Coronal Mass Ejection: Initiation, Magnetic Helicity, and Flux Ropes. I. Boundary Motion-driven Evolution
By Tahar Amari, J. Luciani, J. Aly, Z. Mikić, Jon A. Linker. 2003
275 citations recorded by the source corpus.
Subfields: Astronomy and Astrophysics, Molecular Biology
View Paper: https://www.semanticscholar.org/paper/6ed1e364e899d858d95c7d845c212246a6aa59c3
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Astronomy and Astrophysics
In Molecular Biology
Citations in the corpus
- The standard flare model in three dimensions - III. Slip-running reconnection properties (2013, background): “S R ] 1 7 M ay 2 01 3 flux ropes (Shibata et al. 1995; Shiota et al. 2005; Priest & Forbes 2002; Amari et al. 2003a,b), and unstable flux ropes (Török et al. 2004; Aulanier et al. 2010).”
- The Role of Magnetic Reconnection in the Observable Features of Solar Eruptions (2004, methodology): “Other models (e.g., Mikić, Barnes, & Schnack 1988; Mikić & Linker 1994; Antiochos, DeVore, & Klimchuk 1999; Amari et al. 2003; Manchester 2003) begin with a sheared magnetic structure that becomes unstable as a result of reconnection (Gosling 1993).”
- The Partial Expulsion of a Magnetic Flux Rope (2006, background): “…a pre-CME flux rope (Wolfson et al. 1987; Low & Hundhausen 1995; Linker et al. 2003; Gibson et al. 2006), as are transient sigmoid brightenings (Rust & Kumar 1996; Fan & Gibson 2003, 2004; Kliem et al. 2004) and their transition to cusped postflare loops (Amari et al. 2003b; To¨rök & Kliem 2005).”
- Confined and Ejective Eruptions of Kink-unstable Flux Ropes (2005, methodology): “They also demonstrate the importance of the height dependence of the overlying field for the evolution of the instability into a CME, while Amari et al. (2003b) found the amount of magnetic helicity to be essential.”
- ELECTRIC CURRENTS IN FLARE RIBBONS: OBSERVATIONS AND THREE-DIMENSIONAL STANDARD MODEL (2014, methodology): “As such, different mechanisms for eruptive flares have been proposed (see Forbes et al. 2006; Amari et al. 2003a, 2003b; Shibata & Magara 2011; Aulanier 2014 and references therein).”
- OBSERVING FLUX ROPE FORMATION DURING THE IMPULSIVE PHASE OF A SOLAR ERUPTION (2011, background): “Considerable efforts have also been made in numerical MHD simulations to study the formation and dynamic behavior of flux ropes (Amari et al. 2000, 2003; Aulanier et al. 2010; Fan & Gibson 2003, 2004).”
- MAGNETIC FIELD STRUCTURES TRIGGERING SOLAR FLARES AND CORONAL MASS EJECTIONS (2012, background): “In fact, the converging flow on the solar surface is believed to play the role of a trigger in the flux cancellation (FC) model (Inhester et al. 1992; Priest et al. 1994; Amari et al. 2003a).”
- Direct Observations of the Magnetic Reconnection Site of an Eruption on 2003 November 18 (2005, methodology): “Of course, the configuration in Figure 1 could also be produced in the processes described by other CME models, such as the sheared-arcade and breakout models (Mikić et al. 1988; Mikić & Linker 1994; Antiochos et al. 1999; Amari et al. 2003; Linker et al. 2003).”
- The Origin, Early Evolution and Predictability of Solar Eruptions (2018, background): “Many examples exist including simulations by Steinolfson (1991); Mikic and Linker (1994); Wolfson (1995); Antiochos et al (1999); Amari et al (2003a); Lynch et al (2008); van der Holst et al (2009), which are successful in reproducing many characteristics of CMEs, filament eruptions and flares.”
- Coronal prominence structure and dynamics: A magnetic flux rope interpretation (2006, background): “D twisted flux rope configurations have also been shown in numerical simulations [Linker et al., 2001; Amari et al., 2000, 2003a, 2004a, 2004b; Toeroek and Kliem, 2003; Kusano et al., 2004; Roussev et al., 2004; Kusano, 2005; Fan, 2005; Toeroek and Kliem, 2005; Fan and Gibson, 2006; Gibson and Fan,…”
- The Physical Processes of CME/ICME Evolution (2017, unknown): “The pre-event magnetic field supporting the filament can also be well described by highly sheared magnetic arcades crossing the PIL (e.g., Mikić et al. 1988; Steinolfson 1991; Antiochos et al. 1999; Amari et al. 2003; Manchester 2003; Lynch et al. 2008; van der Holst et al. 2009).”
- Tracking Vector Magnetograms with the Magnetic Induction Equation (2008, background): “…flux cancellation of the overlying coronal field (Linker et al. 2001), flux injection (Chen 1989, 1996), the kink instability of filaments (Rust & Kumar 1996; Török et al. 2004; Kliem et al. 2004), and photospheric footpoint shearing (Amari et al. 2000, 2003a, 2003b; Schrijver et al. 2005).”
- The Calm before the Storm: The Link between Quiescent Cavities and Coronal Mass Ejections (2006, background): “However, the question of whether the flux rope is formed during the eruption or whether the flux rope existed prior to the eruption remains controversial (Amari et al. 2003).”