers used as pump or probe beam sources, the measurement system can be optimized to measure a range of different samples types.

Abstract: The present invention provides a probe beam profile—modulated optical reflectivity metrology system having a modulated pump source for exciting the sample. A separate probe beam is directed to interact with the sample in a manner so that the rays within the probe beam create a spread of angles of incidence. A detector array simultaneously measures intensities of the rays within the reflected/diffracted probe beam simultaneously at different angles of incidence. The intensity and angle of incidence information is used to analyze the sample.

Abstract: A metrology tool for semiconductor wafers is disclosed which combines modulated reflectivity measurement with junction photovoltage measurements. The tool includes an intensity modulated pump beam for periodically exciting the sample. A separate probe beam is used to monitor changes in optical reflectivity of the sample. In addition, capacitive electrodes are provided to measure modulated changes in the voltage across the electrodes. These measurements are combined to evaluate the wafer. These measurement can be particularly useful in characterizing ultrashallow junctions.

Abstract: A modulated reflectance measurement system includes three monochromatic diode-based lasers. Each laser can operate as a probe beam or as a pump beam source. The laser outputs are redirected using a series of mirrors and beam splitters to reach an objective lens. The objective lens focuses the laser outputs on a sample. Reflected energy returns through objective and is redirected by a beam splitter to a detector. A lock-in amplifier converts the output of the detector to produce quadrature (Q) and in-phase (I) signals for analysis. A Processor uses the Q and/or I signals to analyze the sample. By changing the number of lasers used as pump or probe beam sources, the measurement system can be optimized to measure a range of different samples types.

Abstract: A modulated reflectance measurement system includes three monochromatic diode-based lasers. Each laser can operate as a probe beam or as a pump beam source. The laser outputs are redirected using a series of mirrors and beam splitters to reach an objective lens. The objective lens focuses the laser outputs on a sample. Reflected energy returns through objective and is redirected by a beam splitter to a detector. A lock-in amplifier converts the output of the detector to produce quadrature (Q) and in-phase (I) signals for analysis. A Processor uses the Q and/or I signals to analyze the sample. By changing the number of lasers used as pump or probe beam sources, the measurement system can be optimized to measure a range of different samples types.

Abstract: A method is disclosed for determining peak carrier concentration in ultra shallow junctions of semiconductor samples. A region of the surface of the sample is periodically excited. The effects of the excitation are monitored by a probe beam. Synchronous detection produces in-phase (I) and quadrature (Q) signals. These signals are compared to signals obtained from calibration samples to evaluate peak carrier concentration.

Abstract: A modulated reflectance measurement system includes lasers for generating an intensity modulated pump beam and a UV probe beam. The pump and probe beams are focused on a measurement site within a sample. The pump beam periodically excites the measurement site and the modulation is imparted to the probe beam. For one embodiment, the wavelength of the probe beam is selected to correspond to a local maxima of the temperature reflectance coefficient of the sample. For a second embodiment, the probe laser is tuned to either minimize the thermal wave contribution to the probe beam modulation or to equalize the thermal and plasma wave contributions to the probe beam modulation.

Abstract: Methods of obtaining dopant and damage depth profile information are disclosed using modulated optical reflectivity (MOR) measurements. In one aspect, the depth profile is constructed using information obtained from various measurements such as the junction depth, junction abruptness and dopant concentration. In another aspect, a full theoretical model is developed. Actual measurements are fed to the model. Using an iterative approach, the actual measurements are compared to theoretical measurements calculated from the model to determine the actual depth profile.

Abstract: A modulated reflectance measurement system includes lasers for generating an intensity modulated pump beam and a UV probe beam. The pump and probe beams are focused on a measurement site within a sample. The pump beam periodically excites the measurement site and the modulation is imparted to the probe beam. For one embodiment, the wavelength of the probe beam is selected to correspond to a local maxima of the temperature reflectance coefficient of the sample. For a second embodiment, the probe laser is tuned to either minimize the thermal wave contribution to the probe beam modulation or to equalize the thermal and plasma wave contributions to the probe beam modulation.

Abstract: A modulated optical reflectance (MOR) measurement system is disclosed which uses an infrared probe beam. Preferably the probe beam has a wavelength of at least 800 nm and preferable greater than one micron (1000 nm).

Abstract: The present invention provides a probe beam profile—modulated optical reflectivity metrology system having a modulated pump source for exciting the sample. A separate probe beam is directed to interact with the sample in a manner so that the rays within the probe beam create a spread of angles of incidence. A detector array simultaneously measures intensities of the rays within the reflected/diffracted probe beam simultaneously at different angles of incidence. The intensity and angle of incidence information is used to analyze the sample.

