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Linking Interplanetary Coronal Mass Ejections (ICMEs) observed in-situ to their CME origin at the Sun SHINE Student Day tutorial July 29 th 2018 Yeimy Rivera University of Michigan

Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

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Page 1: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Linking Interplanetary Coronal Mass Ejections (ICMEs) observed in-situ to their CME origin at the Sun

SHINE Student Day tutorial

July 29th 2018

Yeimy Rivera

University of Michigan

Page 2: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Overview

• Tutorial: CMEs – Remote sensing

observation of CMEs

– Dynamics and Evolution

– In-situ signatures

• Research: Compositional signatures to derive the thermal history

Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 2

Page 3: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 3

• CMEs are large eruptions at the Sun that propel massive amounts of ionized material into the Interplanetary Medium

• Three-part structure of CMEs – Leading edge and cavity: n=107-8 cm-3 and T > 106 K

– Prominence (Core): n = 109 -11 cm-3 and T =104-5 K (Occurring 70% of the time)

LASCO/SOHO C2 white light image, FOV 1.5-6 Rs

Coronal Mass Ejections

SDO/AIA 171Å band (log T = 5.8), 193Å band (log T = 6.1) taken from Parenti et al. (2012)

Page 4: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

CME Dynamics

• Acceleration/Deceleration – MHD form of 'aerodynamic' drag

imposed by solar wind is significant factor to CME propagation and transit time (Vršnak and Žic 2007, Gopalswamy et al. 2001)

• Expansion – More radial in the inner corona and

self-similar out in the Heliosphere (Chen 2011)

• Heating – Prominence material is observed to

transition from absorption to emission in EUV images (Landi et al. 2010)

– Heating source is still an open question

Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4

LASCO/SOHO C3 white light image, FOV 4 -30 Rs

Series of images for a CME in STEREO-A EUVI-A 284Å line (Fe XV formation temperature of 2x106 K)

taken from Landi et al. (2010)

Page 5: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

• Freeze-in process undergone by ions (Hundhausen et al. 1968)

– Rapid decrease in density diminishes the ionization and recombination processes in the plasma

– Ionization level is unchanged beyond the freeze-in height allowing to probe the plasma near the Sun

Ion Freeze-in Process

Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 5

(Landi et al. 2012)

Page 6: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 6

Rich

ard

son

an

d C

an

e (2

01

0)

Interplanetary CMEs

• Plasma properties

- Low proton density • Magnetic Field

- Flux rope, field rotation

Collection of signatures used to identify ICMEs within the continuous solar wind

Page 7: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 7

Interplanetary CMEs

• Energetic Particles - Counter-streaming

electrons • Forbush effect

- Reduction of cosmic ray flux

Page 8: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 8

Interplanetary CMEs

• Compositional anomalies (as compared to solar wind)

- O7+/O6+ enhancement - Higher average charge

state - Characterized by

period of alpha-to-proton >0.08

Page 9: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Deriving properties of Coronal Mass Ejections (CMEs) using in-situ charge state distributions

Yeimy Rivera1, Enrico Landi1, Sue Lepri 1 and Jason Gilbert1 1University of Michigan

July 29th 2018

Page 10: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Michigan Ionization Code

• The MIC is solves a time-dependent ionization equation that governs the evolution of ions in the plasma as they propagate from the Sun (Landi et al. 2012)

• Main inputs:

– Electron density

– Electron temperature

– Bulk flow

• Assumptions:

– Local Thermodynamic equilibrium at boundary

– Electron velocity Maxwellian distribution

Sources

Sinks

MIC Output

Yeimy Rivera | Deriving properties of CMEs using in-situ ion distributions | 10

Page 11: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Michigan Ionization Code

Χ2 calculation

Vary parameters to adjust input

profiles

Best fit results

MAIN INPUTS 1. Density, temperature

and velocity profiles 2. Parameter ranges

and increment size 3. In-situ relative

abundances for each ion species Search

Algorithm

Search Algorithm

Yeimy Rivera | Deriving properties of CMEs using in-situ ion distributions | 11

Page 12: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Final Distributions

χ2 =0.304, 95% confidence

level

Charge State Charge State

Re

lati

ve

A

bu

nd

an

ce

Re

lati

ve

A

bu

nd

an

ce

*Plasma Component (PC)

*

Yeimy Rivera | Deriving properties of CMEs using in-situ ion distributions | 12

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Plasma Evolution

Yeimy Rivera | Deriving properties of CMEs using in-situ ion distributions | 13

Page 14: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Summary • A combination of ions generated from four plasma components undergoing

distinct thermodynamic evolution effectively reproduced the observed ionic distributions

• Plasma component properties at the Sun are similar to those found in prominences/PCTR also includes a warmer component resembling coronal plasma

Next Steps

• Compare results with heating mechanism – Current sheet dissipation

– Wave heating

Yeimy Rivera | Deriving properties of CMEs using in-situ ion distributions | 14

Heating rate

Page 15: Linking Interplanetary Coronal Mass Ejections (ICMEs) observed … · 2019. 3. 10. · Yeimy Rivera | Linking ICMEs observed in-situ to their CME origin at the Sun | 4 LASCO/SOHO

Thank you!

Yeimy Rivera | Deriving properties of CMEs using in-situ ion distributions | 15

Citations 1. Chen, P F, "Coronal mass ejections: Models and their observational basis", Living

Reviews in Solar Physics 8 (2011).

2. Gopalswamy, Nat and Lara, Alejandro and Yashiro, Seiji and Kaiser, Mike L and Howard,

Russell A, "Predicting the 1-AU arrival times of coronal mass ejections", Journal of

Geophysical Research: Space Physics 106, A12 (2001), pp. 29207--29217.

3. Hundhausen, A. J. and Gilbert, H. E. and S.J., Bame, "Ionization state of the

interplanetary plasma.", Journal of Geophysical Research 73, 13 (1968), pp. 5485--5493.

4. Landi, E and Raymond, J C and Miralles, M P and Hara, H, "Physical Conditions in a

Coronal Mass Ejection from HINODE, STEREO, and SOHO Observations", The

Astrophysical Journal 711, 1 (2010), pp. 75--98.

5. Landi, E. and Gruesbeck, J. R. and Lepri, S. T. and Zurbuchen, T. H., "New Solar Wind

Diagnostic Using Both in Situ and Spectroscopic Measurements", The Astrophysical

Journal 750, 2 (2012), pp. 159.

6. Parenti, S and Schmieder, B and Heinzel, P and Golub, L, "ON THE NATURE OF

PROMINENCE EMISSION OBSERVED BY SDO /AIA", The Astrophysical Journal 754, 1

(2012), pp. 66.

7. Richardson, I G and Cane, H V, "Near-earth interplanetary coronal mass ejections

during solar cycle 23 (1996 - 2009): Catalog and summary of properties", Solar Physics

264, 1 (2010), pp. 189--237.

8. Vršnak, B and Žic, T, "Transit times of interplanetary coronal mass ejections and the

solar wind speed", A&A 472 (2007), pp. 937--943.

SHINE Session:

Insights into CMEs

and Their

Substructure(s)