Back Cover: Large-Area Elemental Imaging Reveals Van Eyck's Original Paint Layers on the Ghent Altarpiece (1432), Rescoping Its Conservation Treatment (Angew. Chem. Int. Ed. 17/2017)

2017 ◽  
Vol 56 (17) ◽  
pp. 4892-4892
Author(s):  
Geert Van der Snickt ◽  
Hélène Dubois ◽  
Jana Sanyova ◽  
Stijn Legrand ◽  
Alexia Coudray ◽  
...  
Keyword(s):  
Large Area ◽  
Elemental Imaging ◽  
Back Cover ◽  
Conservation Treatment

Large-Area Elemental Imaging Reveals Van Eyck's Original Paint Layers on the Ghent Altarpiece (1432), Rescoping Its Conservation Treatment

2017 ◽  
Vol 56 (17) ◽  
pp. 4797-4801 ◽  
Author(s):  
Geert Van der Snickt ◽  
Hélène Dubois ◽  
Jana Sanyova ◽  
Stijn Legrand ◽  
Alexia Coudray ◽  
...  
Keyword(s):  
Large Area ◽  
Elemental Imaging ◽  
Conservation Treatment

Large-Area Elemental Imaging Reveals Van Eyck's Original Paint Layers on the Ghent Altarpiece (1432), Rescoping Its Conservation Treatment

2017 ◽  
Vol 129 (17) ◽  
pp. 4875-4879 ◽  
Author(s):  
Geert Van der Snickt ◽  
Hélène Dubois ◽  
Jana Sanyova ◽  
Stijn Legrand ◽  
Alexia Coudray ◽  
...  
Keyword(s):  
Large Area ◽  
Elemental Imaging ◽  
Conservation Treatment

scholarly journals Rücktitelbild: Large-Area Elemental Imaging Reveals Van Eyck's Original Paint Layers on the Ghent Altarpiece (1432), Rescoping Its Conservation Treatment (Angew. Chem. 17/2017)

2017 ◽  
Vol 129 (17) ◽  
pp. 4972-4972
Author(s):  
Geert Van der Snickt ◽  
Hélène Dubois ◽  
Jana Sanyova ◽  
Stijn Legrand ◽  
Alexia Coudray ◽  
...  
Keyword(s):  
Large Area ◽  
Elemental Imaging ◽  
Conservation Treatment

Inside Back Cover: Large-area fabrication of equidistant free-standing Si crystals on nanoimprinted glass (Phys. Status Solidi RRL 10-11/2011)

2011 ◽  
Vol 5 (10-11) ◽  
Author(s):  
Tobias Sontheimer ◽  
Eveline Rudigier-Voigt ◽  
Matthias Bockmeyer ◽  
Carola Klimm ◽  
Peter Schubert-Bischoff ◽  
...  
Keyword(s):  
Glass Phys ◽  
Large Area ◽  
Free Standing ◽  
Back Cover

A large area full-field EDXRF imaging system based on a THCOBRA gaseous detector

2015 ◽  
Vol 30 (2) ◽  
pp. 343-352 ◽  
Author(s):  
A. L. M. Silva ◽  
M. L. Carvalho ◽  
K. Janssens ◽  
J. F. C. A. Veloso
Keyword(s):  
Imaging System ◽  
Large Area ◽  
Full Field ◽  
X Ray ◽  
Elemental Imaging

A large area EDXRF imaging system based on a 2D-THCOBRA detector, an X-ray tube and a pinhole for elemental imaging applications.

Inside Back Cover: Direct Patterning and Biofunctionalization of a Large-Area Pristine Graphene Sheet (Chem. Asian J. 3/2015)

2015 ◽  
Vol 10 (3) ◽  
pp. 767-767
Author(s):  
Daewha Hong ◽  
KiEun Bae ◽  
Duckshin Park ◽  
Houngkyung Kim ◽  
Seok-Pyo Hong ◽  
...  
Keyword(s):  
Graphene Sheet ◽  
Pristine Graphene ◽  
Large Area ◽  
Back Cover ◽  
Direct Patterning

scholarly journals Back Cover: A Durable, Flexible, Large‐Area, Flame‐Retardant, Early Fire Warning Sensor with Built‐In Patterned Electrodes (Small Methods 4/2021)

