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Chemical Molar and Mass Fractions

1 minute read

Published:

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.

Electron Inelastic Mean Free Path

1 minute read

Published:

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.

Core Electron Transition Energies

1 minute read

Published:

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.

Useful Calculator for the Diffraction Kinematics of Relativistic Electrons

1 minute read

Published:

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.

core states

Core Electron Transition Energies

1 minute read

Published:

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.

egerton

Electron Inelastic Mean Free Path

1 minute read

Published:

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.

electron beam

Useful Calculator for the Diffraction Kinematics of Relativistic Electrons

1 minute read

Published:

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.

fraction

Chemical Molar and Mass Fractions

1 minute read

Published:

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.

imfp

Electron Inelastic Mean Free Path

1 minute read

Published:

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.

inelastic

Electron Inelastic Mean Free Path

1 minute read

Published:

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.

mass

Chemical Molar and Mass Fractions

1 minute read

Published:

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.

molar

Chemical Molar and Mass Fractions

1 minute read

Published:

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.

transition

Core Electron Transition Energies

1 minute read

Published:

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.

widget

Electron Inelastic Mean Free Path

1 minute read

Published:

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.

Core Electron Transition Energies

1 minute read

Published:

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.

Useful Calculator for the Diffraction Kinematics of Relativistic Electrons

1 minute read

Published:

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.