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Stereoscopic Observations of an Erupting Mini-filament Driven Two-Sided-Loop Jet and the Applications for Diagnosing Filament Magnetic field

T0 review · 3 major / 6 minor · reviewed 2026-08-14 · deepseek-v4-flash

Pith's one-line read This paper reports that a two-sided-loop solar jet observed on 2013 June 2 was driven by a mini-filament eruption, and that its two arms traced the cavity magnetic field of the overlying filament, giving a 26.7-degree field-angle…

desk verdict A genuinely new stereoscopic view of a two-sided-loop jet, with a careful event analysis but a load-bearing field-line assumption that leaves the headline angle unproven. read the letter →

arxiv 1908.03660 v2 pith:GVUBZ64H submitted 2019-08-10 astro-ph.SR

classification astro-ph.SR
keywords solarjetstwo-sided-loopmini-filamenteruptionsfilamentmagneticfieldsstereoscopicreconstructionreconnection
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

The paper aims to show that a two-sided-loop jet observed on 2013 June 2 formed through the eruption of a mini-filament beneath a large filament, with two separate magnetic reconnection episodes, and that its two arms ran along the magnetic field lines of the large filament's cavity. If true, this contradicts the established picture in which two-sided-loop jets are produced by an emerging magnetic loop reconnecting with horizontal field lines. It also makes the jet a useful tracer: by triangulating the jet's trajectory from two spacecraft viewpoints, the authors measure the angle between the cavity magnetic field and the filament axis to be about 26.7 degrees, consistent with earlier direct spectropolarimetric measurements. This matters because filament magnetic fields are hard to measure directly, and the event also shows the jet supplying cool mass to the overlying filament, a possible route for filament formation.

What carries the argument

The load-bearing mechanism is stereoscopic triangulation of the jet's trajectory combined with the assumption that the jet plasma flows along magnetic field lines. Paired 193 Å SDO/AIA and 195 Å STEREO-A images at 13:10:30 UT are used to reconstruct the three-dimensional curves of the two-sided-loop jet and the filament axis; projecting these curves to the disk center gives the intersection angle. The two-sided-loop jet is the tracer, meaning a pair of plasma beams ejected in opposite directions from the reconnection site. The mini-filament eruption supplies the cool plasma and drives the second reconnection stage.

What would settle it

A decisive check would be to compare the reconstructed jet trajectory with an independent magnetic field model or spectropolarimetric inversion of the same filament: if the jet arms deviate from the field lines by more than the measurement uncertainty, or if another event yields a jet-derived angle that disagrees with the direct measurement by much more than a few degrees, the tracing assumption is falsified.

Watch

Extended reading notes

Core claim

In the SDO images the jet appeared as a concave structure with projection speeds of about 80-136 km/s, while in the STEREO-A images the same eruption appeared as a spiral structure whose two arms lay along the cavity magnetic field lines hosting the large filament. Two reconnection stages are identified: the first between a rising loop and the filament's field, resembling the classical picture; the second between the rising mini-filament and the overlying field, releasing cool material into both arms. The paired images at 13:10:30 UT are reconstructed in three dimensions, and the intersection angle between the jet/cavity trajectory and the filament axis is measured to be about 26.7 degrees. The authors also find that the hot jet component appeared about three minutes before the cool mini-filament material, and they propose a schematic model in which two-sided-loop jets can be mini-filament-driven, with no coronal mass ejection expected.

Load-bearing premise

The entire field-angle measurement rests on the assumption that the two arms of the jet seen in SDO and STEREO-A are the same plasma streams and that the streams move strictly along the magnetic field lines of the large filament's cavity, so that the jet trajectory is a faithful trace of the field.

Editorial extensions

If this is right

  • Two-sided-loop jets can be added to the class of jets driven by mini-filament eruptions, so the classical emerging-loop mechanism is not the only way these jets form.
  • The trajectory of such a jet can be used to map the magnetic field lines of a filament's cavity, giving a diagnostic for filament magnetic structure where direct polarimetric measurements are unavailable.
  • The event provides a direct observational path for cool mass to enter a filament from below, supporting the injection picture of filament mass formation.
  • Two-sided-loop jets are expected not to produce coronal mass ejections, unlike collimated blowout jets, because the overlying field confines the eruption.
  • Such jets may deposit more energy into the corona than collimated blowout jets because their plasma is confined and eruptive.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • If the tracing assumption holds generally, repeated mini-filament-driven two-sided-loop jets beneath different filaments could be used to build maps of prominence magnetic shear without spectropolarimetry.
  • The method could be extended beyond filaments to other coronal structures: any jet whose arms lie along a pre-existing field system is a natural field-line tracer in stereoscopic data.
  • A direct test would be to catch another two-sided-loop jet with simultaneous spectropolarimetric measurements of the overlying filament; the jet-derived angle should match the spectropolarimetric inclination if the method is sound.
  • The proposed model predicts that the cool material in such jets should systematically lag the hot component by minutes and follow the same field lines; high-cadence multi-wavelength observations could check this.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

3 major / 6 minor

Summary. The paper analyzes the 2013 June 2 two-sided-loop jet observed simultaneously by SDO/AIA, HMI, GONG, and STEREO-A. It reports two distinct reconnection episodes during the jet formation, associates the second episode with the eruption of a mini-filament below a large filament, and uses stereoscopic reconstruction of the jet arms at 13:10:30 UT to infer that the arms trace the cavity magnetic field lines of the overlying large filament. From the reconstructed trajectories the authors measure an intersection angle of about 26.7 degrees between the cavity field and the filament axis, which they compare to earlier spectropolarimetric results. The paper proposes that mini-filament eruptions can drive two-sided-loop jets and that such jets can serve as tracers of filament magnetic structure.

Significance. If the inference is correct, the paper provides a new formation mechanism for two-sided-loop jets, challenging the classical emerging-loop picture, and introduces a novel diagnostic for the magnetic structure of solar filaments. The observational evidence for two reconnection episodes is substantial, including time-distance plots, magnetic island signatures, conjugated flare ribbons, and the dark erupting mini-filament material. The simultaneous SDO and STEREO-A observations are an important asset. However, the central quantitative claim, the 26.7-degree intersection angle, rests on an untested field-line-tracing assumption and on a manual single-time reconstruction with no uncertainty analysis. The validation against previous measurements uses a broad range that is not probative. Therefore, while the observational case for a mini-filament-driven two-sided-loop jet is largely sound, the diagnostic application as presented is not yet fully established.

major comments (3)
  1. [Section 2, Figure 5] The three-dimensional reconstruction at 13:10:30 UT is based on manually selected points (red plus signs and blue asterisks) with no stated selection criteria, no number of points, and no uncertainty estimate for the reconstructed trajectories or the resulting 26.7-degree angle. Please provide a quantitative error analysis, for example by varying the input points, repeating the reconstruction at several times, or comparing with an independent triangulation method. Without such an analysis, the angle measurement is not robust and the agreement with earlier measurements cannot be assessed.
  2. [Section 2] The load-bearing assumption that 'the trajectory of the two-sided-loop jet represents the position of the cavity structure' is asserted rather than demonstrated. Since the entire diagnostic depends on this field-line-tracing assumption, please support it with additional evidence, such as a comparison of the reconstructed jet trajectory with a coronal magnetic field model (e.g., PFSS or NLFFF), an argument why plasma inertia and non-ideal effects are negligible, or a cross-check using another tracer of the cavity field. Without this, the measured angle may reflect the jet flow path rather than the magnetic field direction.
  3. [Section 2 and Section 3] The comparison with earlier direct measurements is presented as validation, but the cited range is inconsistent between the two sections (Section 2 says 20–30 degrees; Section 3 says 15–30 degrees) and is too broad to be probative. A measurement of 26.7 degrees could agree with many values in that interval. Please quantify the uncertainty in the 26.7-degree result and state explicitly which published measurements are consistent with it, rather than invoking a wide range.
minor comments (6)
  1. [Abstract] The projection speed is reported as '80 - 136' without units; please write '80–136 km/s'.
  2. [Section 1] In the sentence 'that is (a physical process that breaks and reconnects...' the parenthesis is misplaced, and 'converts to' should be 'converted to'.
  3. [Section 2, first paragraph] The phrase 'The SDO observations reveals' should be 'The SDO observations reveal'.
  4. [Section 3, final paragraph] The phrase 'well agreement' should be 'in good agreement'.
  5. [Section 2, Figure 4 caption] The white dotted curves marking the cavity profile and the disk limbs are described but are not clearly visible in the printed figures; please increase their contrast or add labels so that the reader can verify the correspondence.
  6. [Section 2, reconstruction paragraph] The paper does not describe the co-alignment procedure between SDO and STEREO-A images used for the 3D reconstruction, nor the estimated co-alignment error. Please specify how the two images were coaligned and how uncertainties in this step affect the reconstructed trajectories.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: the 26.7-degree angle is a direct geometric reconstruction, validated against independent spectropolarimetric measurements.

