Showing 1,921 - 1,940 results of 7,331 for search 'significantly ((((we decrease) OR (linear decrease))) OR (larger decrease))', query time: 0.50s Refine Results
  1. 1921

    Study selection flow diagram. by Laurence Weinberg (2960238)

    Published 2025
    “…</p><p>Results</p><p>From the initial 1826 articles identified, we included 28 studies from eight countries in a total of 6411 nonagenarians. …”
  2. 1922

    Inclusion and exclusion criteria. by Laurence Weinberg (2960238)

    Published 2025
    “…</p><p>Results</p><p>From the initial 1826 articles identified, we included 28 studies from eight countries in a total of 6411 nonagenarians. …”
  3. 1923

    Key characteristics of the included publications. by Laurence Weinberg (2960238)

    Published 2025
    “…</p><p>Results</p><p>From the initial 1826 articles identified, we included 28 studies from eight countries in a total of 6411 nonagenarians. …”
  4. 1924

    Weight and plasma biochemistry. by Søren Egstrand (10906087)

    Published 2025
    “…In the present study, we found significant diurnal rhythmicity of <i>Casr</i>, encoding the Cinacalcet drug target in hyperplastic parathyroid glands (p = 0.006). …”
  5. 1925

    Baseline clinical data. by Lu-Jin Cheng (21743350)

    Published 2025
    “…In vitro experiments showed that the addition of Gal-9 led to a significant increase in the proportion of TIM-3<sup>+</sup>M1 and TIM-3<sup>+</sup>M2 macrophages and a decrease in M1 cell proportions and M1/M2 ratio. …”
  6. 1926

    Tailoring Ionic Conductivity of Polymeric Ionic Liquid Block Copolymers through Morphology Control by Samuel K. J. Adotey (22425591)

    Published 2025
    “…We further show that transport-blocking defects are largely absent from PIL-rich morphologies having nonionic cylindrical or spherical domains embedded in a PIL matrix. …”
  7. 1927

    Alkenyl/Thiol Co-Functionalized Titanium-Oxo Nanoclusters Enable Synergistic Lithography for Enhanced Resolution and Sensitivity by Zuohu Zhou (14258773)

    Published 2025
    “…Such dual cross-linkable group functionalization brought additional thiol–ene click reactions upon exposure to enhance intercluster polymerization, which significantly improved the lithography sensitivity of TOCs, with the required exposure energy being reduced by over 70% (decreasing from >1000 μC/cm<sup>2</sup> of alkenyl-TOC to <300 μC/cm<sup>2</sup> of alkenyl/thiol-TOC). …”
  8. 1928

    Alkenyl/Thiol Co-Functionalized Titanium-Oxo Nanoclusters Enable Synergistic Lithography for Enhanced Resolution and Sensitivity by Zuohu Zhou (14258773)

    Published 2025
    “…Such dual cross-linkable group functionalization brought additional thiol–ene click reactions upon exposure to enhance intercluster polymerization, which significantly improved the lithography sensitivity of TOCs, with the required exposure energy being reduced by over 70% (decreasing from >1000 μC/cm<sup>2</sup> of alkenyl-TOC to <300 μC/cm<sup>2</sup> of alkenyl/thiol-TOC). …”
  9. 1929

    Alkenyl/Thiol Co-Functionalized Titanium-Oxo Nanoclusters Enable Synergistic Lithography for Enhanced Resolution and Sensitivity by Zuohu Zhou (14258773)

    Published 2025
    “…Such dual cross-linkable group functionalization brought additional thiol–ene click reactions upon exposure to enhance intercluster polymerization, which significantly improved the lithography sensitivity of TOCs, with the required exposure energy being reduced by over 70% (decreasing from >1000 μC/cm<sup>2</sup> of alkenyl-TOC to <300 μC/cm<sup>2</sup> of alkenyl/thiol-TOC). …”
  10. 1930

    Defect-Triggered Reversible Phase Transformation for Boosting Electrochemical Performance of Coordination Polymers by Yixiu Xu (11166860)

    Published 2024
    “…Contrary to this common sense, here we demonstrate that both implanting defects and eliminating defects can significantly boost the specific capacitance of the defect-engineered CPs (DECPs), which are about 1.23 and 1.62 times that of the pristine CP, respectively, without loss of rate capability even after 10,000 charge–discharge cycles. …”
  11. 1931

    Defect-Triggered Reversible Phase Transformation for Boosting Electrochemical Performance of Coordination Polymers by Yixiu Xu (11166860)

    Published 2024
    “…Contrary to this common sense, here we demonstrate that both implanting defects and eliminating defects can significantly boost the specific capacitance of the defect-engineered CPs (DECPs), which are about 1.23 and 1.62 times that of the pristine CP, respectively, without loss of rate capability even after 10,000 charge–discharge cycles. …”
  12. 1932

    Primer sequences. by Koichi Yoshimoto (9298643)

    Published 2024
    “…We examined the mRNA expression of <i>Ddit3</i> (CHOP) and <i>Casp3</i> (caspase-3) on day one after the surgery; mRNA expression of both genes appeared to decrease in the KUS121 group, as compared with the control group, although differences between groups were not significant. …”
  13. 1933
  14. 1934

    Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature by Yunlong Jiao (6672764)

    Published 2024
    “…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …”
  15. 1935

    Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature by Yunlong Jiao (6672764)

    Published 2024
    “…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …”
  16. 1936

    Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature by Yunlong Jiao (6672764)

    Published 2024
    “…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …”
  17. 1937

    Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature by Yunlong Jiao (6672764)

    Published 2024
    “…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …”
  18. 1938

    Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature by Yunlong Jiao (6672764)

    Published 2024
    “…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …”
  19. 1939

    Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature by Yunlong Jiao (6672764)

    Published 2024
    “…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …”
  20. 1940

    Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature by Yunlong Jiao (6672764)

    Published 2024
    “…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …”