Abstract:
A user interface for operation of a scanning electron microscope device that combines lower magnification reference images and higher magnification images on the same screen to make it easier for a user who is not used to the high magnification of electron microscopes to readily determine where on the sample an image is being obtained and to understand the relationship between that image and the rest of the sample. Additionally, other screens, such as, for example, an archive screen and a settings screen allow the user to compare saved images and adjust the settings of the system, respectively.
Abstract:
A spectroscopic analysis method, comprising: Directing a beam of radiation onto a location P on a specimen, thereby causing a flux of X-rays to emanate from said location; Examining said flux using a detector arrangement, thus accruing a measured spectrum; Choosing a set of mutually different measurement directions d={dn} that originate from P, where n is a member of an integer sequence; Recording an output On of said detector arrangement for different values of dn, thus compiling a measurement set M={(On, dn)}; Adopting a spectral model On′ for On that is a convoluted mix of terms Band Lp, where: B is a substantially continuous spectral component associated with Bremsstrahlung; Lp is a substantially discrete spectral component associated with the specimen composition at location P; automatically deconvolving the measurement set Mon the basis of said spectral model On′ and distill Lp therefrom.
Abstract:
A method of accumulating an image of a specimen using a scanning-type microscope, comprising the following steps: Providing a beam of radiation that is directed from a source through an illuminator so as to irradiate the specimen; Providing a detector for detecting a flux of radiation emanating from the specimen in response to said irradiation; Causing said beam to undergo scanning motion relative to a surface of the specimen, and recording an output of the detector as a function of scan position, which method additionally comprises the following steps: In a first sampling session S1gathering detector data from a first collection P1 of sampling points distributed sparsely across the specimen; Repeating this procedure so as to accumulate a set {Pn} of such collections, gathered during an associated set {Sn} of sampling sessions, each set with a cardinality N>1; Assembling an image of the specimen by using the set {Pn} as input to an integrative mathematical reconstruction procedure, wherein, as part of said assembly process, a mathematical registration correction is made to compensate for drift mismatches between different members of the set {Pn}.
Abstract:
An improved method of directing a charged particle beam that compensates for the time required for the charged particles to traverse the system by altering one or more of the deflector signals. According to one embodiment of the invention, a digital filter is applied to the scan pattern prior to digital-to-analog (D/A) conversion in order to reduce or eliminate over-shoot effects that can result from TOF errors. In other embodiments, analog filters or the use of signal amplifiers with a lower bandwidth can also be used to compensate for TOF errors. By altering the scan pattern, over-shoot effects can be significantly reduced or eliminated.
Abstract:
A method and apparatus for imaging a specimen using a scanning-type microscope, by irradiating a specimen with a beam of radiation using a scanning motion, and detecting a flux of radiation emanating from the specimen in response to the irradiation, in the first sampling session {S1} of a set {Sn}, gathering data from a first collection of sparsely distributed sampling points {P1} of set {Pn}. A mathematical registration correction is made to compensate for drift mismatches between different members of the set {Pn}, and an image of the specimen is assembled using the set {Pn} as input to an integrative mathematical reconstruction procedure.
Abstract:
Methods and systems are provided for a scanning microscope to rapidly form a partial digital image of an area. The method includes performing an initial scan for the area and using initial scan to identify regions representing features of interest in the area. Then, the method performs additional adaptive scans of the regions representing structures of interest. Such scans adapt the path of the scanning beam to follow the edges of a feature of interest by performing localized scan patterns that intersect the feature edge, and directing the localized scan patterns to follow the feature edge.
Abstract:
A system for analyzing an analogue signal comprising randomly spaced events, the event having an event height, comprises: Converting the signal to a series of samples S(t), with t the moment of sampling, thereby forming a sampled, discrete time signal, Detecting the presence of an event, the event detected at t=T, Estimating the event height, Using a model (412, FIG. 5) to estimate a noise contribution N(t) for t=(T−Δ1) to t=(T+Δ2), the noise contribution derived from samples S(t) with t≦(T−Δ1) and/or samples S(t) with t≧(T+Δ2), with Δ1 and Δ2 predetermined or preset time periods having a value such that the event has a negligible contribution to samples taken before (T−Δ1) or after (T+Δ2), Estimating the event height E by integrating the series of samples from (T−Δ1) to (T+Δ2) minus the noise contribution for said samples, E=Σt=(T−Δ1)t=(T+Δ2)S(t)−Σt=(T−Δ1)t=(T+Δ2)N(t)=Σt=(T−Δ1)t=(T+Δ2)[S(t)−N(t)].
Abstract:
The method relates to a method of scanning a sample. Scanning a sample is typically done by scanning the sample with a probe along a multitude of parallel lines. In prior art scan methods a sample is scanned multiple times with a nominally identical scan pattern. The invention is based on the insight that the coherence between adjacent points in a direction along the scan direction is much better than the coherence of adjacent points perpendicular to the scan direction. By combining two images that are scanned perpendicular to each other, it should thus be possible to form an image making use of the improved coherence (due to shorter temporal distance) in both directions. The method thus involves scanning the sample with two scan patterns, the lines of one scan pattern preferably perpendicular to the lines of the other scan pattern. Hereby it is possible to use the temporal coherence of scan points on a line of one scan pattern to align the lines of the other scan pattern, and vice versa.
Abstract:
The invention relates to a method for analyzing an analogue signal comprising randomly spaced events having an event height. The method includes irradiating a sample with a focused beam of energetic electrons, detecting emission from the sample in response to such irradiation, and converting an analog signal of the emissions to a stationary time signal. The method further includes determining an estimated noise contribution for the stationary time signal, and determining an estimated event height of an event based on the stationary time signal and the estimated noise contribution for the stationary time signal, and determining, based on the estimated event height, an energy of the emission detected by the detector. This method is particularly useful for X-ray detectors, such as Silicon Drift Detectors, used in a SEM. By estimating the noise contribution to the signal, the step height is estimated with improved accuracy.
Abstract:
The invention relates to a method for analyzing the output signal of a silicon drift detector (SDD). A SDD is used for detecting X-rays emitted by a sample as a result of impinging radiation.The signal of a SDD comprises a number of randomly spaced steps, in which the step height is a function of the energy of the detected X-ray photon.The variance in step height is a function of the averaging time that can be used to determine the plateau between steps: averaging over a short interval results in more uncertainty of the plateau value than a long interval. By according a weight factor, a function of the variance such that a step with low variance (high reliability) is associated with a larger weight factor than a step with high variance (low reliability), measurement values with a low variance are emphasized. This results in better resolved spectra.