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Rapid Rotation of an Erupting Prominence and the Associated Coronal Mass Ejection on 13 May 2013

Solar and Stellar Astrophysics · Submitted 1 Feb 2023

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim Therefore, the prominence eruption is most probably triggered by kink instability.

how it is stated · hedged possibility 0.99 read the record →

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arXiv ID2302.00212 (version 1)
Pith IDA2I42D7K, Pith's permanent record of this paper and its review
CitationHaisheng Ji, Qingmin Zhang, Yuhao Zhou. "Rapid Rotation of an Erupting Prominence and the Associated Coronal Mass Ejection on 13 May 2013." arXiv:2302.00212 (2023). https://pith.science/paper/A2I42D7K
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 10,412 input tokens.

What the abstract itself states, as probabilities: claims first 0.02 · states limitation 0.06 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.99 · compares with prior results 0.09 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

In this paper, we report the multiwavelength observations of an erupting prominence and the associated CME on 13 May 2013. The event occurs behind the western limb in the field of view of SDO/AIA. The prominence is supported by a highly twisted magnetic flux rope and shows rapid rotation in the counterclockwise direction during the rising motion. The rotation of the prominence lasts for $\sim$47 minutes. The average period, angular speed, and linear speed are $\sim$806 s, $\sim$0.46 rad min$^{-1}$, and $\sim$355 km s$^{-1}$, respectively. The total twist angle reaches $\sim$7$\pi$, which is considerably larger than the threshold for kink instability. Writhing motion during 17:42$-$17:46 UT is clearly observed by SWAP in 174 {\AA} and EUVI on board the behind STEREO spacecraft in 304 {\AA} after reaching an apparent height of $\sim$405\,Mm. Therefore, the prominence eruption is most probably triggered by kink instability. A pair of conjugate flare ribbons and post-flare loops are created and observed by STA/EUVI. The onset time of writhing motion is consistent with the commencement of the impulsive phase of the related flare. The 3D morphology and positions of the associated CME are derived using the graduated cylindrical shell (GCS) modeling. The kinetic evolution of the reconstructed CME is divided into a slow-rise phase ($\sim$330 km s$^{-1}$) and a fast-rise phase ($\sim$1005 km s$^{-1}$) by the writhing motion. The edge-on angular width of the CME is a constant (60$^{\circ}$), while the face-on angular width increases from 96$^{\circ}$ to 114$^{\circ}$, indicating a lateral expansion. The latitude of the CME source region decreases slightly from $\sim$18$^{\circ}$ to $\sim$13$^{\circ}$, implying an equatorward deflection during propagation.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 In this paper, we report the multiwavelength observations of an erupting prominence and the associated CME on 13 May 2013. contribution 1.00 0.92 0.02 asserted 0.96
s1 The event occurs behind the western limb in the field of view of SDO/AIA. result 0.39 0.71 0.01 asserted 1.00
s2 The prominence is supported by a highly twisted magnetic flux rope and shows rapid rotation in the counterclockwise direction during the rising motion. result 1.00 0.86 0.08 asserted 1.00
s3 The rotation of the prominence lasts for $\sim$47 minutes. result 1.00 0.92 0.03 asserted 1.00
s4 The average period, angular speed, and linear speed are $\sim$806 s, $\sim$0.46 rad min$^{-1}$, and $\sim$355 km s$^{-1}$, respectively. result 1.00 0.93 0.04 asserted 1.00
s5 The total twist angle reaches $\sim$7$\pi$, which is considerably larger than the threshold for kink instability. result 0.95 0.89 0.08 asserted 1.00
s6 Writhing motion during 17:42$-$17:46 UT is clearly observed by SWAP in 174 {\AA} and EUVI on board the behind STEREO spacecraft in 304 {\AA} after reaching an apparent height of $\sim$405\,Mm. result 0.98 0.90 0.03 asserted 1.00
s7 Therefore, the prominence eruption is most probably triggered by kink instability. interpretation 1.00 0.75 0.69 hedged possibility 0.99
s8 A pair of conjugate flare ribbons and post-flare loops are created and observed by STA/EUVI. result 1.00 0.87 0.03 asserted 1.00
s9 The onset time of writhing motion is consistent with the commencement of the impulsive phase of the related flare. result 0.93 0.88 0.04 hedged possibility 0.62
s10 The 3D morphology and positions of the associated CME are derived using the graduated cylindrical shell (GCS) modeling. method 0.98 0.95 0.03 asserted 1.00
s11 The kinetic evolution of the reconstructed CME is divided into a slow-rise phase ($\sim$330 km s$^{-1}$) and a fast-rise phase ($\sim$1005 km s$^{-1}$) by the writhing motion. result 0.99 0.93 0.06 asserted 1.00
s12 The edge-on angular width of the CME is a constant (60$^{\circ}$), while the face-on angular width increases from 96$^{\circ}$ to 114$^{\circ}$, indicating a lateral expansion. result 0.99 0.94 0.04 asserted 0.87
s13 The latitude of the CME source region decreases slightly from $\sim$18$^{\circ}$ to $\sim$13$^{\circ}$, implying an equatorward deflection during propagation. result 0.72 0.91 0.05 hedged possibility 0.70

What kind of paper the classifier reports this is: empirical study 1.00 · evidence from observation or experiment 0.81.

What was examined, and what was not

sources read
  • arXiv listing abstract v1
not examined
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  • references and citing sentences
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  • P abstract
not run
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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

In this paper, we report the multiwavelength observations of an erupting prominence and the associated CME on 13 May 2013. The event occurs behind the western limb in the field of view of SDO/AIA. The prominence is supported by a highly twisted magnetic flux rope and shows rapid rotation in the counterclockwise direction during the rising motion. The rotation of the prominence lasts for $\sim$47 minutes. The average period, angular speed, and linear speed are $\sim$806 s, $\sim$0.46 rad min$^{-1}$, and $\sim$355 km s$^{-1}$, respectively. The total twist angle reaches $\sim$7$\pi$, which is considerably larger than the threshold for kink instability. Writhing motion during 17:42$-$17:46 UT is clearly observed by SWAP in 174 {\AA} and EUVI on board the behind STEREO spacecraft in 304 {\AA} after reaching an apparent height of $\sim$405\,Mm. Therefore, the prominence eruption is most probably triggered by kink instability. A pair of conjugate flare ribbons and post-flare loops are created and observed by STA/EUVI. The onset time of writhing motion is consistent with the commencement of the impulsive phase of the related flare. The 3D morphology and positions of the associated CME are derived using the graduated cylindrical shell (GCS) modeling. The kinetic evolution of the reconstructed CME is divided into a slow-rise phase ($\sim$330 km s$^{-1}$) and a fast-rise phase ($\sim$1005 km s$^{-1}$) by the writhing motion. The edge-on angular width of the CME is a constant (60$^{\circ}$), while the face-on angular width increases from 96$^{\circ}$ to 114$^{\circ}$, indicating a lateral expansion. The latitude of the CME source region decreases slightly from $\sim$18$^{\circ}$ to $\sim$13$^{\circ}$, implying an equatorward deflection during propagation.

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