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It is common when growing single crystals to use compounds which contain an element of interest, rather than using the pure element on its own. For example, copper in the form of CuO is often used instead of pure elemental copper, and fluorine is often used in the form of FeF2 rather than dangerous fluorine gas. When using compounds rather than elements, it is useful to know the relative mass fraction of each element to calculate the mixing ratios needed to grow a particular crystal.
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Unlike x-ray and neutron scattering, electron scattering in a solid is often so strong that the first Born approximation is not enough to describe the distribution of scattered electrons. To understand when higher order (or multiple) scattering occurs, it is useful to have an estimate for the inelastic mean free path (IMFP) for the probe electron. Estimates for the IMFP based on material parameters is therefore a useful metric when performing Electron Energy Loss Spectroscopy (EELS). Indeed, many formulas for estimating the IMFP have been studied in the literature and are nicely compiled in Electron Energy-Loss Spectroscopy in the Electron Microscope by R. Egerton.
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It is useful when performing resonant x-ray scattering, x-ray absorption spectroscopy, or other core-level spectroscopies, to have a quick reference for the element-dependent electron binding energies in solids. These binding energies describe how deep the core electron levels are with respect to the Fermi level (or vacuum, top of valence band, etc.). Because chemical bonding in solids only involves valence electrons, the core levels of atoms in a solid are mostly unchanged compared to that of a free atom in space. Thus, the core level binding energies form a fingerprint uniquely identifying an element.
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When dealing with electron diffraction within an electron microscope, it is often useful to have a quick converter to convert between the beam energy, angles, and reciprocal lattice units (r.l.u.). Below is a simple calculator that converts between electron beam energies, angles, and momentum transfer. For added benefit, there is also a lattice parameter option to present the momentum transfer in reciprocal lattice units where $1\textrm{ r.l.u.} = 2\pi/a$ and $a$ is the lattice parameter.
Short description of portfolio item number 1
Short description of portfolio item number 2
Published in Journal 1, 2009
This paper is about the number 1. The number 2 is left for future work.
Recommended citation: Your Name, You. (2009). "Paper Title Number 1." Journal 1. 1(1). https://academicpages.github.io/files/paper1.pdf
Published in Journal 1, 2010
This paper is about the number 2. The number 3 is left for future work.
Recommended citation: Your Name, You. (2010). "Paper Title Number 2." Journal 1. 1(2). https://academicpages.github.io/files/paper2.pdf
Published in Journal 1, 2015
This paper is about the number 3. The number 4 is left for future work.
Recommended citation: Your Name, You. (2015). "Paper Title Number 3." Journal 1. 1(3). https://academicpages.github.io/files/paper3.pdf
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This is a description of your talk, which is a markdown files that can be all markdown-ified like any other post. Yay markdown!
Published:
This is a description of your conference proceedings talk, note the different field in type. You can put anything in this field.
Undergraduate course, University 1, Department, 2014
This is a description of a teaching experience. You can use markdown like any other post.
Workshop, University 1, Department, 2015
This is a description of a teaching experience. You can use markdown like any other post.