Abstract: A normalization procedure for an ellipsometric system having a rotating optical element such as a polarizer or compensator is disclosed. In operation, a first DC component is extracted from the measured output signals obtained during the first 180 degrees of rotation of the optical element and a second DC component is extracted from the output signals obtained during the second 180 degrees of rotation of the optical element. The first DC component is used to normalize the output signals obtained during the first 180 degrees of rotation of the optical element and the second DC component is used to normalize the output signals obtained during the second 180 degrees of rotation of the optical element.

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 combiner for optical beams includes a substrate overlaid by a multi-layer dielectric film stack. The substrate is a clear material and the dielectric film stack is a series of alternating layer of high and low refractive index. This gives the combiner relatively high reflectivity across UV wavelengths and relatively high transmissivity in the visible and longer wavelengths and allows visible light to pass through the combiner while UV light is reflected. At the same time dielectric film stack has minimal absorption and scatter. This means that the intensity of visible light maintains at least 90% of its intensity as it passes through combiner and UV light retains at least 90% of its intensity as it is reflected by combiner.

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 method and apparatus are disclosed for evaluating relatively small periodic structures formed on semiconductor samples. In this approach, a light source generates a probe beam which is directed to the sample. In one preferred embodiment, an incoherent light source is used. A lens is used to focus the probe beam on the sample in a manner so that rays within the probe beam create a spread of angles of incidence. The size of the probe beam spot on the sample is larger than the spacing between the features of the periodic structure so some of the light is scattered from the structure. A detector is provided for monitoring the reflected and scattered light. The detector includes multiple detector elements arranged so that multiple output signals are generated simultaneously and correspond to multiple angles of incidence. The output signals are supplied to a processor which analyzes the signals according to a scattering model which permits evaluation of the geometry of the periodic structure.

Abstract: An apparatus for scatterometry measurements is disclosed. The apparatus includes a modulated pump source for exciting the sample. A separate probe beam is directed to interact with the sample and the modulated optical response is measured. The measured data is subjected to a scatterometry analysis in order to evaluate geometrical sample features that induce light scattering.

Abstract: A method for simulating the optical properties of samples having non-uniform line edges includes creating a model for the sample being analyzed. To simulate roughness, lines within the model are represented as combinations of three dimensional objects, such as circular or elliptical mesas. The three-dimensional objects are arranged in a partially overlapping linear fashion. The objects, when spaced closely together resemble a line with edge roughness that corresponds to the object size and pitch. A second method allows lines within the model to vary in width over their lengths. The model is evaluated using a suitable three-dimensional technique to simulate the optical properties of the sample being analyzed.

Abstract: The subject invention relates to a broadband optical metrology system that segregates the broadband radiation into multiple sub-bands to improve overall performance. Each sub-band includes only a fraction of the original bandwidth. The optical path—the light path that connects the illuminator, the sample and the detector—of each sub-band includes a unique sub-band optical system designed to optimize the performance over the spectral range spanned by the sub-band radiation. All of the sub-band optical systems are arranged to provide small-spot illumination at the same measurement position. Optional purging of the individual sub-band optical paths further improves performance.

Abstract: A method for modeling the complex refractive index of doped, strained or ultra-thin semiconductors starts with a model for a standard bulk material which may be in any form such as a pre-existing lookup table, a dispersion model derived from an effective medium approximation (EMA) or a critical point (CP) model. The modeling method perturbs the ?2 curve of the bulk material by enhancing, suppressing or shifting the strong features of the curve. A Kramers-Kronig transformation is then applied to the ?2 perturbation to obtain the corresponding perturbation to the ?1 curve. The combination of the perturbed ?2 curve and the correspondingly perturbed ?1 curve are then used to obtain the complex dielectric function or complex refractive index of the modified material.

Abstract: Fluid immersion technology can be utilized to increase the resolution and angular range of existing metrology systems. An immersion fluid placed between the metrology optics and the sample can reduce the refraction at the sample interface, thereby decreasing the spot size of the beam on a feature of the sample while simultaneously increasing the angular range of the system. The decreased spot size, in combination with an increased angular spread, allows an existing metrology system to measure parameters of a sample, such as a semiconductor or microelectronic device, with improved resolution and without expensive and/or complex changes to the mechanics of the metrology system.

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: An apparatus is disclosed for obtaining ellipsometric measurements from a sample. A probe beam is focused onto the sample to create a spread of angles of incidence. The beam is passed through a quarter waveplate retarder and a polarizer. The reflected beam is measured by a detector. In one preferred embodiment, the detector includes eight radially arranged segments, each segment generating an output which represents an integration of multiple angle of incidence. A processor manipulates the output from the various segments to derive ellipsometric information.

Abstract: An optical inspection device includes a light source for generating a probe beam. The probe beam is focused onto a sample to create a spread of angles of incidence. After reflecting from the sample, the light is imaged onto a two dimensional array of photodetectors. Prior to reaching the detector array, the beam is passed through a rotating compensator. A processor functions to evaluate the sample by analyzing the output of the photodetectors lying along one or more azimuthal angles and at different compensator positions.

Abstract: An infrared filter for an optical metrology tool includes a substrate having film stacks on opposing surfaces thereof. A first film stack can be used to reflect ultra-violet radiation and transmit radiation at non-ultraviolet wavelengths. The second film stack can be used to reflect visible to near-infrared radiation and transmit infrared radiation. The combination of film stacks can therefore extract infrared radiation from a broadband beam, with the remaining ultra-violet radiation and visible to near-infrared radiation forming the product of the filter. The filter can be used as part of the illumination or collection side optics in a broadband optical metrology tool.

Abstract: A system for focusing broadband light within a reflectometer includes a concave spherical mirror for gathering light from the surface of a sample under inspection. The concave spherical mirror projects the received light to a convex spherical mirror. The combination of the two mirrors captures the light diverging from the sample and collimates the light into parallel rays. The light can then be passed through an aperture prior to entering a detector. Each of the two mirrors is fabricated as an off-axis section of a spherical mirror and positioned to form a partial Schwarzschild design without the associated problem of a central obscuration.

Abstract: A normal incidence rotating compensator ellipsometer includes an illumination source that produces a broadband probe beam. The probe beam is redirected by a beam splitter to be normally incident on a sample under test. Before reaching the sample, the probe beam is passed through a rotating compensator. The probe beam is reflected by the sample and passes through the rotating compensator a second time before reaching a detector. The detector converts the reflected probe beam into equivalent signals for analysis.

Abstract: A flat spectrum illumination source for use in optical metrology systems includes a first light source generating a visible light beam and a second light source generating an ultraviolet light beam. The illumination source also includes an auxiliary light source generating a light beam at wavelengths between the visible light beam and the ultraviolet light beam. The three light beams are combined to provide a broadband probe beam that has substantially even illumination levels across a broad range of wavelengths. Alternately, the illumination source may be fabricated as an array of light emitting diodes selected to cover a range of separate wavelengths. The outputs of the LED array are combined to produce the broadband probe beam.

Abstract: A method for modeling samples includes the use of control points to define lines profiles and other geometric shapes. Each control point used within a model influences a shape within the model. Typically, the control points are used in a connect-the-dots fashion where a set of dots defines the outline or profile of a shape. The layers within the sample are typically modeled independently of the shape defined using the control points. The overall result is to minimize the number of parameters used to model shapes while maintaining the accuracy of the resulting scatterometry models.

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.