Abstract:
A periodic structure is illuminated by polychromatic electromagnetic radiation. Radiation from the structure is collected and divided into two rays having different polarization states. The two rays are detected from which one or more parameters of the periodic structure may be derived. In another embodiment, when the periodic structure is illuminated by a polychromatic electromagnetic radiation, the collected radiation from the structure is passed through a polarization element having a polarization plane. The element and the polychromatic beam are controlled so that the polarization plane of the element are at two or more different orientations with respect to the plane of incidence of the polychromatic beam. Radiation that has passed through the element is detected when the plane of polarization is at the two or more positions so that one or more parameters of the periodic structure may be derived from the detected signals. At least one of the orientations of the plane of polarization is substantially stationary when the detection takes place. To have as small a footprint as possible, one employs an optical device that includes a first element directing a polychromatic beam of electromagnetic radiation to the structure and a second optical element collecting radiation from the structure where the two elements form an integral unit or are attached together to form an integrated unit. To reduce the footprint, the measurement instrument and the wafer are both moved. In one embodiment, both the apparatus and the wafer undergo translational motion transverse to each other. In a different arrangement, one of the two motions is translational and the other is rotational. Any one of the above-described embodiments may be included in an integrated processing and detection apparatus which also includes a processing system processing the sample, where the processing system is responsive to the output of any one of the above embodiments for adjusting a processing parameter.
Abstract:
Disclosed are apparatus and methods for finding lithographically significant defects on a reticle. In general, at least a pair of related intensity images of the reticle in question are obtained using an inspection apparatus. The intensity images are obtained such that each of the images experience different focus settings for the reticle so that there is a constant focus offset between the two focus values of the images. These images are then analyzed to obtain a transmission function of the reticle. This transmission function is then input into a model of the lithography system (e.g., a stepper, scanner, or other related photolithography system) to then produce an aerial image of the reticle pattern. The aerial image produced can then be input to a photoresist model to yield a “resist-modeled image” that corresponds to an image pattern to be printed onto the substrate using the reticle. This resist-modeled image can then be compared with a reference image to obtain defect information. In particular, due to the introduction of the lithography tool and photoresist model, this defect information pertains to lithographically significant defects.
Abstract:
A method for reducing overlay error in a photolithographic process, by providing a substrate having a permanent layer with a first pattern disposed therein, coating the substrate with photoresist, exposing the photoresist to a second pattern, while measuring temperatures at a plurality of different first positions across the substrate, developing the second pattern in the photoresist, measuring overlay errors between the first and second patterns at a plurality of different second positions across the substrate, correlating the overlay errors with temperatures by position on the substrate, determining any relationship indicated between the correlated overlay errors and temperatures, and adjusting at least one temperature controlling aspect of the photolithographic process in response to any relationship determined.
Abstract:
One embodiment relates to a charged-particle beam apparatus. The apparatus includes at least a source for generating the charged-particle beam, a first deflector, and a second deflector. The first deflector is configured to scan the charged-particle beam in a first dimension. The second deflector is configured to deflect the scanned beam such that the scanned beam impinges telecentrically (perpendicularly) upon a surface of a target substrate. Other embodiments are also disclosed.
Abstract:
A method and apparatus for inspecting patterned substrates, such as photomasks, for unwanted particles and features occurring on the transmissive as well as pattern defects. A transmissive substrate is illuminated by a laser through an optical system comprised of a laser scanning system, individual transmitted and reflected light collection optics and detectors collect and generate signals representative of the light transmitted and reflected by the substrate. The defect identification of the substrate is performed using transmitted and reflected light signals from a baseline comparison between two specimens, or one specimen and a database representation, to form a calibration pixelated training set including a non-defective region. This calibration pixilated training set is compared to a transmitted-reflected plot map of the subject specimen to assess surface quality.
Abstract:
A surface inspection of the system applies a first oblique illumination beam and may also apply a second illumination beam to illuminate a surface either sequentially or simultaneously. Radiation reflected or scattered is collected by preferably three collection channels and detected by three corresponding detector arrays, although a different number of channels and detector arrays may be used. One or both illumination beams are focused to a line on the surface to be inspected and each line is imaged onto one or more detector arrays in the up to three or more detection and collection channels. Relative motion is caused between the lines and the surface inspected in a direction perpendicular to the lines, thereby increasing throughput while retaining high resolution and sensitivity. The same detection channels may be employed by detecting scattered or reflected radiation from both illumination beams. Fourier filters may be employed to filter out diffraction at one or more different spatial frequencies.
Abstract:
The invention is a method for generating a design rule map having a spatially varying overlay error budget. Additionally, the spatially varying overlay error budget can be employed to determine if wafers are fabricated in compliance with specifications. In one approach a design data file that contains fabrication process information and reticle information is processed using design rules to obtain a design map with a spatially varying overlay error budget that defines a localized tolerance to overlay errors for different spatial locations on the design map. This spatially varying overlay error budget can be used to disposition wafers. For example, overlay information obtained from measured metrology targets on a fabricated wafer are compared with the spatially varying overlay error budget to determine if the wafer overlay satisfies the required specification.
Abstract:
A system and method for measuring defects, film thickness, contamination, particles and height of a thin film disk or a silicon wafer. The system includes a processor for determining height. In addition to measuring the height the system can measure film thickness and defects through the measurement of the phase shift of optical signals. An optical profilometer is described which can measure topography on thin film disks, optical substrates or silicon wafers and whose output is independent of the reflectivity of the substrate. This material independent optical profilometer uses a retro-reflector to achieve reflectivity independence and to increase the height sensitivity to 8 times the height of the surface. The reflectivity independent optical profilometer achieves perfect cancellation of the slope of the surface while measuring the topography of the substrate.
Abstract:
Disclosed is a method for determining an overlay error between at least two layers in a multiple layer sample. An imaging optical system is used to measure a plurality of measured optical signals from a plurality of periodic targets on the sample. The targets each have a first structure in a first layer and a second structure in a second layer. There are predefined offsets between the first and second structures. A scatterometry overlay technique is then used to analyze the measured optical signals of the periodic targets and the predefined offsets of the first and second structures of the periodic targets to thereby determine an overlay error between the first and second structures of the periodic targets.