General description
1. Focus on Decay of Active regions
Decay of Active regions: see slides in 4-Bellot-Rubio-SAP4_magnetoconvection5_final.pptx:
Decay process of ARs is not well known:
- Slow, may last a few weeks
- ARs approach limb and suffer from projection effects
- Emerging flux starts to reconnect with preexisting flux very soon
- Appearance of filaments, flux rope eruptions and CMEs in late phases of decay
- Sunspot fragmentation by light bridges?
- Flux erosion by convective flows?
- Role of moving magnetic features?
- How is the AR flux dispersed?
- What is the fate of the flux?
Default SOOP duration: 15 days
Pointing requirements: target pointing and tracking
Triggers: disabled
2. Focus on Thermal Non Equilibrium
Coronal loops in active regions constantly undergo heating and cooling cycles, reflected in the observed intensity variability across the spectrum. The temporal and spatial scales of this variability are key characteristics of the underlying coronal heating mechanisms (SAP 3.1.1.2.1). The heating mechanisms are expected to occur over short temporal and spatial scales. Footpoint or uniformly distributed heating, and quasi-steady or low frequency heating lead to different global thermal evolution of loops.
A leading theory behind the observed EUV intensity variability over several hours scale in loops is thermal non-equilibrium (TNE), in which the loops are preferentially heated at the footpoints and in a quasi-steady manner. Two key observables of TNE are: (1) long-period EUV intensity pulsations (having periods of up to 15 hours or more) and (2) warm and cool condensations, observable in TR and chromospheric lines. The condensations, which correspond to the coronal rain phenomenon, are partially ionised cool and dense clumps driven by thermal instability of widths down to 0.3’’ that occur in groups and can trace the entire loop during their fall to the lower atmosphere. The presence or absence of rain, the global characteristics of the heating and cooling (TNE) cycles such as the evolution of temperature and density and the period of the cycles, are observables that provide major constraints on the heating properties (SAP 1.2.1.3, 1.2.1.7, 1.2.2.3, 1.2.2.5, 1.3.1, 3.1.2.1). Furthermore, observations are currently limited to the follow-up of active regions during their passage on-disk, and the length of TNE cycles is constrained by this artificial limitation.
Since Solar Orbiter can, to some approximation, co-rotate with ARs, it allows a longer follow-up, thus allowing to investigate how much can TNE cycles last. In this study we aim at capturing from the unique standpoint and capabilities of Solar Orbiter the major aspects of TNE cycles in the solar corona.
With Solar Orbiter observations we aim to address three main scientific questions:
Q1: How long do they last? How/when do they start and stop?
Q2: Are condensations in prominence-rain hybrids (null-point topologies) due to TNE cycles? Are their counterparts on the solar disk related to the observed quiet Sun long-period EUV pulsations?
Q3: Are these cycles producing elemental abundances variations?
Duration: Follow-up of a region during one observing window (10 days). If possible, 2 consecutive windows, allowing a follow-up of 20 days.
Pointing requirements: AR, prominence-rain hybrids (limb and on-disk), Tracking mode
Preferred execution time / SolO location: Close to perihelion SolO will be able to have a high-resolution view of the off-limb corona. The aim is to follow an AR during a part of its lifetime, from its appearance off-limb, its passage on-disk and disappearance at the other limb over an extended period of time thanks to SolO’s co-rotation. We aim at characterizing the properties of TNE cycles, in terms of periods, total duration, velocities of the coronal flows and condensations, variation in elemental abundances.
To follow-up the AR we request tracking mode. Since this mode combines observations off-limb and on-disk it combines different observing programs detailed below.
