Abstract:
PROBLEM TO BE SOLVED: To provide a system which relates to a non-destructive technology for measuring a surface parameter of a sample for measuring the birefringence of a surface, a film thickness, etc. using a polarimetric spectrum. SOLUTION: A polarized sample beam 46 of broadband radiation is focused to the surface of a sample 3 and the radiation polarized by the sample is collected by a mirror system in different planes of incidence. The modulated radiation is analyzed with respect to a polarization plane to provide a polarimetric spectrum. Thickness and refractive information may then be derived from the spectrum. The polarization of the sample beam is altered by the focusing and the sample, and the collection of the modulated radiation is repeated employing two different apertures 28 to detect the presence or absence of a birefringence axis in the sample. In the other preferred embodiment, the technology may be combined with ellipsometry for determining the thicknesses and refractive indices of thin films. COPYRIGHT: (C)2011,JPO&INPIT
Abstract:
The present invention relates to in-situ techniques for determining process end points in semiconductor wafer polishing processes. Generally, the technique involves utilizing a scanning inspection machine having multiple pair of lasers and sensors located at different angles for detecting signals caused to emanate from an inspected specimen. The detection techniques determine the end points by differentiating between various material properties within a wafer. An accompanying algorithm is used to obtain an end point detection curve (608) that represents a composite representation of the signals obtained from each of the detectors of the inspection machine. This end point detection curve (608) is then used to determine the process end point (614). Note that computation of the algorithm (610, 612) is performed during the polishing process so that the process end point can be determined without interruptions that diminish process throughputs.
Abstract:
Thickness of a film in a sample may be detected by directing pump laser pulses to the surface of a sample to generate an acoustic pulse in a sample. The acoustic pulse propagates downwards until it reaches an interface between the bottom of the film and a substrate and is reflected back to the top surface of the film as a first echo. A reflection of the first echo propagates downwards and is again reflected back towards the surface as a second echo. Interferometry is used to measure the lapse of time between the first and second echos from which the thickness of the film may be determined.
Abstract:
Thickness of a film in a sample may be detected by directing pump laser pulses to the surface of a sample to generate an acoustic pulse in a sample. The acoustic pulse propagates downwards until it reaches an interface between the bottom of the film and a substrate and is reflected back to the top surface of the film as a first echo. A reflection of the first echo propagates downwards and is again reflected back towards the surface as a second echo. Interferometry is used to measure the lapse of time between the first and second echos from which the thickness of the film may be determined.
Abstract:
Disclosed is a self-clearing objective (100) for directing a beam towards a sample and clearing away debris from an optical viewing path adjacent to the sample. The self-clearing objective includes an optical element (106, 210, 310, 408, 510) and a substantially transparent fluid (104, 213, 326, 512) flowing between the optical element and the sample such that at least a portion adjacent to the sample is substantially cleared of debris. The optical element and the fluid cooperatively direct the beam towards the sample. This self-clearing objective may be coupled with various measurement devices to measure various characteristics of samples having debris that prevents clear optical measurements. Additionally, the measurement device may be integrated with or coupled to various sample processing systems so that the relevant process may be clearly monitored.
Abstract:
A polarized sample beam (12) of broadband radiation is focused onto the surface of a sample (3) and the radiation modified by the sample is collected by means of a mirror system (16) in different planes of incidence. The sample beam focused to the sample has a multitude of polarization states. The modified radiation is analyzed with respect to a polarization plane to provide a polarimetric spectrum. Preferably the polarization of the sample beam is altered only by the focusing and the sample, and the analyzing is done with respect to a fixed polarization plane. In the preferred embodiment, the focusing of the sample beam and the collection of the modified radiation are repeated employing two different apertures (30) to detect the presence or absence of a birefringence axis in the sample. In another preferred embodiment, the above-described technique may be combined with ellipsometry for determining the thickness and refractive indices of thin films.