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Given a value of k, each sample was reconstructed and compared to the observed data.
The phylogeny of the sample was reconstructed using both neighbor-joining and maximum parsimony methods [ 31, 33].
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The XRD recorded from this sample were reconstructed.
A corresponding finite element mesh which precisely depicts the individual microstructure of each sample is reconstructed based on microscope images and computer tomographic (CT) scans.
When analytical pyrolysis is used, the chemical composition of the sample is reconstructed on the basis of an interpretation of the molecular profile of the thermal degradation products of the original components, and on the recognition of specific molecular markers or molecular patterns, which give characteristic fingerprints of the pyrolysed material.
After acquisition, projection images, 935 for the entire sample, were reconstructed (NRecon 1.4.4), and all the sections were cut along a longitudinal plane (CTAn 1.7).
Briefly, 1 million randomly sampled reads per sample were reconstructed into full-length 16S rRNA genes over 100 EMIRGE iterations, and after initial read mapping to a de-replicated version of the SILVA 108 16S rRNA database (http://www.arb-silva.de/).
The A-line depth profile of the sample is reconstructed by first measuring the spectral interference signal expressed by [ 4, 5]: In this expression, s(k) is the spectral intensity distribution of the light source.
The spiral k-space samples were reconstructed through a two-dimensional gridding reconstruction method (Jackson et al., 1991).
Application of periodic boundary conditions appears to be not critically important when reasonably large samples are reconstructed.
Finally, the source samples are reconstructed as (hat {x}'_{n}=hat {x}_{n}+epsilon '_{n}).
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CEO of Professional Science Editing for Scientists @ prosciediting.com