Abstract:
Methods and apparatus for fabricating a semiconductor die including several target structures. A first layer is formed that includes one or more line or trench structures that extend in a first direction (310). A second layer is formed that includes one or more line or trench structures that extend in a second direction that is perpendicular to the first structure, such that a projection of the target structure along the first direction is independent of the second direction and a projection of the target structure along the second direction is independent of the first direction (320). A target structure and a method for generating a calibration curve are also described.
Abstract:
A system for imaging an acquisition target or an overlay or alignment semiconductor target (404) is disclosed. The system includes a beam generator for directing at least one incident beam (402) having a wavelength lamda towards a periodic target (404) having structures with a specific pitch p. A plurality of output beams (406) are scattered from the periodic target (404) in response to the at least one incident beam (402). The system further includes an imaging lens system (410) for passing only a first and second output beam (412a, 412b) from the target (404). The imaging system is adapted such that the angular separation between the captured beams, lamda, and the pitch are selected to cause the first and second output beams (412a, 412b) to form a sinusoidal image (414). The system also includes a sensor for imaging the sinusoidal image or images (414), and a controller for causing the beam generator to direct the at least one incident beam (402) towards the periodic target or targets (404), and for analyzing the sinusoidal image or images (414).
Abstract:
An emissivity compensating non-contact system for measuring the temperature of a semiconductor wafer (24). The system includes a semiconductor wafer emissivity compensation station (10) for measuring the reflectivity of the wafer (24) at discrete wavelengths to yield wafer emissivity in specific wavelength bands. The system further includes a measurement probe (13) which is optically coupled to a semiconductor process chamber (12). The probe (13) senses wafer self-emission using one or more optical detectors (40) and a light modulator (42). A background temperature determining mechanism (44) independently senses the temperature of a source (46) of background radiation. Finally, a mechanism (16) calculates the temperature of the semiconductor wafer based on reflectivity and self-emission of the wafer and background temperature.
Abstract:
A method of characterizing a process by selecting the process to characterize, selecting a parameter of the process to characterize, determining values of the parameter to use in a test matrix, specifying an eccentricity for the test matrix, selecting test structures to be created in cells on a substrate, processing the substrate through the process using in each cell the value of the parameter as determined by the eccentric test matrix, measuring a property of the test structures in the cells, and developing a correlation between the parameter and the property.
Abstract:
Metrology may be implemented during semiconductor device fabrication by a) modeling a first measurement on a first test cell formed in a layer of a partially fabricated device; b) performing a second measurement on a second test cell in the layer; c) feeding information from the second measurement into the modeling of the first measurement; and after a lithography pattern has been formed on the layer including the first and second test cells, d) modeling a third and a fourth measurement on the first and second test cells respectively using information from a) and b) respectively.
Abstract:
In one embodiment, a system for imaging an acquisition target or an overlay or alignment semiconductor target is disclosed. The system includes a beam generator for directing at least one incident beam having a wavelength l towards a periodic target having structures with a specific pitch p. A plurality of output beams are scattered from the periodic target in response to the at least one incident beam. The system further includes an imaging lens system for passing only a first and a second output beam from the target. The imaging system is adapted such that the angular separation between the captured beams, l, and the pitch are selected to cause the first and second output beams to form a sinusoidal image. The system also includes a sensor for imaging the sinusoidal image or images, and a controller for causing the beam generator to direct the at least one incident beam towards the periodic target or targets, and for analyzing the sinusoidal image or images. In one application the detector detects a sinusoidal image of an acquisition target with the same pitch as the designed target and the controller analyzes the pitch of the sinusoidal image compared to design data to determine whether the target has been successfully acquired. In a second application a first and second periodic target that each have a specific pitch p are imaged so that the detector detects a first sinusoidal image of the first target and a second sinusoidal image of the second target and the controller analyzes the first and second sinusoidal image to determine whether the first and second targets have an overlay or alignment error.
Abstract:
A method of determining the thickness map of a film (14) overlying a substrate (14). This method includes illuminating (10) the film simultaneously from different angles and analyzing spectral intensity of the radiation reflected by each point on the film (14). The analysis is effected by collecting reflected radiation from the film (14), passing the radiation through an interferometer (16) which outputs modulated radiation corresponding to a predetermined set of linear combinations of the spectral intensity of the radiation emitted from each pixel, simultaneously and separately scanning optical path differences generated in the interferometer (16) for each pixel, focusing the radiation outputted from the interferometer (16) on a detector array, and processing the output of the detector array to determine the spectral intensity of each pixel thereof to obtain a spectral intensity distribution. Finally, the method includes further processing the spectral intensity distribution to determine the spatial distribution of the thickness of the film (16).
Abstract:
A metrology target design may be optimized using inputs including metrology target design information, substrate information, process information, and metrology system information. Acquisition of a metrology signal with a metrology system may be modeled using the inputs to generate one or more optical characteristics of the metrology target. A metrology algorithm may be applied to the characteristics to determine a predicted accuracy and precision of measurements of the metrology target made by the metrology system. Part of the information relating to the metrology target design may be modified and the signal modeling and metrology algorithm may be repeated to optimize the accuracy and precision of the one or more measurements. The metrology target design may be displayed or stored after the accuracy and precision are optimized.
Abstract:
The present invention relates to overlay marks and methods for determining overlay error. One aspect of the present invention relates to a continuously varying offset mark. The continuously varying offset mark is a single mark that includes over laid periodic structures, which have offsets that vary as a function of position. By way of example, the periodic structures may correspond to gratings with different values of a grating characteristic such as pitch. Another aspect of the present invention relates to methods for determining overlay error from the continuously varying offset mark. The method generally includes determining the center of symmetry of the continuously varying offset mark and comparing it to the geometric center of the mark. If there is zero overlay, the center of symmetry tends to coincide with the geometric center of the mark. If overlay is non zero (e.g., misalignment between two layers), the center of symmetry is displaced from the geometric center of the mark. The displacement in conjunction with the preset gain of the continuously varying offset mark is used to calculate the overlay error.