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Figure 5 Bright field cross-section TEM images for Ti/Al ohmic contacts.

Figure 2 a 002 dark field (cross-section) transmission electron microscopy (TEM) images of two vertically aligned QD formed after depositing1.4 ML of InAs into a GaAs nanohole (QD1), the growth of 4-nm-thick GaAs barrier acting as tunneling layer and a final deposition of 0.9 ML of InAs (QD2).

Figure 2a and 2b shows 002 dark field (cross-sections) transmission electron microscopy (TEM) images for the samples with 1.4 and 1.2 ML of InAs deposited into the nanoholes forming the QD1 layer.

(a) Bright-field cross-section image of the periodic HfO2 stripe pattern.

Dark-field cross-section image (a) and the HRTEM image (b).

In order to understand the effect of film growth on structure and magnetic properties, a micrograph of the cross-section of 500-nm NiFe2O4 film was taken by TEM. Figure 4a is the dark-field cross-section image.

Bright-field, cross-section TEM images of the Pt(Pt2Si /3C-SiC interface for the as-dePt2Si /3C-SiC) and after annealinterface0°C (b), 700°C (c), and 900°C (d). forure 3 Morphology of the SiC surface and current map of an adjacent Pt contact.

We assume a Reid Axford time profile for the particle injection at the base of a flux tube described by an Archimedean spiral magnetic field whose cross section A(r) expands as r2 cos, where r is the radial distance and ψ(r) is the angle between the magnetic field line and the radial direction.

Therefore, the far-field scattering cross section looks like an 8-shape with a major energy flux along the z axis.

The nucleus leads to a clear local disturbance of the flow field in a cross section that includes the nucleus compared to the flow field without.

This Workshop was organized by the National Nuclear Data Center, Brookhaven National Laboratory, to provide a forum for reporting on the status of the growing field of neutron cross section covariances for applications and for discussing future directions of the work in this field.