Cells receive signals from the extracellular matrix through receptor-dependent interactions, but they are also influenced by the mechanical properties of the matrix. Although bulk properties of substrates have been shown to affect cell behavior, we show here that nanoscale properties of collagen fibrils also play a significant role in determining cell phenotype. Type I collagen fibrils assembled into thin films provide excellent viewing of cells interacting with individual fibrils. Cells can be observed to extensively manipulate the fibrils, and this behavior seems to result in an incompletely spread stellate morphology and a nonproliferative phenotype that is typical of these cells in collagen gels. We show here that thin films of collagen fibrils can be dehydrated, and when seeded on these dehydrated fibrils, smooth muscle cells spread and proliferate extensively. The dehydrated collagen fibrils appear to be similar to the fully hydrated collagen fibrils in topology and in presentation of beta(1) integrin ligation sites, but they are mechanically stiffer. This decrease in compliance of dehydrated fibrils is seen by a failure of cell movement of dehydrated fibrils compared to their ability to rearrange fully hydrated fibrils and from direct measurements by nanoindentation and quantitative atomic force measurements. We suggest that increase in the nanoscale rigidity of collagen fibrils can cause these cells to assume a proliferative phenotype.
We have investigated strong optical
nonlinearity of monolayer MoS2(1–x)Se2x
across the exciton resonance, which
is directly tunable by Se doping. The quality of monolayer alloys
prepared by chemical vapor deposition is verified by atomic force
microscopy, Raman spectroscopy, and photoluminescence analysis. The
crystal symmetry of all of our alloys is essentially D
3h
, as confirmed by polarization-dependent
second-harmonic generation (SHG). The spectral structure of the exciton
resonance is sampled by wavelength-dependent SHG (λ = 1000–1800
nm), where the SHG resonance red-shifts in accordance with the corresponding
optical gap. Surprisingly, the effect of compositional variation turns
out to be much more dramatic owing to the unexpected increase of B-exciton-induced SHG, which indeed dominates over the A-exciton resonance for x ≥ 0.3.
The overall effect is therefore stronger and broader SHG resonance
where the latter arises from different degrees of red-shift for the
two exciton states. We report the corresponding absolute SHG dispersion
of monolayer alloys, χ(2), as a function of Se doping.
We believe that our finding is a critical step toward engineering
highly efficient nonlinear optical van der Waals materials working
in a broader performance range.
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