Abstract:
3D metrology techniques are disclosed for determining a changing topography of a substrate processed in an additive manufacturing system. Techniques include fringe scanning, simultaneous fringe projections, interferometry, and x-ray imaging. The techniques can be applied to 3D printing systems to enable rapid topographical measurements of a 3D printer powder bed, or other rapidly moving, nearly continuous surface to be tested. The techniques act in parallel to the system being measured to provide information about system operation and the topography of the product being processed. A tool is provided for achieving higher precision, increasing throughput, and reducing the cost of operation through early detection and diagnosis of operating problems and printing defects. These techniques work well with any powder bed 3D printing system, providing real-time metrology of the powder bed, the most recently printed layer, or both without reducing throughput.
Abstract:
A system for measuring a target grating includes an illumination source, a reference transmission grating, a pupil filter, and a detector. The illumination source is disposed to generate an incident light beam that illuminates the reference transmission grating. The reference transmission grating splits the incident light beam into a plurality of diffraction orders. The plurality of diffraction orders interrogates a target grating. The reference transmission grating and the target grating are parallel. The pupil filter allows transmission of a subset of diffraction orders of light that has been diffracted and/or reflected from the target grating after being split again by passing through the reference transmission grating. The detector takes a measurement of the subset of diffraction orders of light after transmission through the pupil filter.
Abstract:
New and useful concepts for an autofocus system and method are provided. A basic concept uses fringe projection in an autofocus system and method. A further aspect provides spatial filtering concepts for the fringe projection concept. In yet another aspect, the fringe projection autofocus system and method is provided with temporal phase shifting using no moving parts. In a still further aspect, the fringe projection autofocus system and method is provided with unambiguous height measurement concepts.
Abstract:
System and method for monitoring of performance of a mirror array of a digital scanner with a use of a lateral shearing interferometer (operated in either static or a phase-shifting condition) to either simply identify problematic pixels for further troubleshooting or measure the exact magnitude of the mirror's deformation.
Abstract:
System and method for accurately measuring alignment of every exposure field on a pre-patterned wafer without reducing wafer-exposure throughput. Diffraction grating disposed in scribe-lines of such wafer, used as alignment marks, and array of encoder-heads (each of which is configured to define positional phase(s) of at least one such alignment mark) are used. Determination of trajectory of a wafer-stage scanning during the wafer-exposure in the exposure tool employs determining in-plane coordinates of such spatially-periodic alignment marks by simultaneously measuring position-dependent phases of signals produced by these marks as a result of recombination of light corresponding to different diffraction orders produced by these marks. Measurements may be performed simultaneously at all areas corresponding to at least most of the exposure fields of the wafer, and/or with use of a homodyne light source, and/or in a wavelength-independent fashion, and/or with a pre-registration process allowing for accommodation of wafers with differently-dimensioned exposure fields.
Abstract:
An encoder head configured for use with a lithographic exposure tool. The head is devoid of a multiplicity of stand-alone optical retroreflectors. The head includes a single, geometrically substantially perfect optically-isotropic cuboid complemented with optically-isotropic prismatic elements to form a contraption that, in combination with a diffraction grating disposed on a wafer-stage of the exposure tool, splits a single input beam of light delivered to the contraption into four measurement (sub-)beams of light (two in xz-plane, two in yz-plane) and causes each of these sub-beams traverse two prismatic elements and be retro-reflected internally within the cuboid to exit the encoder head at a non-zero angle with respect to the input beam of light, thereby solving problems of (i) structural complexity of a conventional encoder head for use in an exposure tool, (ii) burdensome alignment of the multitude of optical prisms in the process of forming such encoder head, and (iii) cyclic non-linear errors associated with measurements involving conventional corner-cubes-based encoder heads while, at the same time, reducing the geometrical footprint of the encoder head (without reducing the cross-section of the single input beam).
Abstract:
A measurement system for measuring the position of a work piece (28) includes a stage grating (234) and an encoder head (236). A first measurement beam (38A) is directed at the stage grating (234) at a first angle, the first measurement beam (38A) being at a first wavelength. A second measurement beam (38B) is directed at the stage grating (234) at a second angle that is different than the first angle, the second measurement beam (38B) being at a second wavelength that is different than the first wavelength. At least a portion of the first measurement beam (38A) and at least a portion of the second measurement beam (38B) are interfered with one another to create a measurement signal along a signal axis.
Abstract:
Laser radar systems include a pentaprism configured to scan a measurement beam with respect to a target surface. A focusing optical assembly includes a corner cube that is used to adjust measurement beam focus. Target distance is estimated based on heterodyne frequencies between a return beam and a local oscillator beam. The local oscillator beam is configured to propagate to and from the focusing optical assembly before mixing with the return beam. In some examples, heterodyne frequencies are calibrated with respect to target distance using a Fabry-Perot interferometer having mirrors fixed to a lithium aluminosilicate glass-ceramic tube.
Abstract:
A measurement system (22) for measuring the position of a work piece (28) along a first axis includes a grating (234), and an encoder head (238) that directs a first measurement beam (240) at the grating (234) at a first angle, and directs a second measurement beam (242) at the grating (234) at a second angle. An absolute value of the first angle relative to a normal (244) of the grating (234) is different from an absolute value of the second angle relative to the normal (244) of the grating (234). Additionally, the first measurement beam (240) has a first wavelength, and the second measurement beam (242) has a second wavelength that can be different from the first wavelength. Further, the first measurement beam (240) and the second measurement beam (242) can impinge at approximately the same location on the grating (234).
Abstract:
A detector (550) for detecting light (248B) from a light source (248A) comprises a single array of pixels (574) and a first mask (576). The single array of pixels (574) includes a plurality of rows of pixels (574R), and a plurality of columns of pixels (574C) having at least a first active column of pixels (574AC) and a spaced apart second active column of pixels (574AC). The first mask (576) covers one of the plurality of columns of pixels (574C) to provide a first masked column of pixels (574MC) that is positioned between the first active column of pixels (574AC) and the second active column of pixels (574AC). Additionally, a charge is generated from the light (248B) impinging on the first active column of pixels (574AC), is transferred to the first masked column of pixels (574MC), and subsequently is transferred to the second active column of pixels (574AC).