Abstract:
Metrology methods are provided, which comprise identifying overlay critical patterns in a device design, the overlay critical patterns having an overlay sensitivity to process variation above a specified threshold that depends on design specifications; and using metrology targets that correspond to the identified overlay critical patterns. Alternatively or complementarily, metrology methods comprise identifying yield critical patterns according to a corresponding process window narrowing due to specified process variation, wherein the narrowing is defined by a dependency of edge placement errors (EPEs) of the patterns on process parameters. Corresponding targets and measurements are provided.
Abstract:
In one embodiment, a semiconductor target for detecting overlay error between two or more successive layers of a substrate or between two or more separately generated patterns on a single layer of a substrate is disclosed. The target comprises at least a plurality of a plurality of first grating structures having a course pitch that is resolvable by an inspection tool and a plurality of second grating structures positioned relative to the first grating structures. The second grating structures have a fine pitch that is smaller than the course pitch, and the first and second grating structures are both formed in two or more successive layers of a substrate or between two or more separately generated patterns on a single layer of a substrate. The first and second gratings have feature dimensions that all comply with a predefined design rules specification.
Abstract:
The present invention may include performing a first measurement on a wafer of a first lot of wafers via an omniscient sampling process, calculating a first set of process tool correctables utilizing one or more results of the measurement performed via an omniscient sampling process, randomly selecting a set of field sampling locations of the wafer of a first lot of wafers, calculating a second set of process tool correctables by applying an interpolation process to the randomly selected set of field sampling locations, wherein the interpolation process utilizes values from the first set of process tool correctables for the randomly selected set of field sampling locations in order to calculate correctables for fields of the wafer of the first lot not included in the set of randomly selected fields, and determining a sub-sampling scheme by comparing the first set of process tool correctables to the second set of correctables.
Abstract:
A resultant image of a grating target may be obtained by dividing an image of the target into first and second portions and optically modifying the first and/or second portion such that a final image formed from their combination is characterized by a Moiré pattern. The resultant image may be analyzed to determine a shift in the grating target from a shift in the Moiré pattern. Optical alignment apparatus may include a first beam splitter, an image transformation element optically coupled to the first beam splitter, and a second beam splitter. The first beam splitter divides an image of a grating target into first and second portions. The second beam splitter combines the first portion and the second portion. The image transformation element optically modifies the first and/or second portion such that a final image formed from their combination is characterized by a Moiré pattern.
Abstract:
Metrology targets and methods are provided, which provide self-Moiré measurements of unresolved target features, i.e., interaction of electromagnetic fields re-scattered off elements within a single target layer provides signals with Moiré pitches that are measurable, although the actual target pitches are unresolved and possibly device-like. Targets comprise cell(s) with interlaced lines of elements having different device-like pitches which are selected to yield resolved Moiré pitch(es). Different target designs are presented for scatterometry and imaging metrology measurements, as well as for critical dimension, dose and focus, and pitch walk measurements - of device-like targets.
Abstract:
Scatterometry targets, measurement and calibration methods as well as metrology systems are provided, which exhibit reflection symmetry instead of prior art rotational symmetry. Targets are designed to be reflection symmetric with respect to one, two or more reflection planes, and respective measurement methods and tool calibration methods are introduced. The disclosure removes inaccuracies involved in present targets and measurement procedures that result from using rotationally symmetric targets and calibrations, and new types of targets and scatterometry information sources are presented.
Abstract:
The disclosure is directed to various apodization schemes for pupil imaging scatterometry. In some embodiments, the system includes an apodizer disposed within a pupil plane of the illumination path. In some embodiments, the system further includes an illumination scanner configured to scan a surface of the sample with at least a portion of apodized illumination. In some embodiments, the system includes an apodized pupil configured to provide a quadrupole illumination function. In some embodiments, the system further includes an apodized collection field stop. The various embodiments described herein may be combined to achieve certain advantages.
Abstract:
Metrology methods, systems and targets are provided, which implement a side by side paradigm. Adjacent cells with periodic structures are used to extract the overlay error, e.g., by introducing controllable phase shifts or image shifts which enable algorithmic computation of the overlay. The periodic structures are designed to exhibit a rotational symmetry to support the computation and reduce errors.
Abstract:
A method for determining an overlay offset may include, but is not limited to: obtaining a first anti-symmetric differential signal (ΔS 1 ) associated with a first scatterometry cell; obtaining a second anti-symmetric differential signal (ΔS 2 ) associated with a second scatterometry cell and computing an overlay offset from the first anti-symmetric differential (ΔS 1 ) signal associated with the first scatterometry cell and the second anti-symmetric differential signal (ΔS 2 ) associated with the second scatterometry cell.