Observations requirement (baseline)
1. Active region decay:
Instrument | Mode | Comment |
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EUI | EUV & LYA Coronal hole modes (C) 600 s cadence | EUV + Lyman alpha, FOV and resolution matching PHI |
SPICE | SPICE Dynamics (bracketed by SPICE Composition Mapping) | 2" slit, 128 slit positions, scan duration 11 minutes |
PHI | PHI_magnetograph_FDT/HRT_2 HRT | Full FOV, 10 min cadence, 5 quantities, 2x2 binning |
Metis | METIS standard modes: MAGTOP or GLOBAL | Metis can potentially provide context data before and after the 15 day SOOP (offpointing during the 15 days) |
2. Non thermal equilibrium
Instruments | Mode | Comment | Rebin/subfield (pixels) |
EUI | FSI Synoptic mode (S)
EUV & LYA Active Region modes (A) | 1-2 observing windows Cadence (for FSI): 10 min 1h per day for HRI |
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SPICE | Preferred spectral lines: Mg VIII 772, Ne VIII 770, OVI 1032, CII, C III, OV doublet (760.2 & 760.4) | Raster off-limb can be of reduced X | |
STIX | STIX Normal mode | Triggers Active |
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PHI | FDT Synoptic mode | Covering whole observation, 1hr cadence | Full disk |
Science objectives
1. Active region decay
SAP objective | Target | Duration | Opportunity (e.g., orbital requirements, solar cycle phase, quadrature ...) | Operational constraints | Additional comments |
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5.5.2.4 | Isolated AR , complex AR on E limb | 15 days | Perihelion: to ensure near-co-rotation, Stereoscopy, which constrains Earth-Sun-SC angle | Duration 15 days | Potentially coordinated with ground based DKIST/EST/GREGOR/NST for short-term studies |
1.1.3.3 What is the distribution of the open magnetic flux? | coronal holes, QS, AR | ||||
1.2.1.3 Contribution of flare-like events on all scales | increase cadence; only partially | ||||
1.2.1.7 Detect and characterise waves in closed and open structures | plumes | high latitude pointing | |||
1.2.2.5 Magnetic reconnection in the chromosphere, the transition region and the corona | increase cadence | ||||
(2.1.1.1 CME initiation) probably better FDT | |||||
4.1.1.1 Track granules and magnetic features to follow their motion and interactions | increase cadence | ||||
4.1.3.2 Follow individual magnetic features flux from lower to high latitudes | |||||
4.1.3.4 How supergranular flows facilitate/impede transport of magnetic features? | increase cadence |
2. Non thermal equilibrium
SAP Objective | Target | Duration | Opportunity | Operational constraints | Additional comments |
3.1.2.1 Understand energy release and particle acceleration process | Active Region
Properties of flare energy release
Acceleration relating to the magnetic reconnection process
| 2 hours | SolO close to Perihelion | Target tracking? |
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3.1 How and where are energetic particles accelerated at the Sun? | Active region | 2 hours | SolO close to Perihelion |
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Flaring region in AR | 2 hours | SolO close to Perihelion |
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Active region | 2 hours | SolO close to Perihelion |
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1.2.2.3 What are the origins of waves, turbulence and small scale structures? | Active region | 2 hours |
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Active region loops, spicules above limb | 2 hours |
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1.2.1.7 Detect and characterise waves in closed and open structures | Active region loops, spicules at limb | 2 hours |
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Active region loops | 2 hours | SolO close to Perihelion |
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1.2.2.5 Magnetic reconnection in the chromosphere, the transition region and the corona | Active region loops | 2 hours | SolO close to Perihelion |
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Active region loops |
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1.2.1.10 Heating in flaring loops and compare to heating in active regions | Active region loops | 2 hours |
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Instances run / planned
LTP6:
2022-03-31 to 04-04 (SOOP coordinators: L. Bellot ) (science objective: Active region decay)
LTP9:
2022-10-16 to 27, 2022-10-29, 2022-11-01 to 06 (SOOP coordinators: S. Parenti, G. Valori) (science objective: Active region decay)
Science outcomes
Ref of paper using the SOOP data
Original SOOP proposers
Luis Bellot-Rubio, Andrzej Fludra, S. Parenti
1 Comment
Anik De Groof
SOOP ID in SOOP Kitchen = RS0