full rationale

The paper's central quantitative result is a geometric measurement: paired SDO/AIA and STEREO-A images at 13:10:30 UT are used to reconstruct the three-dimensional trajectories, and the intersection angle between the reconstructed jet trajectory and the large filament axis is measured to be about 26.7 degrees (Section 2, Figure 5). No parameter is fitted to a target quantity and then renamed as a prediction; the projection speeds in the TDS plots are descriptive kinematic measurements, not predictions derived from the model. The only load-bearing inference is the physical assumption that the jet arms propagate along cavity magnetic field lines, explicitly stated as "Since the two-sided loop jet was along the magnetic field lines of the cavity structure, the trajectory of the two-sided loop jet represents the position of the cavity structure." This is an empirical premise used to interpret the observed trajectory, not a definitional equivalence that makes the conclusion true by construction; if field-line tracing fails it would be a correctness risk, not circularity. The validation against Casini et al. (2003) is an external, independent check, and the self-citations (e.g., Shen et al. 2012, 2017 for the blowout-jet context) are illustrative rather than load-bearing for the 26.7-degree measurement. No equation in the paper reduces to its own input.

Assumptions & free parameters 0 free parameters · 4 assumptions · 0 invented entities

The paper does not introduce new entities or fitted parameters. Its central inference rests on the assumption that the jet arms trace the cavity magnetic field lines, plus standard domain assumptions about reconnection signatures and feature correspondence between the two spacecraft views.

assumptions (4)
  • domain assumption The two-sided-loop jet's trajectory follows the magnetic field lines of the cavity structure.
    Stated in Section 2 and essential for interpreting the 3D reconstruction and the 26.7 degree angle.
  • domain assumption The features identified as current sheets containing magnetic islands represent actual magnetic reconnection.
    Used to claim two distinct reconnection processes; based on morphological similarity to numerical simulations.
  • domain assumption The concave structure in SDO and the spiral structure in STEREO-A are the same physical jet.
    Needed for the stereoscopic 3D reconstruction; the two views differ strongly because of the 140 degree separation.
  • domain assumption The linear fits to the time-distance plots give representative speeds of the jet arms.
    The derived projection speeds are line-of-sight projected and no deprojection or error analysis is provided.

