Related Experiment Video
Updated: Feb 3, 2026

13:31
High Speed Sub-GHz Spectrometer for Brillouin Scattering Analysis
Published on: December 22, 2015
15.7K
X-ray spectrometer throughput model for (selected) flat Bragg crystal spectrometers on laser plasma facilities
D B Thorn1, F Coppari1, T Döppner1
1Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
The Review of Scientific Instruments
|November 8, 2018
Summary
We present a simple ray trace method to calibrate x-ray spectrometers at large laser facilities like OMEGA and the National Ignition Facility (NIF). This method uses basic optical design information for accurate calibration and performance estimates.
Area of Science:
- Plasma Physics
- Spectroscopy
- Optical Engineering
Background:
- X-ray spectrometers are crucial for diagnosing plasma conditions and monitoring backlighters at major laser facilities.
- Calibration of these spectrometers is often outdated or unknown, limiting diagnostic accuracy.
- Accurate calibration is essential for reliable experimental data.
Purpose of the Study:
- To develop a straightforward ray tracing method for calibrating flat crystal x-ray spectrometers.
- To provide a practical solution for addressing unknown or outdated spectrometer calibrations.
- To enable accurate photometric throughput, dispersion, solid angle, and spectral resolution estimates.
Main Methods:
- A simple ray trace model was developed using fundamental optical design parameters.
- The model was applied to specific spectrometers at the National Ignition Facility (NIF) and OMEGA laser facility.
- The method requires only basic information about the spectrometer's optical design.
Main Results:
- The ray trace method successfully calibrated flat crystal spectrometers.
- Photometric throughput, dispersion, solid angle, and spectral resolution were estimated.
- The model was validated on the mono angle crystal spectrometer and Super Snout I at NIF, and the X-Ray Spectrometer at OMEGA.
Conclusions:
- The developed ray trace method offers a simple and effective way to calibrate x-ray spectrometers.
- This approach enhances the reliability of plasma diagnostics and backlighter monitoring at large laser facilities.
- Accurate calibration is achievable using basic optical design information, improving experimental outcomes.
Related Concept Videos
IR Spectrometers
2.6K
There are two main infrared (IR) spectrophotometers: dispersive IR spectrometers and Fourier transform infrared (FTIR) spectrometers. In a dispersive IR spectrometer, a beam of infrared radiation produced by a hot wire is divided into two parallel equal-intensity beams using mirrors. One beam passes through the sample, while another is a reference beam. The beams then move through the monochromator, which separates the radiations into a continuous spectrum of different frequencies. The...
2.6K
Mass Spectrometers
8.9K
This lesson details the instrumentation of a mass spectrometer—a physical instrument to perform mass spectrometry on analyte molecules and record the characteristic mass spectra. This is achieved via three chief functions:
8.9K
NMR Spectrometers: Overview
2.2K
NMR spectrometers consist of a strong magnet, a radiofrequency transmitter, and a detector attached to a computer console for recording spectra of samples containing NMR-active nuclei. In first-generation NMR instruments called continuous-wave spectrometers, the resonance frequencies of the nuclei are determined by frequency-sweep or field-sweep methods. The magnetic field strength is fixed and the rf signal is swept in the former, while the radiofrequency signal is fixed and the magnetic field...
2.2K
UV–Vis Spectrometers
3.6K
The absorbance of UV and visible (UV–visible) radiations is measured using a UV–visible spectrophotometer. Deuterium lamps, which emit UV radiation, and tungsten lamps, which produce radiation in the visible region, are used as light sources in UV–visible spectrophotometers. A monochromator or prism is used for diffraction grating, i.e., to split the incoming radiation into different wavelengths. A system of slits is used to focus the desired wavelength on the sample cell.
3.6K
X-ray Crystallography
26.2K
The size of the unit cell and the arrangement of atoms in a crystal may be determined from measurements of the diffraction of X-rays by the crystal, termed X-ray crystallography.
Diffraction
Diffraction is the change in the direction of travel experienced by an electromagnetic wave when it encounters a physical barrier whose dimensions are comparable to those of the wavelength of the light. X-rays are electromagnetic radiation with wavelengths about as long as the distance between neighboring...
Diffraction
Diffraction is the change in the direction of travel experienced by an electromagnetic wave when it encounters a physical barrier whose dimensions are comparable to those of the wavelength of the light. X-rays are electromagnetic radiation with wavelengths about as long as the distance between neighboring...
26.2K
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences
1.8K
A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
1.8K