Small Methods ◽  
2021 ◽  
Vol 5 (4) ◽  
pp. 2170016
Author(s):  
Fawad Khan ◽  
Shanchi Wang ◽  
Zhewen Ma ◽  
Adnan Ahmed ◽  
Pingan Song ◽  
...  
Keyword(s):  
Flame Retardant ◽  
Large Area ◽  
Back Cover ◽  
Patterned Electrodes

Convergent Beam Electron Diffraction

1978 ◽  
Vol 36 (3) ◽  
pp. 304-315
Author(s):  
G. Lehmpfuhl
Keyword(s):  
Electron Diffraction ◽  
Diffraction Pattern ◽  
Crystal Surface ◽  
Diffraction Spot ◽  
Crystal Thickness ◽  
Large Area ◽  
Electron Microscopic ◽  
Additional Information ◽  
Microscopic Investigations

Introduction In electron microscopic investigations of crystalline specimens the direct observation of the electron diffraction pattern gives additional information about the specimen. The quality of this information depends on the quality of the crystals or the crystal area contributing to the diffraction pattern. By selected area diffraction in a conventional electron microscope, specimen areas as small as 1 µ in diameter can be investigated. It is well known that crystal areas of that size which must be thin enough (in the order of 1000 Å) for electron microscopic investigations are normally somewhat distorted by bending, or they are not homogeneous. Furthermore, the crystal surface is not well defined over such a large area. These are facts which cause reduction of information in the diffraction pattern. The intensity of a diffraction spot, for example, depends on the crystal thickness. If the thickness is not uniform over the investigated area, one observes an averaged intensity, so that the intensity distribution in the diffraction pattern cannot be used for an analysis unless additional information is available.

TEM Study of a Tilt Boundary in Hot-Pressed Silicon

1981 ◽  
Vol 39 ◽  
pp. 160-161
Author(s):  
C. B. Carter ◽  
J. Rose ◽  
D. G. Ast
Keyword(s):  
Electron Diffraction ◽  
Imaging Technique ◽  
Interface Structure ◽  
Large Area ◽  
Weak Beam ◽  
Lattice Fringe ◽  
Electron Diffraction Technique ◽  
Tilt Boundaries ◽  
Beam Technique ◽  
Twist Boundaries

The hot-pressing technique which has been successfully used to manufacture twist boundaries in silicon has now been used to form tilt boundaries in this material. In the present study, weak-beam imaging, lattice-fringe imaging and electron diffraction techniques have been combined to identify different features of the interface structure. The weak-beam technique gives an overall picture of the geometry of the boundary and in particular allows steps in the plane of the boundary which are normal to the dislocation lines to be identified. It also allows pockets of amorphous SiO2 remaining in the interface to be recognized. The lattice-fringe imaging technique allows the boundary plane parallel to the dislocation to be identified. Finally the electron diffraction technique allows the periodic structure of the boundary to be evaluated over a large area - this is particularly valuable when the dislocations are closely spaced - and can also provide information on the structural width of the interface.

P20 phosphor on polyimide as a large area high-resolution transmission screen for slow scan CCD systems

1995 ◽  
Vol 53 ◽  
pp. 20-21
Author(s):  
C. C. Ahn ◽  
S. Karnes ◽  
M. Lvovsky ◽  
C. M. Garland ◽  
H. A. Atwater ◽  
...  
Keyword(s):  
Mechanical Stability ◽  
High Energy ◽  
Practical Implementation ◽  
Line Pair ◽  
Modulation Transfer ◽  
Large Area ◽  
Ccd Imaging ◽  
Transmission Electron ◽  
The One ◽  
Beam Broadening

The bane of CCD imaging systems for transmission electron microscopy at intermediate and high voltages has been their relatively poor modulation transfer function (MTF), or line pair resolution. The problem originates primarily with the phosphor screen. On the one hand, screens should be thick so that as many incident electrons as possible are converted to photons, yielding a high detective quantum efficiency(DQE). The MTF diminishes as a function of scintillator thickness however, and to some extent as a function of fluorescence within the scintillator substrates. Fan has noted that the use of a thin layer of phosphor beneath a self supporting 2μ, thick Al substrate might provide the most appropriate compromise for high DQE and MTF in transmission electron microcscopes which operate at higher voltages. Monte Carlo simulations of high energy electron trajectories reveal that only little beam broadening occurs within this thickness of Al film. Consequently, the MTF is limited predominantly by broadening within the thin phosphor underlayer. There are difficulties however, in the practical implementation of this design, associated mostly with the mechanical stability of the Al support film.

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