48 research outputs found
Cut-off features in interplanetary solar radio type IV emission
Solar
radio type IV bursts can sometimes show directivity, so that no burst
is observed when the source region in located far from the solar disk
center. This has recently been verified also from space observations, at
decameter wavelengths, using a 3D-view to the Sun with STEREO and Wind
satellites. It is unclear whether the directivity is caused by the
emission mechanism, by reduced radio wave formation toward certain
directions, or by absorption/blocking of radio waves along the line of
sight. We present here observations of three type IV burst events that
occurred on 23, 25, and 29 July 2004, and originated from the same
active region. The source location of the first event was near the solar
disk center and in the third event near the west limb. Our analysis
shows that in the last two events the type IV bursts experienced partial
cut-offs in their emission, that coincided with the appearance of
shock-related type II bursts. The type II bursts were formed at the
flanks and leading fronts of propagating coronal mass ejections (CMEs).
These events support the suggestion of absorption toward directions
where the type II shock regions are located.</div
Formation of Isolated Radio Type II Bursts at Low Frequencies
The first appearance of radio type II burst emission at decameter-hectometer (DH) waves typically occurs in connection, and often simultaneously, with other types of radio emissions. As type II bursts are signatures of propagating shock waves that are associated with flares and coronal mass ejections (CMEs), a rich variety of radio emissions can be expected. However, sometimes DH type II bursts appear in the dynamic spectra without other or earlier radio signatures. One explanation for them could be that the flare-CME launch happens on the far side of the Sun, and the emission is observed only when the source gets high enough in the solar atmosphere. In this study we have analysed 26 radio type II bursts that started at DH waves and were well-separated ('isolated') from other radio emission features. These bursts were identified from all DH type II bursts observed in 1998 - 2016, and for 12 events we had observations from at least two different viewing angles with the instruments on board Wind and the Solar Terrestrial Relations Observatory (STEREO) satellites. We found that only 30% of the type II bursts had their source origin on the far side of the Sun, but also that no bursts originated from the central region of the Sun (longitudes E30 - W40). Almost all of the isolated DH type II bursts could be associated with a shock near the CME leading front, and only few were determined to be shocks near the CME flank regions. In this respect our result differs from earlier findings. Our analysis, which included inspection of various CME and radio emission characteristics, suggests that the isolated DH type II bursts could be a special subgroup within DH type II bursts, where the radio emission requires particular coronal conditions to form and to die out
Formation of Radio Type II Bursts During a Multiple Coronal Mass Ejection Event
We study the solar event on 27 September 2001 that consisted of three
consecutive coronal mass ejections (CMEs) originating from the same
active region, which were associated with several periods of radio type
II burst emission at decameter-hectometer (DH) wavelengths. Our analysis
shows that the first radio burst originated from a low-density
environment, formed in the wake of the first, slow CME. The
frequency-drift of the burst suggests a low-speed burst driver, or that
the shock was not propagating along the large density gradient. There is
also evidence of band-splitting within this emission lane. The origin of
the first shock remains unclear, as several alternative scenarios exist.
The second shock showed separate periods of enhanced radio emission.
This shock could have originated from a CME bow shock, caused by the
fast and accelerating second or third CME. However, a shock at CME
flanks is also possible, as the density depletion caused by the three
CMEs would have affected the emission frequencies and hence the radio
source heights could have been lower than usual. The last type II burst
period showed enhanced emission in a wider bandwidth, which was most
probably due to the CME-CME interaction. Only one shock that could
reliably be associated with the investigated CMEs was observed to arrive
near Earth.
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Investigating the origins of two extreme solar particle events: proton source profile and associated electromagnetic emissions
We analyze the high-energy particle emission from the Sun in two extreme solar particle events, in which protons are accelerated to relativistic energies and can cause a significant signal even in the ground-based particle detectors. Analysis of a relativistic proton event is based on modeling of the particle transport and interaction, from a near-Sun source through the solar wind and the Earth’s magnetosphere and atmosphere to a detector on the ground. This allows us to deduce the time profile of the proton source at the Sun and compare it with observed electromagnetic emissions. The 2 May 1998 event is associated with flare and coronal mass ejection (CME) well observed by the Nan¸cay Radioheliograph, so that the images of radio sources are available. For the 2 November 2003 event, there are available the low-corona images of the CME liftoff obtained at the Mauna Loa Solar Observatory. Those complementary data sets are analyzed jointly with the broadband dynamic radio spectra, EUV images and other data available for both events. We find a common scenario for both eruptions, including the flare’s dual impulsive phase, the CME-launch-associated decimetric-continuum burst, and the late, low-frequency type III radio bursts at the time of the relativistic proton injection into the interplanetary medium. The analysis supports the idea that the two considered events start with emission of relativistic protons previously accelerated during the flare and CME launch, then trapped in large-scale magnetic loops and later released by the expanding CME
Investigating the Origins of Two Extreme Solar Particle Events: Proton Source Profile and Associated Electromagnetic Emissions
We analyze the high-energy particle emission from the Sun in two extreme solar particle events. in which protons are accelerated to relativistic energies and can cause a significant signal even in the ground-based particle detectors. Analysis of a relativistic proton event is based on modeling of the particle transport and interaction, from a near-Sun source through the solar wind and the Earth's magnetosphere and atmosphere to a detector on the ground. This allows us to deduce the time profile of the proton source at the Sun and compare it with observed electromagnetic emissions. The 1998 May 2 event is associated with a. flare and a coronal mass ejection (CME), which were well observed by the Nancay Radioheliograph, thus. the images of the. radio sources are available. For the 2003 November 2 event, the low corona images of the CME liftoff obtained at the Mauna Loa Solar Observatory. are available. Those complementary data sets are analyzed jointly with the broadband dynamic radio spectra, EUV images, and other data available for both events. We find a common scenario for both eruptions, including the flare's dual impulsive phase, the CME-launch-associated decimetric-continuum burst, and the late, low-frequency type III radio bursts at the time of the relativistic proton injection into the interplanetary medium. The analysis supports the idea that the two considered events start with emission of relativistic protons previously accelerated during the flare and CME launch, then trapped in large-scale magnetic loops and later released by the expanding CME