Abstract: Disclosed is a metrology apparatus for measuring a parameter of a lithographic process, and associated computer program and method. The metrology apparatus comprises an optical system for measuring a target on a substrate by illuminating the target with measurement radiation and detecting the measurement radiation scattered by the target; and an array of lenses. Each lens of the array is operable to focus the scattered measurement radiation onto a sensor, said array of lenses thereby forming an image on the sensor which comprises a plurality of sub-images, each sub-image being formed by a corresponding lens of the array of lenses. The resulting plenoptic image comprises image plane information from the sub-images, wavefront distortion information (from the relative positions of the sub-images) and pupil information from the relative intensities of the sub-images.

Abstract: An illumination system has a microLED array 502. The microLED array 502 is imaged or placed very close to a phosphor coated glass disc 504 which upconverts the light from the microLED array into a narrow band emission. The plate has at least two different photoluminescent materials arranged to be illuminated by the microLED array and to thereby emit output light. The different photoluminescent materials have different emission spectral properties of the output light, e.g. different center wavelength and optionally different bandwidth. Illumination of different photoluminescent materials by the illumination sources is selectable, by selective activation of the microLEDs or by movement of the photoluminescent materials relative to the illumination sources, to provide different illumination of the different photoluminescent materials. This provides tunable spectral properties of the output light.

Abstract: A method of adjusting a metrology apparatus, the method including: spatially dividing an intensity distribution of a pupil plane of the metrology apparatus into a plurality of pixels; and reducing an effect of a structural asymmetry in a target on a measurement by the metrology apparatus on the target, by adjusting intensities of the plurality of pixels.

Abstract: A metrology apparatus is disclosed that measures a structure formed on a substrate to determine a parameter of interest. The apparatus comprises an optical system configured to focus radiation onto the structure and direct radiation after reflection from the structure onto a detector, wherein: the optical system is configured such that the detector detects a radiation intensity resulting from interference between radiation from at least two different points in a pupil plane field distribution, wherein the interference is such that a component of the detected radiation intensity containing information about the parameter of interest is enhanced relative to one or more other components of the detected radiation intensity.

Abstract: Methods and apparatus for measuring a parameter of interest of a target structure formed on substrate are disclosed. In one arrangement, the target structure comprises a first sub-target and a second sub-target. The first sub-target comprises a first bias and the second sub-target comprises a second bias. The method comprises determining the parameter of interest using a detected or estimated reference property of radiation at a first wavelength scattered from the first sub-target and a detected or estimated reference property of radiation at a second wavelength scattered from the second sub-target. The first wavelength is different to the second wavelength.

Abstract: Methods and apparatuses for measuring a plurality of structures formed on a substrate are disclosed. In one arrangement, a method includes obtaining data from a first measurement process. The first measurement process including individually measuring each of the plurality of structures to measure a first property of the structure. A second measurement process is used to measure a second property of each of the plurality of structures. The second measurement process includes illuminating each structure with radiation having a radiation property that is individually selected for that structure using the measured first property for the structure.

Abstract: A radiation receiving system for an inspection apparatus, used to perform measurements on target structures on lithographic substrates as part of a lithographic process, comprises a spectrometer with a number of inputs. The radiation receiving system comprises: a plurality of inputs, each input being arranged to provide radiation from a target structure; a first optical element operable to receive radiation from each of the plurality of inputs; a second optical element operable to receive radiation from the first optical element and to scatter the radiation; and a third optical element operable to direct the scattered radiation onto a detector. The second optical element may for example be a reflective diffraction grating that diffracts incoming radiation into an output radiation spectrum.

Abstract: Measurement system comprising a radiation source configured to generate a measurement radiation beam, a polarizer and a grating to receive the measurement radiation beam and provide a polarized measurement radiation beam patterned by the grating, optics to form an image of the grating at a target location on a substrate. The image comprises a first part having a first polarization and a second part having a second polarization, detection optics to receive radiation from the target location of the substrate and form an image of the grating image at a second grating, and a detector to receive radiation transmitted through the second grating and produce a two output signal indicative of the intensity of the transmitted radiation for the first and second parts of the grating image respectively. Topography of the substrate can be determined from the signals.

Abstract: A topography measurement system comprising a radiation source configured to generate a radiation beam, a spatially coded grating configured to pattern the radiation beam and thereby provide a spatially coded radiation beam, optics configured to form an image of the spatially coded grating at a target location on a substrate, detection optics configured to receive radiation re-fleeted from the target location of the substrate and form an image of the grating image at a second grating, and a detector configured to receive radiation transmitted through the second grating and produce an output signal.

Abstract: Metrology apparatus and methods are disclosed. In one arrangement, a metrology apparatus comprises an optical system that illuminates a structure with measurement radiation and detects the measurement radiation scattered by the structure. The optical system comprises an array of lenses that focuses the scattered measurement radiation onto a sensor. A dispersive element directs scattered measurement radiation in each of a plurality of non-overlapping wavelength bands exclusively onto a different respective lens of the array of lenses.

Abstract: A lithographic apparatus comprises comprise a substrate table constructed to hold a substrate; and a sensor configured to sense a position of an alignment mark provided onto the substrate held by the substrate table. The sensor comprises a source of radiation configured to illuminate the alignment mark with a radiation beam, a detector configured to detect the radiation beam, having interacted with the alignment mark, as an out of focus optical pattern, and a data processing system. The data processing system is configured to receive image data representing the out of focus optical pattern, and process the image data for determining alignment information, comprising applying a lensless imaging algorithm to the out of focus optical pattern.

