Analyzing Solar Energetic Particle Onset Times
A study on the impact of CME characteristics on particle release times.
― 6 min read
Table of Contents
- Types of Particle Events
- Importance of Onset Times
- Case Study of Two Events
- CME Development and Shock Wave Formation
- Statistical Observations
- Event Characteristics
- Radio Bursts and Their Significance
- Active Region Properties
- Evaluating Proton Release Times
- Shock Wave Behavior
- Potential CME Interactions
- Summary of Observations
- Implications for Space Weather Prediction
- Future Research Directions
- Conclusion
- Original Source
- Reference Links
Solar energetic particle events are important phenomena that occur during solar activity. These events involve the release of high-energy particles, such as Protons, from the Sun, typically as a result of coronal mass ejections (CMEs). CMEs are massive bursts of solar wind and magnetic fields rising above the solar corona, or the outer layer of the sun. Understanding these events is critical because they can significantly impact space weather, which can affect satellite operations, communications, and even human health in space.
Types of Particle Events
Solar energetic particle events can be classified into two main types: gradual events and impulsive events. Gradual events are usually linked to fast-moving CMEs and exhibit a slow onset of particle release. Impulsive events, on the other hand, are associated with solar flares and show a rapid increase in particle intensity. The focus here is on gradual events, particularly those that show varying onset times.
Importance of Onset Times
The onset time, or TO, is defined as the time at which the first particles are detected following the launch of a CME. Analyzing TO is important for predicting space weather since the timing of energetic particle arrivals can help forecasters assess potential impacts on Earth. It has been observed that there is a wide range of TOS for these events, even when the source regions on the sun are relatively close to the Earth and have similar CME characteristics.
Case Study of Two Events
In this discussion, two particular events from the western hemisphere are examined. Despite having similar characteristics, such as CME speed and the regions from which they originated, these events displayed significantly different onset times for particle release. By studying 10 MeV protons from satellite data, important insights into the reasons behind these differences can be gained.
CME Development and Shock Wave Formation
The development of a CME and the associated shock wave plays a significant role in determining the TO. When a CME is launched, it generates shock waves that can accelerate particles like protons. The Alfvén Mach number, which measures how fast the shock wave moves compared to the local solar wind, is a crucial factor in this process. A higher Mach number indicates a more effective shock wave capable of accelerating particles.
To understand how these shock waves develop, researchers analyze the height and speed of the CME as it moves away from the sun. They combine measurements of CME speed with radio dynamic spectra, which can indicate shock wave activity. By examining how the shock wave progresses over time, it is possible to gain insights into the delays in particle release.
Statistical Observations
Studies have shown that there is a general trend in TO based on the location of the CME. Events originating from regions in the western hemisphere tend to show shorter TO when compared to those from other areas. However, there are numerous exceptions to this rule, where some events with short TO originate from poorly connected locations, indicating that other factors may also play a role.
Event Characteristics
The two events selected for this analysis occurred on different dates but had similar CME speeds and source locations. By comparing the parameters of these events, such as the onset of Type II Radio Bursts and the timing of high-energy proton detection, the reasons for the differing TO can be explored.
Radio Bursts and Their Significance
Type II radio bursts are a key indicator of shock wave formation. They can provide information on the timing and strength of the shock wave generated by a CME. In the first event, the type II radio burst started shortly after the CME was launched, suggesting that a strong shock was formed early on. In contrast, the second event exhibited weaker and intermittent type II bursts, indicating that the shock wave was not as strong, which may have contributed to the longer TO.
Active Region Properties
The properties of the active regions that produced the CMEs are also important in understanding the differences in TO. The first region was found to be more complex magnetically, while the second region featured a simpler configuration. This complexity may affect how efficiently particles are accelerated and released during events.
Evaluating Proton Release Times
To accurately assess the proton release times for the two events, additional analyses were performed using different satellite data that provided better detection capabilities in the energy ranges of interest. These analyses revealed that the release times were still significantly different, even when considering the delays in detection. This suggests that the differences in TO were not solely due to observational factors but involved physical processes related to CME dynamics and the shock wave's development.
Shock Wave Behavior
As the CME propagates, the shock wave evolves in strength and speed. The rate at which the CME accelerates influences the strength of the shock wave and the Alfvén Mach number. For the first event, the CME quickly reached a high speed, resulting in a strong shock wave that allowed for rapid particle acceleration. Conversely, the CME in the second event exhibited a slower acceleration, which resulted in a weaker shock and delayed proton release.
Potential CME Interactions
Another factor that may contribute to the differences in TO is the interaction between CMEs. If a fast CME catches up to a slower one, the interaction could lead to enhanced particle acceleration. In the case of the second event, a preceding CME may have affected the conditions under which particles were accelerated, although the timing of the radio signals indicates that this interaction might not have been immediately apparent.
Summary of Observations
The differences in TO observed in the two events highlight the complexities involved in CME dynamics and particle acceleration. Factors such as the characteristics of the shock wave, interactions between CMEs, and the properties of the active regions all contribute to the varying release times of energetic particles.
Implications for Space Weather Prediction
Understanding the factors that influence TO can improve space weather forecasting efforts. By developing methods to analyze shock wave behavior and active region properties, scientists can better predict the arrival of energetic particles on Earth. This is vital for protecting satellite systems and informing astronauts of potential risks during solar events.
Future Research Directions
Further research is needed to confirm the findings from this study and explore additional factors that may affect TO and particle release. This could include using more advanced modeling techniques to simulate CME dynamics, as well as gathering additional data from various satellite missions to create a more comprehensive understanding of solar energetic particle events.
Conclusion
Solar energetic particle events are a key aspect of space weather that can have significant impacts on technology and human activities. By studying the factors that control the onset times of these events, scientists can improve their understanding of solar activity and enhance space weather forecasts. The investigation of CME dynamics and their interactions will continue to be a vital area of research as we seek to better understand our solar environment.
Title: Solar Energetic Particle Events with Short and Long Onset Times
Abstract: Gradual solar energetic particle (SEP) events, usually attributed to shock waves driven by coronal mass ejections (CMEs), show a wide variety of temporal behaviors. For example, TO, the >10 MeV proton onset time with respect to the launch of the CME, has a distribution of at least an order of magnitude, even when the source region is not far from the so-called well-connected longitudes. It is important to understand what controls TO, especially in the context of space weather prediction. Here we study two SEP events from the western hemisphere that are different in TO on the basis of >10 MeV proton data from the Geostationary Operations Environmental Satellite, despite similar in the CME speed and longitude of the source regions. We try to find the reasons for different TO, or proton release times, in how the CME-driven shock develops and the Alfv\'en Mach number of the shock wave reaches some threshold, by combining the CME height-time profiles with radio dynamic spectra. We also discuss how CME-CME interactions and active region properties may affect proton release times.
Authors: Kosuke Kihara, Ayumi Asai, Seiji Yashiro, Nariaki V. Nitta
Last Update: 2023-02-27 00:00:00
Language: English
Source URL: https://arxiv.org/abs/2302.13541
Source PDF: https://arxiv.org/pdf/2302.13541
Licence: https://creativecommons.org/licenses/by/4.0/
Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.
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