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Optional stages for micropositioning and material testing allow scanning of a sample under a variety of conditions.
Lateral scanning of a sample with an x-y translation stage (T-LS28M, Zaber Inc., Canada) allowed for a 28 mm scanning range in two directions.
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Figure 2 CT scan of a sample component.
Right: Computer tomography scan of a sample section, visualization by Fraunhofer ITWM, Department Image Processing.
Applying this correction to 2 scans of a sample generates 4 Ci point measurements that are then averaged, assuming the transformation appears reversible, to a reported value of Tc and standard measurement error.
At a press briefing here today, mission manager Jun'ichiro Kawaguchi explained that two micron-sized particles have been spotted during a microscope scan of a sample tray and 10 or more additional particles can be seen on the inside surfaces of the sample container (inset).
Four to six scans of a sample containing only buffer were averaged and subtracted from the averaged data for each protein sample to remove the Pd Kβ fluorescence and produce a flat pre-edge baseline.
Four to six scans of a sample containing only buffer were averaged and subtracted from the averaged data for each protein sample to remove the Ni Kβ fluorescence and produce a flat pre-edge baseline.
Figure 2 XRD 2 theta-scanning of (a) samples A, B, and C; (b) sample D; (c) sample E. Finally, to evaluate these two strategies in terms of peak absorption wavelength, samples were fabricated into 200 × 200 μmesaesandnd then measured by the photocurrent spectrums which were performed by a Fourier transform infrared spectrometer with multi-pass configuration.
In this work, the experimental behavior observed in the z-scan curves of a sample of bleached photographic film for different incident powers is theoretically modeled.
These spectra are obtained by determining the scan profile of a sample in basic solution and zeroing the same sample in an acidic or neutral solution [ 2, 39].
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