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Probe angle reflects underlying cTnC orientation.
Changes in probe angle were found at [Ca2+] well below those required to generate tension.
Fluorescence polarization, giving probe angle and its dispersion relative to the fiber long axis, was monitored simultaneously with isometric tension.
The time course of the probe angle change and tension after photolytic release [Ca2+] by laser photolysis of NP-EGTA was Ca2+ sensitive and biphasic: a rapid component ∼10 times faster than that of tension and a slower rate similar to that of tension.
Figure 7 Energy influx versus probe angle to the ion beam axis.
Lateral resolution increases linearly with increasing probe angle; however, depth resolution increases quadratically.
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A number of factors affect digitizing accuracy, such as the travel speed of the probe, pitch values, probe angles (part orientations), probe sizes, and feature sizes.
For the larger probe angles, the two dopant atoms can be easily located at 2- and 8-nm depth.
The probe convergence angle and the inner/outer detector angles for high-angle annular dark-field (HAADF) imaging were 10 and 88 234 mrad, respectively.
The probe convergence angle and the inner/outer detector angles for HAADF and annular bright-field (ABF) imaging were 22, 90 370 and 11 22 mrad, respectively.
Figure 4f shows that when f is small, PRISM will slightly over-estimate the image intensity at scattering angles below the probe semi-angle, and slightly under-estimates the intensity at higher scattering angles.
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