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Cite this review

Pith. "Pith review of Stereoscopic Observations of an Erupting Mini-filament Driven Two-Sided-Loop Jet and the Applications for Diagnosing Filament Magnetic field." pith.science (2026). https://pith.science/paper/GVUBZ64H

@misc{pith2026190803660,
  author       = {Pith},
  title        = {Pith review of: Stereoscopic Observations of an Erupting Mini-filament Driven Two-Sided-Loop Jet and the Applications for Diagnosing Filament Magnetic field},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/GVUBZ64H}},
  note         = {Machine review of arXiv:1908.03660}
}
read the original abstract

The ubiquitous solar jets or jet-like activities are generally regarded as an important source of energy and mass input to the upper solar atmosphere and the solar wind. However, questions about their triggering and driving mechanisms are not completely understood. By taking advantage of high temporal and high spatial resolution stereoscopic observations taken by the Solar Dynamic Observatory (SDO) and the Solar Terrestrial Relations Observatory (STEREO), we report an intriguing two-sided-loop jet occurred on 2013 June 02, which was dynamically associated with the eruption of a mini-filament below an overlying large filament, and two distinct reconnection processes are identified during the formation stage. The SDO observations reveals that the two-sided-loop jet showed a concave shape with a projection speed of about 80 - 136. From the other view angle, the STEREO ahead observations clearly showed that the trajectory of the two arms of the two-sided-loop were along the cavity magnetic field lines hosting the large filament. Contrary to the well-accepted theoretical model, the present observation sheds new light on our understanding of the formation mechanism of two-sided-loop jets. Moreover, the eruption of the two-sided-loop jet not only supplied mass to the overlying large filament, but also provided a rare opportunity to diagnose the magnetic structure of the overlying large filament via the method of three-dimensional reconstruction.

Figures

Figures reproduced from arXiv: 1908.03660 by the authors.

Figure 1
Figure 1. Pre-eruption magnetic configuration. (a) HMI LOS magnetogram in which bright (black) patches are positive (negative) polarities. (b) GONG Hα image shows LF, in which the red (blue) contours indicate the magnetogram in (a) at 100 (-100) Gauss. (c–d) AIA 304 ˚A and 193 ˚A images shows the coronal condition. (e–f) STEREO-A 304 ˚A and 195 ˚A images. The close-up shot of the eruption source region is plotted at the top-r… view at source ↗
Figure 2
Figure 2. Eruption details of the two-sided-loop jet in AIA images. (a1–a3) composite high temperature images made from the AIA 94 ˚A (red), 335 ˚A (green), and 193 ˚A (blue) channels. (b1–b3) composite low temperature images made from the AIA 304 ˚A (red), 211 ˚A (green), and 171 ˚A (blue) channels. (c1–c3) AIA 304 ˚A images. The white arrows in this figure indicate the reconnection current sheet, while the paired blue arrow… view at source ↗
Figure 3
Figure 3. TDS plots along the jet’s main axis and the magnetic flux variations in the eruption source region. (a) composite TDS plot made from AIA high temperature channels (94 ˚A (red), 335 ˚A (green), and 193 ˚A (blue)). (b) composite TDS plot made from AIA low temperature channels (304 ˚A (red), 211 ˚A (green), and 171 ˚A (blue)). The red and blue arrows in (a) indicate the first and the second reconnection processes, and … view at source ↗
Figures from the paper (3 more)
Figure 4
Figure 4. Figure 4: Eruption details of the two-sided-loop jet in STEREO-A and SDO/AIA images. (a1–a3) and (c1–c3) are STEREO-A 195 ˚A and 304 ˚A images, while (b1–b3) and (d1–d3) are AIA 193 ˚A and 304 ˚A images, respectively. The white arrow in (a1) indicates the beginning of the two-si…
Figure 5
Figure 5. Figure 5: Three-dimensional reconstruction of the trajectories of the two-sided-loop jet and the main axis of the LF. Top row shows the paired simultaneous SDO/AIA 193 ˚A and STEREO-A 195 ˚A images at 13:10:30 UT. The middle row shows the projected trajectories of the two-sided-…
Figure 6
Figure 6. Figure 6: Schematic depiction of the eruption processes of collimated blowout jet (top row) and two￾sided-loop jets (bottom row). Here, only a few representative field lines are drawn. The red (blue) patches represent positive (negative) polarities, while the lines represent mag…

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Works this paper leans on

68 extracted references · 54 canonical work pages

  1. [1]

