Abstract:
An imaging spectrometer is disclosed that comprises imaging means for dividing a received image into two or more spatially separated images and means for detecting each spectral image, and is characterised in that the imaging means comprises at least one polarizing beam splitter. The polarizing beam splitter may be a Wollaston prism. In one embodiment of the invention, the imaging means comprises image replication means to produce two or more spatially separated images, and one or more filter elements such as dichroic filters which act to alter the spectral characteristics of one or more of the spatially separated images. In a further embodiment of the invention the imaging means comprises one or more spectral replication means arranged in optical series, each spectral replication means comprising an optical retardation element and a polarising beam splitter.
Abstract:
Measurements at multiple distinct polarization measurement states are taken to define the polarization state of an input, for example to calculate a Stokes vector. High accuracy and/or capability of frequent recalibration are needed, due to the sensitivity of measurement to retardation of the input signal. A multiple measurement technique takes a set of spatially and/or temporally distinct intensity measurements through distinct waveplates and polarizers. These can be optimized as to orientation and retardation using initial choices and also using tunable elements, especially controllable birefringence elements. A device matrix defines the response of the device at each of the measurement states. The matrix can be corrected using an iterative technique to revise the device matrix, potentially by automated recalibration. Two input signals (or preferably the same signal before and after a polarization transform) that are known to have a common polarization attribute or other attribute relationship are measured and the common attribute and/or attribute relationship is derived for each and compared. The device matrix is revised, for example by iterative correction or by random search of candidates to improve the accuracy of the device matrix. Optional tunable spectral and temporal discrimination provide additional functions.
Abstract:
Disclosed are multi-element lenses which demonstrate reduced achromatic focal length and reduced electromagentic beam spot size dispersal effects in ellipsometer and polarimeter systems. Also disclosed is methodology for evaluating parameters in parameterized equations which enables calculating retardance entered to, or between, orthogonal components in a beam of electromagnetic radiation which is caused to pass through input and/or output optical elements and interact with a material system, by each of the input and output optical elements, substantially uncorrelated with retardation entered by the material system. Present invention input and/or output focusing lens(es) find application in spectroscopic ellipsometer mediated investigation of small spots on material systems, wherein a beam of electromagnetic radiation is caused to converge via an input lens, interact with a very small, chromatically undispersed spot area on a material system, then optionally re-collimate via an output lens, prior to entering a detector system. Present invention methodology provides benefit where it is necessary to separate out birefringent effects of input and/or output optical element focusing lens(es), optionally in combination with beam directing and/or window elements present in an ellipsometer system which are positioned with respect to input and/or output len(es) so as to be ellipsometrically indistinguishable therefrom, to arrive at material system characterizing ellipsometric PSI and DELTA results.
Abstract:
A spectroscopic ellipsometer having a multiwavelength light source, spectrometer (or wavelength-scanning monochromator and photodetector), a polarizer and polarization analyzer, and one or more objectives in the illumination and collection light paths, further comprises a stationary polarization modulator that modulates the light polarization versus wavelength. Modulator can be an optically active crystal rotating the linear polarization plane by a different angle for each wavelength or a non-achromatic waveplate retarder that varies the relative phase delay of the polarization components periodically over wavelength. The measured spectrum can be used to characterize selected features or parameters of a sample, e.g. by comparison with one or more theoretical spectra.
Abstract:
Two phase modulators or polarizing elements are employed to modulate the polarization of an interrogating radiation beam before and after the beam has been modified by a sample to be measured. Radiation so modulated and modified by the sample is detected and up to 25 harmonics may be derived from the detected signal. The up to 25 harmonics may be used to derive ellipsometric and system parameters, such as parameters related to the angles of fixed polarizing elements, circular deattenuation, depolarization of the polarizing elements and retardances of phase modulators. A portion of the radiation may be diverted for detecting sample tilt or a change in sample height. A cylindrical objective may be used for focusing the beam onto the sample to illuminate a circular spot on the sample. The above-described self-calibrating ellipsometer may be combined with another optical measurement instrument such as a polarimeter, a spectroreflectometer or another ellipsometer to improve the accuracy of measurement and/or to provide calibration standards for the optical measurement instrument. The self-calibrating ellipsometer as well as the combined system may be used for measuring sample characteristics such as film thickness and depolarization of radiation caused by the sample.
Abstract:
A method and apparatus for polarization measurements. A polarization state of an optical signal can be determined using a polarization analyzer comprising a polarization controller, a polarizer, a wavelength dispersive element and a photo-detector. The method and apparatus can be applied to polarization and polarization mode dispersion measurements in wavelength division multiplexed communication systems.
Abstract:
An apparatus incorporated within a spectroscopic imaging system, typically a microscope, but also applicable to other image gathering platforms, namely fiberscopes, macrolens imaging systems and telescopes employing a polarizing beam splitting element is disclosed. The apparatus allows simultaneous spectroscopic (i.e. chemical) imaging and rapid acquisition spectroscopy to be performed without the need for moving mechanical parts or time sequenced sampling and without introducing significant optical signal loss or degradation to the spectroscopic imaging capability. In addition, the apparatus affords a more compact design, an improved angular field of view and an improved overall ruggedness of optical design at a lower manufacturing and maintenance cost compared to previous devices.
Abstract:
A method for obtaining spectral radiation data for points in a field of view utilizes a broad band variable filter to produce different intensity distributions on a photocell array. The array is in the focal plane of a camera and photocell locations correspond to points in the field of view. The variable filter has a sequence of optical train elements comprised of a first linear polarizer, a body of optically active material, a retarder and a second linear polarizer. A series of radiance measurements are taken at each photocell of the array and at least one of the optical train components is repositioned between measurements. For each photocell, a collection of photocell values is stored in a computer memory and is converted to a system of linear equations. Intensities for spectral components of light incident thereon are derived for each photocell. The method can be used to create a two-dimensional intensity map for the pixel array for each wavelength measured. Also, the method can be used to create a broad band spectroradiometer for points in the field of view.
Abstract:
A Fourier-transform spectrometer contains a birefringent optical component, removing the need for a Michelson interferometer used in conventional instruments. A suitable birefringent element such as a Wollaston prism, is used to introduce a path difference between two light polarisations. Use of an extended light source so that all areas of the birefringent component are illuminated simultaneously ensures that different positions on the birefringent component correspond to different path differences between the two polarisations. A Fourier-transform of the resulting interferogram at the detector results in the spectral distribution of the input light being obtained. The use of an extended light source permits a Fourier-transform spectrometer with no moving parts to be achieved.
Abstract:
A spectrum measuring device for measuring optical spectrum of input light includes first and second double-image elements which separate input light to be measured into two polarized wave components having respective planes of polarization perpendicularly intersecting each other and having different optical axes, a third double-image element which separates the two polarized wave components from the first and second double-image elements into four polarized wave components each two of which having respective planes of polarization perpendicularly intersecting each other and having different optical axes, a dispersing element which is irradiated by the four polarized wave components from the third double-image element in which the dispersing element separates optical components of each wavelength contained in the four polarized wave components at the same angle of separation, and a photodetector for measuring an overall intensity of the four polarized wave components of the same wavelength separated by the dispersing element.