摘要:
The invention relates to a method of using a CMOS chip for direct charged particle counting. To avoid reset noise, it is known to use Correlative Double Sampling: for each signal value the pixel is sampled twice: once (204) directly after reset and once (206) after an integration time. The signal is then determined (208) by subtracting the reset value from the later acquired value, and the pixel is reset again (202). Typically the integration time is chosen sufficiently short that the chance that two particles impinge on one pixel is negligible, thereby enabling event counting. Although this technique removes reset noise and fixed pattern noise, it also lowers the image rate to half the frame rate, as a pixel needs to be sampled twice for one signal value. The invention proposes to reset the pixel only after a large number of read-outs. This is based on the insight that typically a large number of events, typically approximately 10, are needed to cause a full pixel. By either resetting after a large number of images, or when one pixel of the image shows a signal above a predetermined value (for example 0.8 x the full-well capacity), the image speed can be almost doubled when compared to the prior art method, using a reset after acquiring a signal.
摘要:
The invention relates to a method for analyzing an analogue signal (fig. 3, 400) comprising randomly spaced events (301, 302), the event having an event height, the method comprising: • 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 number of samples preceding the event and a number of samples following S(T), the method further comprising: • Using a model (412, fig. 5) to estimate a noise contribution N(t) for t = (T-Δ 1 ) to t = (T+Δ 2 ), the noise contribution derived from samples S(t) with t ≤ (T-Δ 1 ) and/or samples S(t) with t ≥ (T+Δ 2 ), with Δ 1 and Δ 2 predetermined or preset time periods, Δ 1 having a value such that the event has a negligible contribution to samples taken before (T-Δ 1 ) and Δ 2 having a value such that the event has a negligible contribution to samples taken after (T+Δ 2 ), • Estimating the event height E by integrating the series of samples from (T-Δ 1 ) to (T+Δ 2 ) minus the noise contribution for said samples, E = ∑ t = T − Δ 1 t = T + Δ 2 S t − ∑ t = T − Δ 1 t = T + Δ 2 N t = ∑ t = T − Δ 1 t = T + Δ 2 S t − N t . In an important aspect of the invention, the sampled signal is subjected to a sparsification operation that causes said event to be temporally compressed. 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. The invention further describes several methods to be used as a model.
摘要翻译:本发明涉及一种用于分析包含随机间隔事件(301,302)的模拟信号(图3,400)的方法,所述事件具有事件高度,所述方法包括:将信号转换为一系列样本S (t),t为采样时刻,从而形成采样的离散时间信号,¢检测事件的存在,t = T时检测到的事件,¢使用前面的多个样本估计事件高度 事件和S(T)之后的多个样本,该方法还包括:使用模型(412,图5)估计t =(T-1)到t =的噪声贡献N(t) (T +“2),从t‰(T - 1)和/或样本S(t)得到的样本S(t)的噪声贡献与t‰(T +”2),“1和”2 预定或预设的时间段,“1具有使得事件对(T-1)之前采取的样本的贡献可忽略不计的值,并且”2具有使得事件具有可忽略的公理 对(T +“2)之后采样的样本的贡献,¢通过将来自(T-1)到(T + 2)的一系列样本减去所述样本的噪声贡献来估计事件高度E,E ='t = T'“1 t = T +”2 S t“t = T'”1 t = T +“2 N t ='t = T'”1 t = T + t'N t。 在本发明的一个重要方面,采样信号经受使所述事件被时间压缩的稀疏化操作。 该方法对于SEM中使用的X射线检测器,例如硅漂移探测器特别有用。 通过估计对信号的噪声贡献,以提高的精度估计台阶高度。 本发明还描述了用作模型的几种方法。
摘要:
The invention relates to a method for analyzing an analogue signal (fig. 3, 400) comprising randomly spaced events (301, 302), the event having an event height, the method comprising: • 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 number of samples preceding the event and a number of samples following S(T), Characterized in that the method further comprises • Using a model (412, fig. 5) to estimate a noise contribution N(t) for t = (T-Δ 1 ) to t = (T+Δ 2 ), the noise contribution derived from samples S(t) with t ≤ (T-Δ 1 ) and/or samples S(t) with t ≥ (T+Δ 2 ), witch Δ 1 and Δ 2 predetermined or preset time periods, Δ 1 having a value such that the event has a negligible contribution to samples taken before (T-Δ 1 ) and Δ 2 having a value such that the event has a negligible contribution to samples taken after (T+Δ 2 ), • Estimating the event height E by integrating the series of samples from (T-Δ 1 ) to (T+Δ 2 ) minus the noise contribution for said samples, E = ∑ t = T - Δ 1 t = T + Δ 2 S t - ∑ t = T - Δ 1 t = T + Δ 2 N t = ∑ t = T - Δ 1 t = T + Δ 2 S t - N t . 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. The invention further describes several methods to be used as a model.