    C., Moore, R

    Adams, M., Sterling, A. C., Moore, R. L., & Gary, G. A. 2014, ApJ, 783, 11

  2. [2]

    1999, SoPh, 190, 167

    Alexander, D., & Fletcher, L. 1999, SoPh, 190, 167

  3. [3]

    2016, ApJ, 823, 129

    Alzate, N., & Morgan, H. 2016, ApJ, 823, 129

  4. [4]

    2003, A&A, 402, 769 Canfield, R

    Aulanier, G., & D´ emoulin, P. 2003, A&A, 402, 769 Canfield, R. C., Reardon, K. P., Leka, K. D., et al. 1996, ApJ, 464, 1016

  5. [5]

    Lites, B. W. 2003, ApJL, 598, L67

  6. [6]

    Chae, J., Qiu, J., Wang, H., & Goode, P. R. 1999, ApJL, 513, L75

  7. [7]

    2018, SoPh, 293, 93

    Chen, H., Yang, J., Yang, B., Ji, K., & Bi, Y. 2018, SoPh, 293, 93

  8. [8]

    2003, in Astronomical Society of the Pacific Conference Series, Vol

    Ramos, A. 2003, in Astronomical Society of the Pacific Conference Series, Vol. 307, Solar Polarization, ed. J. Trujillo-Bueno & J. Sanchez Almeida, 468

Show all 68 references
  1. [9]

    2019, arXiv e-prints, arXiv:1907.07310

    Duan, Y., Shen, Y., Chen, H., & Liang, H. 2019, arXiv e-prints, arXiv:1907.07310

  2. [10]

    1977, SoPh, 52, 37

    Engvold, O., & Jensen, E. 1977, SoPh, 52, 37

  3. [11]

    W., Hill, F., Hubbard, R

    Harvey, J. W., Hill, F., Hubbard, R. P., et al. 1996, Science, 272, 1284

  4. [12]

    2014, ApJ, 796, 73

    Hong, J., Jiang, Y., Yang, J., et al. 2014, ApJ, 796, 73

  5. [13]

    2017, ApJ, 835, 35

    Hong, J., Jiang, Y., Yang, J., Li, H., & Xu, Z. 2017, ApJ, 835, 35

  6. [14]

    2018, ApJL, 853, L26

    Huang, Z., Mou, C., Fu, H., et al. 2018, ApJL, 853, L26

  7. [15]

    2013, ApJ, 775, 132

    Jiang, Y., Bi, Y., Yang, J., et al. 2013, ApJ, 775, 132

  8. [16]

    2008, ApJ, 677, 699

    Jiang, Y., Shen, Y., Yi, B., Yang, J., & Wang, J. 2008, ApJ, 677, 699

  9. [17]

    C., Chen, H

    Jiang, Y. C., Chen, H. D., Li, K. J., Shen, Y. D., & Yang, L. H. 2007, A&A, 469, 331

  10. [18]

    L., Kucera, T

    Kaiser, M. L., Kucera, T. A., Davila, J. M., et al. 2008, SSRv, 136, 5

  11. [19]

    R., Raulin, J.-P., Nitta, N., Shibata, K., & Shimojo, M

    Kundu, M. R., Raulin, J.-P., Nitta, N., Shibata, K., & Shimojo, M. 1998, SoPh, 178, 173

  12. [20]

    R., Title, A

    Lemen, J. R., Title, A. M., Akin, D. J., et al. 2012, SoPh, 275, 17

  13. [21]

    Leroy, J. L. 1989, in Astrophysics and Space Science Library, Vol. 150, Dynamics and Structure of Quiescent Solar Prominences, ed. E. R. Priest, 77–113

  14. [22]

    2019, ApJ, 872, 87

    Li, H., & Yang, J. 2019, ApJ, 872, 87

  15. [23]

    2017, ApJL, 842, L20

    Li, H., Jiang, Y., Yang, J., et al. 2017, ApJL, 842, L20

  16. [24]

