Monolithic quartz platform for cellular contact guidance

2020 ◽  
Vol 10 (2) ◽  
pp. 242-251
Author(s):  
Michael C. Robitaille ◽  
Joseph A. Christodoulides ◽  
Jinny L. Liu ◽  
Wonmo Kang ◽  
Jeff M. Byers ◽  
...  

Abstract

2019 ◽  
Vol 116 (10) ◽  
pp. 1994-2008 ◽  
Author(s):  
Antonetta B.C. Buskermolen ◽  
Hamsini Suresh ◽  
Siamak S. Shishvan ◽  
Andrea Vigliotti ◽  
Antonio DeSimone ◽  
...  

ACS Nano ◽  
2014 ◽  
Vol 8 (4) ◽  
pp. 3546-3555 ◽  
Author(s):  
Meghan K. Driscoll ◽  
Xiaoyu Sun ◽  
Can Guven ◽  
John T. Fourkas ◽  
Wolfgang Losert

2013 ◽  
Vol 104 (2) ◽  
pp. 148a ◽  
Author(s):  
Wolfgang Losert ◽  
Meghan Driscoll ◽  
Can Guven ◽  
Xiaoyu Sun ◽  
John Fourkas

2010 ◽  
Vol 11 (11) ◽  
pp. 3067-3072 ◽  
Author(s):  
Jirun Sun ◽  
Yifu Ding ◽  
Nancy J. Lin ◽  
Jing Zhou ◽  
Hyunwook Ro ◽  
...  

2018 ◽  
Author(s):  
A.B.C. Buskermolen ◽  
H. Suresh ◽  
S.S. Shishvan ◽  
A. Vigliotti ◽  
A. DeSimone ◽  
...  

AbstractContact guidance—the widely-known phenomenon of cell alignment induced by anisotropic environmental features—is an essential step in the organization of adherent cells, but the mechanisms by which cells achieve this orientational ordering remain unclear. Here we seeded myofibroblasts on substrates micropatterned with stripes of fibronectin and observed that contact guidance emerges at stripe widths much greater than the cell size. To understand the origins of this surprising observation, we combined morphometric analysis of cells and their subcellular components with a novel statistical framework for modelling non-thermal fluctuations of living cells. This modelling framework is shown to predict not only the trends but also the statistical variability of a wide range of biological observables including cell (and nucleus) shapes, sizes and orientations, as well as stress-fibre arrangements within the cells with remarkable fidelity. By comparing observations and theory, we identified two regimes of contact guidance: (i) guidance on stripe widths smaller than the cell size (w ≤ 160 μm), which is accompanied by biochemical changes within the cells, including increasing stress-fibre polarisation and cell elongation, and (ii) entropic guidance on larger stripe widths, which is governed by fluctuations in the cell morphology. Overall, our findings suggest an entropy-mediated mechanism for contact guidance associated with the tendency of cells to maximise their morphological entropy through shape fluctuations.


2011 ◽  
Vol 7 (6) ◽  
pp. 2492-2498 ◽  
Author(s):  
Maxime D. Guillemette ◽  
Emmanuel Roy ◽  
François A. Auger ◽  
Teodor Veres

2020 ◽  
Vol 1 (5) ◽  
pp. 100055 ◽  
Author(s):  
Antonetta B.C. Buskermolen ◽  
Tommaso Ristori ◽  
Dylan Mostert ◽  
Mark C. van Turnhout ◽  
Siamak S. Shishvan ◽  
...  

Author(s):  
Carolyn Nohr ◽  
Ann Ayres

Texts on electron diffraction recommend that the camera constant of the electron microscope be determine d by calibration with a standard crystalline specimen, using the equation


Author(s):  
Kin Lam

The energy of moving ions in solid is dependent on the electronic density as well as the atomic structural properties of the target material. These factors contribute to the observable effects in polycrystalline material using the scanning ion microscope. Here we outline a method to investigate the dependence of low velocity proton stopping on interatomic distances and orientations.The interaction of charged particles with atoms in the frame work of the Fermi gas model was proposed by Lindhard. For a system of atoms, the electronic Lindhard stopping power can be generalized to the formwhere the stopping power function is defined as


Author(s):  
A. Kosiara ◽  
J. W. Wiggins ◽  
M. Beer

A magnetic spectrometer to be attached to the Johns Hopkins S. T. E. M. is under construction. Its main purpose will be to investigate electron interactions with biological molecules in the energy range of 40 KeV to 100 KeV. The spectrometer is of the type described by Kerwin and by Crewe Its magnetic pole boundary is given by the equationwhere R is the electron curvature radius. In our case, R = 15 cm. The electron beam will be deflected by an angle of 90°. The distance between the electron source and the pole boundary will be 30 cm. A linear fringe field will be generated by a quadrupole field arrangement. This is accomplished by a grounded mirror plate and a 45° taper of the magnetic pole.


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