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 poly chromatic 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:
This invention concerns an ellipsometer for the examination of a sample (50) whereby the ellipsometer has a broadband light source (1) on the emitter side (A) and a detector (8) on the receiver side (B) for a receiver light beam reflected (3B) from the sample (50). A refractive optic for the generation of a measuring spot on the sample and a first aperture (2) arranged on the emitter side (A) for the definition of a measuring spot on the sample. nullsicnull Using the spectroscopic ellipsometer makes it possible to easily produce a precisely defined measuring spot on the sample (50).
Abstract:
A pollen sensor and method for detecting pollen which discriminates pollen particles floating in air from other particles on a real time basis. The pollen sensor includes an illumination position for generating a light beam, a first receiver for measuring the intensity (I) or (Ip) of a light beam scattered by floating particles in a detection zone, a second receiver for measuring the intensity (Is) of a polarized light beam in a direction perpendicular to light illuminated by the light beam and means for measuring the degree of polarization of the particles for distinguishing pollen particles from other particles.
Abstract:
An ellipsometer, and a method of ellipsometry, for analyzing a sample using a broad range of wavelengths, includes a light source for generating a beam of polychromatic light having a range of wavelengths of light for interacting with the sample. A polarizer polarizes the light beam before the light beam interacts with the sample. A rotating compensator induces phase retardations of a polarization state of the light beam wherein the range of wavelengths and the compensator are selected such that at least a first phase retardation value is induced that is within a primary range of effective retardations of substantially 135null to 225null, and at least a second phase retardation value is induced that is outside of the primary range. An analyzer interacts with the light beam after the light beam interacts with the sample. A detector measures the intensity of light after interacting with the analyzer as a function of compensator angle and of wavelength, preferably at all wavelengths simultaneously. A processor determines the polarization state of the beam as it impinges the analyzer from the light intensities measured by the detector.
Abstract:
Achromatic optics may be employed in spectroscopic measurement systems. The achromatic optics comprises a spherical mirror receiving a beam of radiation in a direction away from its axis and a pair of lenses: a positive lens and a negative meniscus lens. The negative meniscus lens corrects for the spherical aberration caused by off-axis reflection from the spherical mirror. The positive lens compensates for the achromatic aberration introduced by the negative lens so that the optics, as a whole, is achromatic over visible and ultraviolet wavelengths. Preferably, the two lenses combined have zero power or close to zero power. By employing a spherical mirror, it is unnecessary to employ ellipsoidal or paraboloidal mirrors with artifacts of diamond turning which limit the size of the spot of the sample that can be measured in ellipsometry, reflectometry or scatterometry.
Abstract:
A birefringence measurement apparatus for calculating information of polarization of light emitted from an object to be measured includes a light source, a first polarization element for extracting a beam in a specific polarization direction from light emitted from the light source, a sample stage that holds an object to be measured, at least one beam splitting unit that splits the light emitted from the object into two beams having the same polarization as that of the light emitted from the object, at least two second polarization elements for extracting beams in a specific polarization direction of the light split by the beam splitting unit, at least two light-quantity detectors for detecting light quantity of beams that have transmitted through the second polarization element, and an operation part for operating a light quantity received by the light-quantity detectors.
Abstract:
A device for the photoelectric measurement of a measured object constructed especially as densitometer or color measurement device includes a light source (1, 2) for exposure of the measured object (6) to measurement light, a polarization filter (8) located between the light source (1, 2) and the measured object (6), a photoelectric sensor (4), a second polarization filter (9) located between the measured object (6) and the sensor (4), a measurement lens (3), which directs the measurement light originating from a measurement location from the measurement object (6) through the second polarization filter (9) onto the sensor (4), and a control electronic (5) cooperating with the sensor (4) for the processing of the electrical signals produced thereby. At least one of the two polarization filters (9) is electronically controllable, whereby its polarization plane can be rotated by the controlled electronic (5) by 90null relative to that the other of the two polarization filters. The polarization filter(s) is (are) thereby constructed according to liquid crystal technology and preferably consist of several layers in order to reliably suppress light portions which are not located in the polarization plane. The rotation of the polarization plane and thereby the activation or deactivation of the shine suppression can be easily and quickly achieved purely electronically due to the electronically controllable construction of the polarization filter and by the application of suitable electrical signals.
Abstract:
Method and apparatus for determining scattering parameters of a scattering matrix of an optical device. A method according to the present invention comprises applying an optical stimulus to a plurality of ports of the optical device, measuring optical fields emerging from the plurality of ports in amplitude and phase, and calculating the scattering parameters using the measured optical fields. The applying step includes applying the optical stimulus to the plurality of ports simultaneously. The method ensures a consistent phase reference for measurement of all of the scattering parameters so that all measurable characteristics of the device can be calculated directly from the scattering parameters.
Abstract:
A solid immersion tunneling ellipsometer and methods relating thereto may include a solid immersion apparatus (e.g., a prism or an objective lens in combination with a solid immersion lens) that facilitates optical tunneling and provide information that can be used in the determination of one or more characteristics (e.g., thickness, index of refraction, etc.) of samples (e.g., thin films, ultrathin films, etc.).
Abstract:
A birefringence measurement apparatus includes a measurement part for measuring a birefringence azimuth and a birefringence amount of an object to first and second light having different wavelengths from each other, and a determination part for calculating at least one of a birefringence azimuth and a birefringence amount to third light different in wavelength from the first and second light based on the birefringence azimuth and birefringence amount of the object to the first and second light.