Time course thyroid phenotype progression by genotype. by Wendy J. Bailey (14926392)

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Representative average structure of MD simulation trajectories during production run for WT and mutant mouse TG models. by Wendy J. Bailey (14926392)

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Antihypertensive treatment of 151 T2DM patients with hypertension at different subgroups. by Ningning Wang (560944)

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OPG147 contributes to VACV evasion of host defense and is a virulence factor <i>in vivo.</i> by Xue-Mei Yi (18851202)

Relationship between <i>D</i> on <i>I</i>_s at different weathering levels (R²: 0.82, 0.89, 0.93 for highly, moderately, and slightly). by Hong Zhang (25820)

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Relationship between <i>I</i>_s and <i>β</i> at different weathering levels (R²: 0.88, 0.83, 0.91 for highly, moderately, and slightly). by Hong Zhang (25820)

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Dual-species biofilms of <i>S</i>. <i>mutans</i> and <i>C</i>. <i>albicans</i> on the dentin surface after pH cycling study showing sparse biofilm development on SDF exposed dentin... by Suphanida Kaewkamchai (19762172)

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Dose-dependent reduction of lactate formation by Jurkat cells. by Samo Lešnik (21073880)

Distribution of groups of municipalities formed by municipalities with similar fertility rate of women aged 15 to 19 years in the pre-pandemic period (on the left) and in the pande... by Rosa Maria Soares Madeira Domingues (2795005)

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Distribution of groups of municipalities formed by municipalities with similar fertility rate of women aged 10 to 14 years in the pre-pandemic period (on the left) and in the pande... by Rosa Maria Soares Madeira Domingues (2795005)

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SEM Samples of FSW Joints: (i) ABS (800 rpm,10 mm/min) [(a) Cross-sectional View, (b) 250X, (c)1000X} (ii) ABS (1200 rpm,10 mm/min) [(d) Cross-sectional View, (e) 250X, (f)1000X} (... by Shaheer Ahmed Khan (17797647)

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Co-infected cells express both KSHV and EBV genes <i>in vitro</i> necessary for their survival and growth. by Mitchell Hayes (5334887)

PP1/PP2A does not dephosphorylate pS295 <i>in vitro</i>. by Takahiko Chimura (729098)

“…<p>(A) Western-blot analysis showing that PP1/PP2A was active in our <i>in-vitro</i> dephosphorylation assay. …”

Effect of the smoking factor on lung function parameters (FVC, FEV1, PEF, FEF 25_75). by Prasanna Herath (20714794)

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Analysis of Significantly Different ARGs and Resistance Mechanisms. by Xu Jia (187142)

Dynamics of Solid–Liquid Compound Droplets on Cylindrically Concave Superhydrophobic Surfaces by Niju K. Mohammed (22631779)

“…The droplet extension on a concave surface follows the relation <i>D</i>_<i>z</i>^max/<i>D</i>₀ ≈ <i>f</i>(<i>We</i>, δ, Bo), and for a flat plate, when δ → 0, the correlation reduces to the established scaling law <i>D</i>_<i>z</i>^max/<i>D</i>₀ ≈ <i>We</i>^1/4. …”

Dynamics of Solid–Liquid Compound Droplets on Cylindrically Concave Superhydrophobic Surfaces by Niju K. Mohammed (22631779)

“…The droplet extension on a concave surface follows the relation <i>D</i>_<i>z</i>^max/<i>D</i>₀ ≈ <i>f</i>(<i>We</i>, δ, Bo), and for a flat plate, when δ → 0, the correlation reduces to the established scaling law <i>D</i>_<i>z</i>^max/<i>D</i>₀ ≈ <i>We</i>^1/4. …”

Dynamics of Solid–Liquid Compound Droplets on Cylindrically Concave Superhydrophobic Surfaces by Niju K. Mohammed (22631779)

“…The droplet extension on a concave surface follows the relation <i>D</i>_<i>z</i>^max/<i>D</i>₀ ≈ <i>f</i>(<i>We</i>, δ, Bo), and for a flat plate, when δ → 0, the correlation reduces to the established scaling law <i>D</i>_<i>z</i>^max/<i>D</i>₀ ≈ <i>We</i>^1/4. …”

Dynamics of Solid–Liquid Compound Droplets on Cylindrically Concave Superhydrophobic Surfaces by Niju K. Mohammed (22631779)

“…The droplet extension on a concave surface follows the relation <i>D</i>_<i>z</i>^max/<i>D</i>₀ ≈ <i>f</i>(<i>We</i>, δ, Bo), and for a flat plate, when δ → 0, the correlation reduces to the established scaling law <i>D</i>_<i>z</i>^max/<i>D</i>₀ ≈ <i>We</i>^1/4. …”

Dynamics of Solid–Liquid Compound Droplets on Cylindrically Concave Superhydrophobic Surfaces by Niju K. Mohammed (22631779)

“…The droplet extension on a concave surface follows the relation <i>D</i>_<i>z</i>^max/<i>D</i>₀ ≈ <i>f</i>(<i>We</i>, δ, Bo), and for a flat plate, when δ → 0, the correlation reduces to the established scaling law <i>D</i>_<i>z</i>^max/<i>D</i>₀ ≈ <i>We</i>^1/4. …”