The mean number of clusters per feature for <i>q</i> = 5 (left) and <i>q</i> = 7 (right) for different values of the agreement threshold <i>a</i>. by Pádraig MacCarron (8921690)

PEA performed for different durations of incubation after the dilution step, for three concentrations of rPCT. by Frederic Bedin (3402254)

“…<p>The incubation time after dilution of the binding product was progressively decreased from 5 min (reference test, ref.) down to 30 sec. …”

PEA performed for different durations of antigen/antibody binding, for three concentrations of rPCT. by Frederic Bedin (3402254)

“…<p>The time of incubation between the rPCT and the PEA probes was progressively decreased from 1h (reference test, ref.) down to 5 minutes. …”

Layer-Thickness-Dependent Strengthening–Toughening Mechanisms in Crystalline/Amorphous Nanolaminates by Xiaoling Zhou (4644826)

“…The mechanical performance of these materials is strongly governed by the crystalline–amorphous interfaces (CAIs), yet the underlying strengthening and toughening mechanisms remain poorly understood. Here, we employ large-scale molecular dynamics simulations to investigate the compressive deformation of C/A nanopillars composed of alternating equal-thickness crystalline Cu and amorphous Cu₅₀Zr₅₀ layers. …”

Layer-Thickness-Dependent Strengthening–Toughening Mechanisms in Crystalline/Amorphous Nanolaminates by Xiaoling Zhou (4644826)

“…The mechanical performance of these materials is strongly governed by the crystalline–amorphous interfaces (CAIs), yet the underlying strengthening and toughening mechanisms remain poorly understood. Here, we employ large-scale molecular dynamics simulations to investigate the compressive deformation of C/A nanopillars composed of alternating equal-thickness crystalline Cu and amorphous Cu₅₀Zr₅₀ layers. …”

Layer-Thickness-Dependent Strengthening–Toughening Mechanisms in Crystalline/Amorphous Nanolaminates by Xiaoling Zhou (4644826)

“…The mechanical performance of these materials is strongly governed by the crystalline–amorphous interfaces (CAIs), yet the underlying strengthening and toughening mechanisms remain poorly understood. Here, we employ large-scale molecular dynamics simulations to investigate the compressive deformation of C/A nanopillars composed of alternating equal-thickness crystalline Cu and amorphous Cu₅₀Zr₅₀ layers. …”

Layer-Thickness-Dependent Strengthening–Toughening Mechanisms in Crystalline/Amorphous Nanolaminates by Xiaoling Zhou (4644826)

“…The mechanical performance of these materials is strongly governed by the crystalline–amorphous interfaces (CAIs), yet the underlying strengthening and toughening mechanisms remain poorly understood. Here, we employ large-scale molecular dynamics simulations to investigate the compressive deformation of C/A nanopillars composed of alternating equal-thickness crystalline Cu and amorphous Cu₅₀Zr₅₀ layers. …”

Layer-Thickness-Dependent Strengthening–Toughening Mechanisms in Crystalline/Amorphous Nanolaminates by Xiaoling Zhou (4644826)

“…The mechanical performance of these materials is strongly governed by the crystalline–amorphous interfaces (CAIs), yet the underlying strengthening and toughening mechanisms remain poorly understood. Here, we employ large-scale molecular dynamics simulations to investigate the compressive deformation of C/A nanopillars composed of alternating equal-thickness crystalline Cu and amorphous Cu₅₀Zr₅₀ layers. …”

Layer-Thickness-Dependent Strengthening–Toughening Mechanisms in Crystalline/Amorphous Nanolaminates by Xiaoling Zhou (4644826)

“…The mechanical performance of these materials is strongly governed by the crystalline–amorphous interfaces (CAIs), yet the underlying strengthening and toughening mechanisms remain poorly understood. Here, we employ large-scale molecular dynamics simulations to investigate the compressive deformation of C/A nanopillars composed of alternating equal-thickness crystalline Cu and amorphous Cu₅₀Zr₅₀ layers. …”

Mechanical energy to create a burrow of 1 m length and 1.2 mm radius as a function of normalized water content using a penetration model and a fracture model. by Siul Ruiz (757454)

Growth and B12 uptake of <i>C. reinhardtii</i> metE7 in axenic cultures containing <i>7.5×10⁻¹⁴ mol</i>/<i>mL</i> B12 (i.e. <i>100 ng</i>/<i>L</i>). by Hannah Laeverenz Schlogelhofer (10834313)

PEA performed at different extension times and different enzyme inactivation times, for three concentrations of rPCT. by Frederic Bedin (3402254)

Decrease in parasite biomass and IRBC accumulation in organs in infected Rag2^−/− mice. by Carla Claser (185910)

Increased polymyxin B susceptibility in <i>bipA</i>-deleted strains at 20°C. by Eunsil Choi (8271039)

Flagella-mediated motility affected by <i>bipA</i> deletion in <i>S</i>. Typhimurium. by Eunsil Choi (8271039)

Elevated expression of <i>fimD</i> in <i>bipA</i>-deleted strains. by Eunsil Choi (8271039)

Image_1_Overexpression of a SDD1-Like Gene From Wild Tomato Decreases Stomatal Density and Enhances Dehydration Avoidance in Arabidopsis and Cultivated Tomato.PDF by Samuel Morales-Navarro (5481347)

Image_3_Overexpression of a SDD1-Like Gene From Wild Tomato Decreases Stomatal Density and Enhances Dehydration Avoidance in Arabidopsis and Cultivated Tomato.PDF by Samuel Morales-Navarro (5481347)

Image_2_Overexpression of a SDD1-Like Gene From Wild Tomato Decreases Stomatal Density and Enhances Dehydration Avoidance in Arabidopsis and Cultivated Tomato.PDF by Samuel Morales-Navarro (5481347)

Table_1_Overexpression of a SDD1-Like Gene From Wild Tomato Decreases Stomatal Density and Enhances Dehydration Avoidance in Arabidopsis and Cultivated Tomato.PDF by Samuel Morales-Navarro (5481347)