Novel growth mode of solid–liquid–solid (SLS) silica nanowires

2011 ◽  
Vol 26 (17) ◽  
pp. 2232-2239 ◽  
Author(s):  
Jae Ho Lee ◽  
Michael A. Carpenter ◽  
Robert E. Geer
Keyword(s):  
Growth Mode ◽  
Silica Nanowires ◽  
Image Position ◽  
Solid Liquid

Abstract

Experimental data for solid–liquid flows at intermediate and high Stokes numbers

2019 ◽  
Vol 883 ◽  
Author(s):  
Sarah E. Mena ◽  
Jennifer Sinclair Curtis
Keyword(s):  
Experimental Data ◽  
Image Position ◽  
Liquid Flows ◽  
Solid Liquid

An In-Plane Solid-Liquid-Solid Growth Mode for Self-Avoiding Lateral Silicon Nanowires

2009 ◽  
Vol 102 (12) ◽  
Author(s):  
Linwei Yu ◽  
Pierre-Jean Alet ◽  
Gennaro Picardi ◽  
Pere Roca i Cabarrocas
Keyword(s):  
Silicon Nanowires ◽  
Growth Mode ◽  
Solid Liquid

scholarly journals Cryogenic specimens for nanoscale characterization of solid–liquid interfaces

MRS Bulletin ◽  
2019 ◽  
Vol 44 (12) ◽  
pp. 949-955 ◽  
Author(s):  
Michael J. Zachman ◽  
Niels de Jonge ◽  
Robert Fischer ◽  
Katherine L. Jungjohann ◽  
Daniel E. Perea
Keyword(s):  
Liquid Interfaces ◽  
Nanoscale Characterization ◽  
Image Position ◽  
Solid Liquid

Abstract

scholarly journals Growth-mode induced defects in epitaxial SrTiO3 thin films grown on single crystal LaAlO3 by a two-step PLD process

2011 ◽  
Vol 26 (6) ◽  
pp. 770-774 ◽  
Author(s):  
Dong Su ◽  
Tomoaki Yamada ◽  
Roman Gysel ◽  
Alexander K. Tagantsev ◽  
Paul Muralt ◽  
...  
Keyword(s):  
Thin Films ◽  
Single Crystal ◽  
Growth Mode ◽  
Image Position ◽  
Induced Defects

Abstract

Importance of line and interfacial energies during VLS growth of finely stranded silica nanowires

2011 ◽  
Vol 26 (17) ◽  
pp. 2247-2253 ◽  
Author(s):  
Martin Bettge ◽  
Scott MacLaren ◽  
Steve Burdin ◽  
Daniel Abraham ◽  
Ivan Petrov ◽  
...  
Keyword(s):  
Interfacial Energies ◽  
Silica Nanowires ◽  
Vls Growth ◽  
Image Position

Abstract

Simple Identification of Electron Diffraction Ring Patterns

1969 ◽  
Vol 27 ◽  
pp. 160-161
Author(s):  
Carolyn Nohr ◽  
Ann Ayres
Keyword(s):  
Electron Microscope ◽  
Electron Diffraction ◽  
Diffraction Ring ◽  
Image Position

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

Atomic orientation effects in proton stopping at low velocity

1983 ◽  
Vol 41 ◽  
pp. 708-709
Author(s):  
Kin Lam
Keyword(s):  
Polycrystalline Material ◽  
Charged Particles ◽  
Target Material ◽  
Stopping Power ◽  
Low Velocity ◽  
Electronic Density ◽  
Interatomic Distances ◽  
Frame Work ◽  
Image Position ◽  
Atomic Orientation

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

A Magnetic Spectrometer for a Scanning Transmission Electron Microscope

1974 ◽  
Vol 32 ◽  
pp. 436-437
Author(s):  
A. Kosiara ◽  
J. W. Wiggins ◽  
M. Beer
Keyword(s):  
Scanning Transmission Electron Microscope ◽  
Magnetic Spectrometer ◽  
Fringe Field ◽  
Curvature Radius ◽  
Magnetic Pole ◽  
Quadrupole Field ◽  
Transmission Electron ◽  
Scanning Transmission ◽  
Under Construction ◽  
Image Position

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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