Notes
Outline
Radio Observations of Coronal Mass Ejections
N. Gopalswamy
NASA/GSFC, Greenbelt, MD
FASR Workshop, May 22-25, Green Bank WV
Summary: CMEs in Radio
Microwave Observations (FASR HF)
 Prominence Core (best observed)
 DSF (for Space Weather App.), Cavity on the disk
à Arcade formation – CME aftermath
Frontal structure (new)- rarely observed – DR problem
Meterwave  Observations (FASR LF)
à Thermal (CME, Filament, Cavity)
à Nonthermal: type II (shock)
à Nonthermal: type IV (CME core, or other substrucutres)
Longer wavelengths (LOFAR, SIRA)
Nonthermal: Type II, type IV, complex type III
Nonthermal: CME cannibalism
 Maybe thermal emission from CMEs
Reviews:  (Gopalswamy, 1999, 2002)   http://cdaw.gsfc.nasa.gov
Defining a CME:
SOHO/LASCO/C3 Images
CME Structures in the
IP Medium: Magnetic Clouds
• Axial field orientation from Multi-spacecraft Observations (Helios 1&2, Voyager 2, IMP 8
• Flux Rope Structure from Force Free equilibrium calculations
(Burlaga et al., 1981)
Prominence: H-alpha (left, Hiraiso) versus Microwaves (right, Nobeyama)
Prominence Eruption in Microwaves
A Prominence Eruption in Microwaves & EUV (304 A)
click on images to start movie
The Eruption of 2001 Dec 20
Dec 20, 2001 EUV
Arcade formation at the site of eruption in EUV movie
The filament can be seen in the previous day’s movie
2001 Dec 20 LASCO/C2
The ejection occurs into a less dense region. Clear 3-part structure
2000 Oct 22 Event (Fast)
2000 Oct 22 LASCO/C2
Statistical Results
Gopalswamy, Shimojo,  Shibasaki et al. (2002)
BBSO Statistics: 50 limb events (from the last bin)
BBSO study concluded that only 36% of prominence eruptions were associated with white light CMEs!
(Yang & Wang 2002)
Radio Vs Ha Prominence Eruptions (PEs)
A Microwave CME: 2001/04/18
Gopalswamy, Shimojo, Shibasaki, & Howard (2002)
Nobeyama movie of the 2001/04/18 Eruption
The remote brightenings indicate the extent of the CME
Spatial Association: Radio & White Light
Microwave, SXT, EIT, LASCO
Height-Time Plot
CME speed: 1925 km/s (microwaves)
à 2465 km/s in White light
- initial accel: 440 ms-2
- later decel 10 ms-2
• Core: 1625 km/s à close to the LE speed in microwaves.
Hudson et al (2001) associated HXR source (930 km/s) with the microwave core – may not be  correct
•  Imaging was possible because the flare source was occulted
Density, Mass,  Size, & Energy
(Preliminary Results)
Speed & Source Longitude of SEP-associated CMEs of Cycle 23
Gopalswamy et al. 2002, ApJL June 10 issue
SEP CMEs are very fast
  (> 900km/s)
They occur west of E45
The largest bin is 90+: 21%  of SEP events à can be imaged in microwaves
Radio Sun in Meterwaves
•Thermal emission: optical depth could be large at low frequencies.
• Direct imaging using free free emission from  the corona & CMEs (Sheridan et al., 1978; Gopalswamy and Kundu, 1992;  Maia et al., 2000)
Radio CMEs
A Type II Radio Burst
Image of a type II Burst
Imaged by the Clark Lake Radioheliograph in the 1980s
Meterwaves: Nonthermal
Type II radio bursts due to shocks: Relation to CME is controversial (Wagner & MacQeen, 1983; Cane 1984; Gary et al., 1994; Gopalswamy et al., 1998; Cliver et al., 1999; Reiner et al., 2001)
Two Shocks from the same source?
Easy to drive shocks on either side of the “Alfven-speed hump” Gopalswamy et al. JGR  (2001)
Easier to shock the corona in the transverse direction?
(Gopalswamy, Kaiser & Pick, 2000)
Meterwaves: Nonthermal
 Type IV radio  bursts: Nonthermal electrons trapped in CME cores or substructures produce plasma or synchrotron emission (Boischot, 1957; Stewart, 1985; Gopalswamy & Kundu 1990; Bastian et al, 2001)
DH Type II Radio Bursts
New radio window in the decameter-hectometric (DH) wavelength  domain due to WAVES experiment on Wind (Bougeret et al. 1995)
All are CME related: Early phase of IP shocks
Shock-accelerated  (SA) electrons produce complex type III bursts (Reiner & Kaiser, 1999)
Associated CMEs are faster and wider (Gopalswamy et al. 2000-GRL, 2001-JGR)
Good Indicators of geoeffective CMEs
CME interaction discovered (Gopalswamy et al. 2001, ApJL, 548, L91)
No imaging: Need SIRA and LOFAR for studying these radio burst sources
Example of a DH type II burst due to a CME
Radio Signature due to CME Interaction: 00/06/10
This event is unlike the previous: there is a broadband emission for ~0.5 hr following a regular type II burst
A Slow CME is Deflected
Slow CME (290 km/s) overtaken by a fast CME (660 km/s)
The slow CME core deflected to the left from its trajectory
Before reaching the slow CME, the fast one produces a normal type II. During collision with the slow CME, the enhanced radio emission is  produced
A DH Type II & its CME
Properties of radio-rich CMEs
Type II burst starts when the CME reaches ~ 2 Ro !
The RAD2 spectral range (14-1 MHz) Wind/WAVES correspond to 2-10 Ro à Type II bursts can identify shock-driving CMEs in the near-Sun IP medium.
For accelerating CMEs: shocks form at large heliocentric distances
For Halo CMEs: type II occurs first because it takes some time for the CME to be visible above the occulting disk.
(CME time – when the CME first appears in the C2 FOV)
Conclusions for FASR
CME core: optically thick at all FASR frequencies, but can be imaged only at higher frequencies because of the low brightness temperature
CME frontal: can be easily observed in meterwaves if the nonthermal emission is not too strong. In microwaves behind-the-limb high density CMEs can be imaged.
Nonthermal emission from electrons trapped in CME substructures can be a good source of information
Filaments & filament Cavities on the disk à CME source regions