2020
DOI: 10.1017/s1431927620024721
|View full text |Cite
|
Sign up to set email alerts
|

Development of a Practicable Digital Pulse Read-Out for Dark-Field STEM

Abstract: Abstract

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
11
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
6
1

Relationship

3
4

Authors

Journals

citations
Cited by 20 publications
(14 citation statements)
references
References 49 publications
0
11
0
Order By: Relevance
“…A practical microscope in the lab does not have a continuum of options, so a fixed-size aperture with a probe semi-angle of 28 mrad was chosen. The pixel dwell time was taken as 40 μ s (Mullarkey et al, 2021), giving a total exposure time of ~8.35 s for each simulated image. Previously, Prismatic assumed a point source for electron emission at the gun, but in this work a source-size contribution was added.…”
Section: Methodsmentioning
confidence: 99%
“…A practical microscope in the lab does not have a continuum of options, so a fixed-size aperture with a probe semi-angle of 28 mrad was chosen. The pixel dwell time was taken as 40 μ s (Mullarkey et al, 2021), giving a total exposure time of ~8.35 s for each simulated image. Previously, Prismatic assumed a point source for electron emission at the gun, but in this work a source-size contribution was added.…”
Section: Methodsmentioning
confidence: 99%
“…where δ t is the pixel dwell-time, n p is the number of image pixels, n L is the number of scan lines, T LFB is the line flyback time, and T FFB is the frame flyback time. Equation (2) can be understood intuitively as the ratio of useful, information collecting time, to the total frame time (Mullarkey et al, 2020), and as η is always less than 1 we can see that equation (1) always underestimates the dose. Of the variables in this equation (δ t , n p , n L , T LFB , and T FFB ) generally only the first four out of five can be readily changed by the operator.…”
Section: Electron Dose and Scanning Efficiencymentioning
confidence: 99%
“…However, CS requires additional fast (and expensive) hardware to be introduced that may not be available to all microscopists (Béché et al, 2016; Kovarik et al, 2016). Moreover, where readout noise is not the limiting factor, such as with digital read-out approaches (Jones & Downing, 2018; Mullarkey et al, 2020), CS may not offer any appreciable benefit over conventional (Shannon) scanning (Sanders & Dwyer, 2018; Van den Broek et al, 2019).…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, the requirement for synchronizing electronics also limited this experiment to long pixel dwell times (typically tens of µs). More recently, SE image histograms have been investigated for counting SEs [2,10], motivated in part by similar work in scanning transmission electron microscopy (STEM) [11,12,13,14]. However, such techniques are limited by the same voltage signal variations that are present in conventional SE imaging.…”
Section: Introductionmentioning
confidence: 99%