<i>E</i>. <i>faecium</i> protection in wild-type and mutant <i>C</i>. <i>elegans</i>. by Yu Sang (2551267)

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Dissipative Self-Assembly of Patchy Particles under Nonequilibrium Drive: A Computational Study by Shubhadeep Nag (18888287)

“…We also validated our key findings by simulating a larger system of 100 patchy particles. …”

Synthesis, Structure, and Physical Properties of <i>A</i>-site Ordered Perovskites <i>A</i>Cu₃Co₄O₁₂ (<i>A</i> = Ca and Y) by Ikuya Yamada (1406056)

“…Substitution of Ca with Y at the <i>A</i>-site changes the metallic CaCu₃Co₄O₁₂ to an insulating YCu₃Co₄O₁₂, and a metal−insulator transition occurs at <i>x</i> = 0.50−0.75. …”

TUG1 is not regulated by EC activation, induction of quiescence, oxidative stress or inflammation. by Anna Theresa Gimbel (13883632)

Inhibition of diverse influenza A virus in siRNA treated NHBE cells. by Michael A. Estrin (5236526)

“…Each combination was tested in triplicate and normalized to Allstars nontargeting siRNA. Relative mean viral growth is reported; 1.00 denotes no change relative to non-targeting siRNA, 0.50 denotes a 50% decrease in viral growth, and 0.00 denotes complete inhibition of viral growth.…”

Influence of T180A-SHIP2 on LEC functional responses. by Germaine D. Agollah (623510)

“…Scale bar  = 100 µm (<b>B</b>) and 50 µm (<b>C</b> and <b>D</b>) MW =  molecular weight marker.…”

Reproducibility of response time and brain measures. by Jan Willem Koten (17743224)

Erosivity by wind of sedimentary beds as a function of particle size. by Ferran Garcia-Pichel (257121)

“…The particle size dependence holds also for water erosion over sediments, and the values of the minimum range between 50 and 200 µm under a wide variety of conditions and sediment bulk densities <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0007801#pone.0007801-Lick1" target="_blank">[23]</a>.…”

Different Ignition Modes and Temperature Evolution of Typical Hypergolic Ionic Liquids by Lihan Fei (14142567)

“…It is found that the vapor delay time (VDT), explosion delay time (EDT), and ignition delay time (IDT) are all reduced with <i>U</i>₀ by at most 50%. For a given <i>U</i>₀, the three time scales decrease in the order [BMIm][DCA], [EMIm][DCA], and [EMIm][CDB] (IDT as low as 14.4 ms).…”