{ "cells": [ { "cell_type": "markdown", "id": "d7599a90", "metadata": {}, "source": [ "# Mono Calibration and EXAFS Results\n", "\n", "This notebook explores the effect of energy miscalibration on EXAFS results.\n", "\n", "EXAFS measurements need a well-calibrated energy, typically coming from a double-cystal monochromator. While EXAFS can be measured in modes without a double-crystal monochromator, that is sort of unusual, and we are not discussing that situation here. A double-cystal monochromator uses Bragg's Law to relate the monochromator angle $\\theta$ to X-ray energy $E$ with\n", "\n", " $\\lambda = \\frac{hc}{E} = 2d\\sin(\\theta) $\n", "\n", "With $h$ being Planck's constant, $c$ the speed of light, and $d$ the lattice spacing of the monochromator crystal. With $d$ in Angstroms and $E$ in eV, $hc \\approx 12398.419$ eV A. The crystal $d$ values for Si, Ge, and C (the most common crystals used0 are typically very well known, but there may be thermally-induced changes. The values of $d$ and an angular offset ($\\theta_0$ may need to be adjusted to calibrate a monochromator.\n", "This is typically done by scanning across a known (or at least reproducible) energies, say the $K$-edges of metal foils, and adjusting $d$ or $\\theta_0$ until the energy is correct. \n", "\n", "\n", "Most commonly, the XANES of some metal foil is measured and the maximumn of the first derivative is set to the tabulated edge energy for the metal. This method will give a bit of a variation as \n", "the energy resolution changes. These days, most good XAFS beamlines have high enough energy \n", "resolution that this is not much of a problem, but it can be a problem for older data. It should \n", "also be said that those tabulated values are not always accurate to better than 1 or 2 eV. In fact, \n", "rather than use the tabulated values such as at https://xraydb.xrayabsorption.org/ the values from Kraft et al Review of Scientific Instruments 67, p681 (1996): (https://doi.org/10.1063/1.1146657) should be used, as they were carefully measured with a single, very high-resolution and consistently calibrated monochromator.\n", "\n", "\n", "Ideally, a well-calibrated monochromator would have a single d-spacing and angular offset that \n", "stays calibrated across the edges of many edges. That is, if the energy needs to be recalibrated\n", "at every edge, the energy will be drifting between those edges, and the reason for any need to\n", "recalibrate should be investigated. If the beamline is well collimated and the angle of the beam \n", "incident on the monochomator is stable, it is certainly possible to have a monochromator set up t\n", "that stays calibrated for weeks and over an energy range of 10 keV or more. \n", "\n", "\n", "For any XAS analysis, the energy scale is critical. Because of the variations above in calibrating \n", "energy, small energy shifts between beamlines or even runs at the same beamline but different months \n", "are not uncommon. If the shift is relatively small, say 1 to 5 eV at 10 keV, simply adding a constant \n", "energy offset is satisfactory.\n", " \n", "You may hear people say that poor calibration leads to large errors in XAFS results or even leads \n", "\"the wrong results\". You should know that when people say things are Wrong is describing scientific\n", "measurements and analysis, they are almost certainly wrong. \n", "\n", "Here, we'll look at these effects\n" ] }, { "cell_type": "code", "execution_count": 12, "id": "7c518804", "metadata": {}, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "3.1352527849954046\n" ] }, { "data": { "application/vnd.plotly.v1+json": { "config": { "plotlyServerURL": "https://plot.ly" }, "data": [ { "line": { "color": "red", "width": 2 }, "name": "angle", "type": "scatter", "uid": "ab35ec84-a2e6-4cfd-bcf5-594f8dcdbae5", "x": [ 8786.204, 8796.258, 8806.253, 8816.27, 8826.27, 8836.292, 8846.337, 8856.322, 8866.372, 8876.361, 8886.416, 8896.409, 8906.425, 8916.464, 8926.483, 8936.483, 8936.998, 8937.471, 8937.944, 8938.417, 8938.976, 8939.406, 8939.878, 8940.352, 8940.824, 8941.384, 8941.814, 8942.287, 8942.761, 8943.319, 8943.793, 8944.224, 8944.697, 8945.257, 8945.73, 8946.204, 8946.635, 8947.108, 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