Abstract: A method comprises determining at least one property of a first marker feature corresponding to a marker of a lithographic patterning device installed in a lithographic apparatus, wherein the first marker feature comprises a projected image of the marker obtained by projection of radiation through the lithographic patterning device by the lithographic apparatus, the determining of at least one property of the projected image of the marker comprises using an image sensor to sense radiation of the projected image prior to formation of at least one desired lithographic feature on the substrate, and the method further comprises determining at least one property of a second marker feature arising from the same marker, after formation of said at least one desired lithographic feature on the substrate.

Abstract: Metrology apparatus and methods for measuring a structure formed on a substrate by a lithographic process are disclosed. In one arrangement an optical system illuminates the structure with radiation and detects radiation scattered by the structure. The optical system comprises a first dispersive element. The first dispersive element spectrally disperses scattered radiation exclusively from a first portion of a pupil plane field distribution along a first dispersion direction. A second dispersive element, separated from the first dispersive element, spectrally disperses scattered radiation exclusively from a second portion of the pupil plane field distribution, different from the first portion of the pupil plane field distribution, along a second dispersion direction.

Abstract: Methods of measuring a target formed by a lithographic process, a metrology apparatus and a polarizer assembly are disclosed. The target comprises a layered structure having a first periodic structure in a first layer and a second periodic structure in a second layer. The target is illuminated with polarized measurement radiation. Zeroth order scattered radiation from the target is detected. An asymmetry in the first periodic structure is derived using the detected zeroth order scattered radiation from the target. A separation between the first layer and the second layer is such that the detected zeroth order scattered radiation is independent of overlay error between the first periodic structure and the second periodic structure. The derived asymmetry in the first periodic structure is used to derive the correct overlay value between the first periodic structure and the second periodic structure.

Abstract: A broadband spectroscopic analysis is used for controlling a distance (d) between a miniature solid immersion lens (SIL, 60) and a metrology target (30?). An objective lens arrangement (15, 60) including the SIL illuminates the metrology target with a beam of radiation with different wavelengths and collects a radiation (709) reflected or diffracted by the metrology target. A mounting (64) holds the SIL within a distance from the metrology target that is less than the coherence length of the illuminating radiation (703). A detection arrangement (812, 818) produces a spectrum of the radiation reflected or diffracted by the metrology target. The distance between the SIL and the metrology target or other target surface can be inferred from spectral shifts observed in the detected spectrum. Servo control of the distance is implemented based on these shifts, using an actuator (66).

Abstract: An optical system (10) includes an arrangement for splitting a source beam into a measurement beam and a reference beam. The reference beam is reflected off a reflective element (42) which mounted on a delay line (44). A target (35) scatters the radiation from the measurement beam. The scattered radiation and the reference beam are brought to interfere on a detector (40) by calibrating the delay line (44). The detected interference pattern is Fourier-transformed and filtered to select a region of interest around a side-band of the Fourier-transformed interference pattern in order to remove noise caused by stray radiation that hits the detector.

Abstract: Metrology apparatus and methods are disclosed. In one arrangement, a metrology apparatus comprises an optical system that illuminates a structure with measurement radiation and detects the measurement radiation scattered by the structure. The optical system comprises an array of lenses that focusses the scattered measurement radiation onto a sensor. A dispersive element directs scattered measurement radiation in each of a plurality of non-overlapping wavelength bands exclusively onto a different respective lens of the array of lenses.

Abstract: Devices and methods for processing a radiation beam with coherence are disclosed. In one arrangement, an optical system receives a radiation beam with coherence. The radiation beam comprises components distributed over one or more radiation beam spatial modes. A waveguide supports a plurality of waveguide spatial modes. The optical system directs a plurality of the components of the radiation beam belonging to a common radiation beam spatial mode and having different frequencies onto the waveguide in such a way that each of the plurality of components couples to a different set of the waveguide spatial modes, each set comprising one or more of the waveguide spatial modes.

Abstract: An illumination system has a microLED array 502. The microLED array 502 is imaged or placed very close to a phosphor coated glass disc 504 which upconverts the light from the microLED array into a narrow band emission. The plate has at least two different photoluminescent materials arranged to be illuminated by the microLED array and to thereby emit output light. The different photoluminescent materials have different emission spectral properties of the output light, e.g. different center wavelength and optionally different bandwidth. Illumination of different photoluminescent materials by the illumination sources is selectable, by selective activation of the microLEDs or by movement of the photoluminescent materials relative to the illumination sources, to provide different illumination of the different photoluminescent materials. This provides tunable spectral properties of the output light.

Abstract: A scatterometer performs diffraction based measurements of one or more parameters of a target structure. To make two-color measurements in parallel, the structure is illuminated simultaneously with first radiation (302) having a first wavelength and a first angular distribution and with second radiation (304) having a second wavelength and a second angular distribution. The collection path (CP) includes a segmented wavelength-selective filter (21, 310) arranged to transmit wanted higher order portions of the diffracted first radiation (302X, 302Y) and of the diffracted second radiation (304X, 304Y), while simultaneously blocking zero order portions (302?, 304?) of both the first radiation and second radiation.