摘要翻译:本发明涉及一种用于分析包含随机间隔事件(301,302)的模拟信号(图3,400)的方法,所述事件具有事件高度,所述方法包括:将信号转换为一系列样本S (t),t为采样时刻,从而形成采样的离散时间信号,¢检测事件的存在,t = T时检测到的事件,¢使用前面的多个样本估计事件高度 事件和S(T)之后的多个样本,其特征在于该方法还包括使用模型(412,图5)估计t =(T-1)至 t =(T +“2),样本S(t)与t‰(T-”1)和/或样本S(t)t +(T +“2)的噪声贡献, “2个预定或预设时间段”1具有使得该事件对(T-1)之前采取的采样具有可忽略的贡献的值,并且“2具有使得偶数 对(T +“2)之后采样的样本贡献可以忽略不计,通过将来自(T-1)到(T + 2)的一系列样本减去所述样本的噪声贡献来估计事件高度E,E = t = T - “1 t = T +”2 S t - 't = T - “1 t = T +”2 N t ='t = T - “1 t = T + t - N t。 该方法对于SEM中使用的X射线检测器,例如硅漂移探测器特别有用。 通过估计对信号的噪声贡献,以提高的精度估计台阶高度。 本发明还描述了用作模型的几种方法。
摘要:
The invention relates to a method of preparing and imaging a sample (101) using a particle-optical apparatus ( 100 ), equipped with an electron column (120) and an ion beam column (140), a camera system (110), a manipulator (160) the method comprising the steps of Deriving a first ptychographic image of the sample from a first electron image, then thinning the sample, and forming a second ptychographic image of the sample. In an embodiments of the invention the seed image used for the second image is the first ptychografic image. In another embodiment the second ptychographic image is the image of the layer removed during the thinning, In yet another embodiment the inner potential of the sample is determined and dopant concentrations are determined.
摘要:
The invention relates to a method of using a CMOS chip for direct charged particle counting. To avoid reset noise, it is known to use Correlative Double Sampling: for each signal value the pixel is sampled twice: once (204) directly after reset and once (206) after an integration time. The signal is then determined (208) by subtracting the reset value from the later acquired value, and the pixel is reset again (202). Typically the integration time is chosen sufficiently short that the chance that two particles impinge on one pixel is negligible, thereby enabling event counting. Although this technique removes reset noise and fixed pattern noise, it also lowers the image rate to half the frame rate, as a pixel needs to be sampled twice for one signal value. The invention proposes to reset the pixel only after a large number of read-outs. This is based on the insight that typically a large number of events, typically approximately 10, are needed to cause a full pixel. By either resetting after a large number of images, or when one pixel of the image shows a signal above a predetermined value (for example 0.8 x the full-well capacity), the image speed can be almost doubled when compared to the prior art method, using a reset after acquiring a signal.
摘要:
Electron beam modulation in response to optical pump pulses applied to a sample is measured using SPAD elements. Individual detection events are used to form histograms of numbers of events in time bins associated with pump pulse timing. The histograms can be produced at a SPAD array, simplifying data transfer. In some examples, two SPAD arrays are stacked and a coincidence circuit discriminates signal events from noise events by determining corresponding events are detected withing a predetermined time window.
摘要:
When detecting particulate radiation, such as electrons, with a pixelated detector, a cloud of electron/hole pairs is formed in the detector. Using the signal caused by this cloud of electron/hole pairs a position of the impact is estimated. Inventors found that, when the size of the cloud is comparable to the pixel size, or much smaller, the estimated position shows a strong bias to the center of the pixel and the corners, as well to the middle of the borders. This hinders forming an image with super-resolution. By shifting the position or by attributing the electron to several sub-pixels this bias can be countered, resulting in a more truthful representation. Inventors further found that by spreading the image Moiré-effects and interferences in the image can be countered. As long as the image is a sparse image (almost all pixels representing one or no impact) this spreading is a reversible process. After spreading (effectively a spatial low-pass filtering) a high-pass filtering may be used to crisp the image. It is noted that shifting and/or spreading the information over several image pixels should take place before adding the events per image pixel. When said spreading is done after combining detector images, information is lost. It is noted that shifting cannot take place after combining detector images.
摘要:
When detecting particulate radiation, such as electrons, with a pixelated detector, a cloud of electron/hole pairs is formed in the detector. Using the signal caused by this cloud of electron/hole pairs a position of the impact is estimated. Inventors found that, when the size of the cloud is comparable to the pixel size, or much smaller, the estimated position shows a strong bias to the center of the pixel and the corners, as well to the middle of the borders. This hinders forming an image with super-resolution. By shifting the position or by attributing the electron to several sub-pixels this bias can be countered, resulting in a more truthful representation. Inventors further found that by spreading the image Moiré-effects and interferences in the image can be countered. As long as the image is a sparse image (almost all pixels representing one or no impact) this spreading is a reversible process. After spreading (effectively a spatial low-pass filtering) a high-pass filtering may be used to crisp the image. It is noted that shifting and/or spreading the information over several image pixels should take place before adding the events per image pixel. When said spreading is done after combining detector images, information is lost. It is noted that shifting cannot take place after combining detector images.
摘要:
Disclosed herein are methods, apparatuses, systems, and computer-readable media related to defective pixel management in charged particle microscopy. For example, in some embodiments, a charged particle microscope support apparatus may: identify a working pixel region of a charged particle camera, wherein the working pixel region is proximate to a defective pixel region in which the charged particle camera cannot detect charged particle events; generate a set of charged particle event indicators that represent a charged particle event in the working pixel region; adjust the set of charged particle event indicators so that a charged particle event intensity over the working pixel region is not significantly greater than a charged particle event intensity over the defective pixel region; and output charged particle event data, wherein the charged particle event data includes data representative of the adjusted set of charged particle event indicators.
摘要:
Electron beam modulation in response to optical pump pulses applied to a sample is measured using SPAD elements. Individual detection events are used to form histograms of numbers of events in time bins associated with pump pulse timing. The histograms can be produced at a SPAD array, simplifying data transfer. In some examples, two SPAD arrays are stacked and a coincidence circuit discriminates signal events from noise events by determining corresponding events are detected withing a predetermined time window.