Observing the solar corona with a tunable Fabry-Perot filter.
Matthew W Noble1, David M Rust, Pietro N Bernasconi
1Johns Hopkins University Applied Physics Laboratory, 11100 Johns Hopkins Road, Laurel, Maryland 20723, USA.
Applied Optics
|January 6, 2009
Summary
Researchers used a specialized Fabry-Perot etalon during a solar eclipse to rapidly scan the solar corona. This allowed detailed observation of the [Fe X] emission line, revealing coronal structures and velocities.
Area of Science:
- Solar Physics
- Coronal Plasma Studies
- Spectroscopy
Background:
- The solar corona is a dynamic outer atmosphere of the Sun.
- Understanding coronal plasma requires high-resolution spectral analysis of emission lines.
- Observational challenges exist due to the faintness and rapid changes in coronal structures.
Purpose of the Study:
- To utilize a novel solid Fabry-Perot etalon for rapid spectral scanning of the solar corona.
- To observe the [Fe X] emission line during a solar eclipse to map coronal structure.
- To investigate the velocity of coronal plasma features.
Main Methods:
- Employed a Y-cut lithium niobate Fabry-Perot etalon with a 0.16 A passband.
- Used voltage-controlled passband shifting (0.0011 A V(-1)) for spectral scanning.
- Acquired 18 filtergrams across the [Fe X] line profile (6374.4 A) during a 180 s solar eclipse.
Main Results:
- Successfully mapped the structure of the solar corona above a sunspot region.
- Obtained detailed spectral profiles of the forbidden [Fe X] emission line from 10(6) K plasma.
- Detected coronal features with line-of-sight velocities as low as 10 km s(-1).
Conclusions:
- The solid Fabry-Perot etalon is effective for rapid coronal spectral analysis.
- Eclipse observations provide valuable insights into coronal structure and dynamics.
- The study demonstrates the capability to measure subtle velocity variations in coronal plasma.
Related Concept Videos
Flame Photometry: Lab
In a flame photometer, when a solution like potassium chloride is aspirated into the flame, the solvent evaporates, leaving behind dehydrated salt. This salt dissociates into free gaseous atoms in their ground state. Some of these atoms absorb energy from the flame, leading to their excitation. The excited atoms return to the ground state, emitting photons at characteristic wavelengths. Because only electronic transitions are involved, the resulting emission lines are very narrow. The intensity...
Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation
Inductively coupled plasma (ICP) is the common plasma source used in atomic emission spectroscopy (AES), a technique that detects and analyzes various elements in a sample. This method is often called inductively coupled plasma atomic emission spectroscopy (ICP-AES).
There are three main types of inductively coupled plasma atomic emission spectroscopy (ICP-AES) instruments: sequential, simultaneous multichannel, and Fourier transform instruments, with the latter being less commonly used.
There are three main types of inductively coupled plasma atomic emission spectroscopy (ICP-AES) instruments: sequential, simultaneous multichannel, and Fourier transform instruments, with the latter being less commonly used.
Atomic Emission Spectroscopy: Instrumentation
The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers. Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.
UV–Vis Spectrometers
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. Samples for...
UV–Vis Spectroscopy: Woodward–Fieser Rules
UV–Visible absorption spectra of conjugated dienes arise from the lowest energy π → π* transitions. The light-absorbing part of the molecule is called the chromophore, and the substituents directly attached to the chromophore are called auxochromes. A strong correlation exists between the absorption maxima, λmax, and the structure of a conjugated π system. The Woodward–Fieser rules predict the value of λmax for a given structure by adding the contributions...
Inductively Coupled Plasma Atomic Emission Spectroscopy: Principle
Inductively coupled plasma (ICP) is the most widely used plasma source in atomic emission spectroscopy (AES), also known as Inductively Coupled Plasma Optical Emission Spectroscopy (ICP-OES). The ICP source, or torch, consists of three concentric quartz tubes with argon gas flowing through them. A spark from a Tesla coil initiates the ionization of argon, generating a high-temperature plasma.
The ions and electrons produced interact with the fluctuating magnetic field created by a water-cooled...
The ions and electrons produced interact with the fluctuating magnetic field created by a water-cooled...