Abstract: The repeatability of wafer uniformity measurements can be increased by taking spatially averaged measurements of wafer response. By increasing the time over which measurements are obtained, the amount of noise can be significantly reduced, thereby improving the repeatability of the measurements. These measurements can be taken at several locations on the wafer to ensure wafer uniformity. In order to get a stable and repeatable assessment of the wafer process, addressing uncertainties related to damage relaxation or incomplete anneal, an anneal decay factor (ADF) characterization can be performed at a distance away from the TW measurement boxes. From the ADF measurement and the spatially averaged measurements of wafer response, a repeatable assessment of the wafer process can be obtained.

Abstract: The ability of a Modulated Optical Reflectivity (MOR) or Thermal Wave (TW) system to measure characteristics of a sample based on the amplitude and phase of a probe beam reflected from the surface of the sample can be improved by providing a polychromatic pump and/or probe beam that can be scanned over a wide spectral range, such as a range of at least 100 nm. The information contained in the spectral dependencies of a TW response obtained from the sample can be compared and/or fitted to corresponding theoretical dependencies in order to obtain more precise and reliable information about the properties of the particular sample than is available for single-wavelength systems. This information can further be combined with measurements taken for varying spot separations or varying pump source modulation frequency, as well as with photo-thermal radiometry (PTR), spectroscopic reflectometry, and/or ellipsometry measurements.

Abstract: A metrology tool for semiconductor wafers is disclosed which combines modulated reflectivity measurement with junction photovoltage measurements. The tool includes an intensity modulated pump beam for periodically exciting the sample. A separate probe beam is used to monitor changes in optical reflectivity of the sample. In addition, capacitive electrodes are provided to measure modulated changes in the voltage across the electrodes. These measurements are combined to evaluate the wafer. These measurement can be particularly useful in characterizing ultrashallow junctions.

Abstract: To measure USJ profile abruptness, a PMR-type optical metrology tool is to perform a series of two or more measurements, each with different pump/probe beam separations. Quadrature (Q) and in-phase (I) measurements are obtained for each measurement and used to derive a line in I-Q space. An abruptness measurement is derived by comparing the line slope to a similar line slope obtained for a sample having a known USJ profile. USJ profile depth is measured by obtaining quadrature (Q) values for one or more measurements. Each Q value is translated to a corresponding depth measurement using a table or similar lookup device.

Abstract: A system for evaluating semiconductor wafers includes illumination sources for generating probe and pump beams. The pump beam is focused on the surface of a sample and a beam steering mechanism is used to modulate the point of focus in a predetermined pattern. The moving pump beam introduces thermal and plasma waves in the sample causing changes in the reflectivity of the surface of the sample. The probe beam is focused within or adjacent to the area illuminated by the pump beam. The reflected probe beam is gathered and used to measure the changes in reflectivity induced by the pump beam. By analyzing changes in reflectivity, a processor is able to deduce structure and chemical details of the sample.

Abstract: A modulated reflectance measurement system includes lasers for generating an intensity modulated pump beam and a UV probe beam. The pump and probe beams are focused on a measurement site within a sample. The pump beam periodically excites the measurement site and the modulation is imparted to the probe beam. For one embodiment, the wavelength of the probe beam is selected to correspond to a local maxima of the temperature reflectance coefficient of the sample. For a second embodiment, the probe laser is tuned to either minimize the thermal wave contribution to the probe beam modulation or to equalize the thermal and plasma wave contributions to the probe beam modulation.

Abstract: A modulated reflectance measurement system includes three monochromatic diode-based lasers. Each laser can operate as a probe beam or as a pump beam source. The laser outputs are redirected using a series of mirrors and beam splitters to reach an objective lens. The objective lens focuses the laser outputs on a sample. Reflected energy returns through objective and is redirected by a beam splitter to a detector. A lock-in amplifier converts the output of the detector to produce quadrature (Q) and in-phase (I) signals for analysis. A Processor uses the Q and/or I signals to analyze the sample. By changing the number of lasers used as pump or probe beam sources, the measurement system can be optimized to measure a range of different samples types.

Abstract: A modulated reflectance measurement system includes lasers for generating an intensity modulated pump beam and a UV probe beam. The pump and probe beams are focused on a measurement site within a sample. The pump beam periodically excites the measurement site and the modulation is imparted to the probe beam. For one embodiment, the wavelength of the probe beam is selected to correspond to a local maxima of the temperature reflectance coefficient of the sample. For a second embodiment, the probe laser is tuned to either minimize the thermal wave contribution to the probe beam modulation or to equalize the thermal and plasma wave contributions to the probe beam modulation.

Abstract: A modulated reflectance measurement system includes three monochromatic diode-based lasers. Each laser can operate as a probe beam or as a pump beam source. The laser outputs are redirected using a series of mirrors and beam splitters to reach an objective lens. The objective lens focuses the laser outputs on a sample. Reflected energy returns through objective and is redirected by a beam splitter to a detector. A lock-in amplifier converts the output of the detector to produce quadrature (Q) and in-phase (I) signals for analysis. A Processor uses the Q and/or I signals to analyze the sample. By changing the number of lasers used as pump or probe beam sources, the measurement system can be optimized to measure a range of different samples types.