    2015, ApJL, 814, L13

    Li, X., Yang, S., Chen, H., Li, T., & Zhang, J. 2015, ApJL, 814, L13

  17. [25]

    E., Title, A

    Liu, W., Berger, T. E., Title, A. M., & Tarbell, T. D. 2009, ApJL, 707, L37

  18. [26]

    2005, ApJL, 631, L93

    Liu, Y., Kurokawa, H., & Shibata, K. 2005, ApJL, 631, L93

  19. [27]

    2010, SSRv, 151, 333

    Schmieder, B., & Aulanier, G. 2010, SSRv, 151, 333

  20. [28]

    B., et al

    Miao, Y., Liu, Y., Li, H. B., et al. 2018, ApJ, 869, 39

  21. [29]

    D., et al

    Miao, Y., Liu, Y., Shen, Y. D., et al. 2019, ApJ, 877, 61

  22. [30]

    Falconer, D. A. 2010, ApJ, 720, 757

  23. [31]

    2012, ApJ, 750, 50

    Neugebauer, M. 2012, ApJ, 750, 50

  24. [32]

    A., & Lin, J

    Ni, L., Zhang, Q.-M., Murphy, N. A., & Lin, J. 2017, ApJ, 841, 27

  25. [33]

    2008, ApJL, 683, L83 Nistic` o, G., Bothmer, V., Patsourakos, S., &

    Nishizuka, N., Shimizu, M., Nakamura, T., et al. 2008, ApJL, 683, L83 Nistic` o, G., Bothmer, V., Patsourakos, S., &

  26. [34]

    2009, SoPh, 259, 87

    Zimbardo, G. 2009, SoPh, 259, 87

  27. [35]

    V., Mason, G

    Nitta, N. V., Mason, G. M., Wiedenbeck, M. E., et al. 2008, ApJL, 675, L125

  28. [36]

    2001, A&A, 375, L39 10 Shen et al

    Semel, M. 2001, A&A, 375, L39 10 Shen et al

  29. [37]

    K., Sterling, A

    Panesar, N. K., Sterling, A. C., & Moore, R. L. 2017, ApJ, 844, 131

  30. [38]

    D., Thompson, B

    Pesnell, W. D., Thompson, B. J., & Chamberlin, P. C. 2012, SoPh, 275, 3

  31. [39]

    C., & Romoli, M

    Pucci, S., Poletto, G., Sterling, A. C., & Romoli, M. 2013, ApJ, 776, 16 Raouafi, N. E., Patsourakos, S., Pariat, E., et al. 2016, SSRv, 201, 1

  32. [40]

    M., & Kumar, A

    Rust, D. M., & Kumar, A. 1994, SoPh, 155, 69

  33. [41]

    Schmieder, B., Golub, L., & Antiochos, S. K. 1994, ApJ, 425, 326

  34. [42]

    F., Liu, Y

    Shen, Y., Chen, P. F., Liu, Y. D., et al. 2019, ApJ, 873, 22

  35. [43]

    2012, ApJ, 745, 164

    Shen, Y., Liu, Y., Su, J., & Deng, Y. 2012, ApJ, 745, 164

  36. [44]

    2011, ApJL, 735, L43

    Shen, Y., Liu, Y., Su, J., & Ibrahim, A. 2011, ApJL, 735, L43

  37. [45]

    D., Su, J., Qu, Z., & Tian, Z

    Shen, Y., Liu, Y. D., Su, J., Qu, Z., & Tian, Z. 2017, ApJ, 851, 67

  38. [46]

    W., et al

    Shibata, K., Ishido, Y., Acton, L. W., et al. 1992, PASJ, 44, L173

  39. [47]

    2007, Science, 318, 1591

    Shibata, K., Nakamura, T., Matsumoto, T., et al. 2007, Science, 318, 1591

  40. [48]

    Dwivedi, B. N. 2019, SoPh, 294, 68

  41. [49]

    Sterling, A. C. 2018, in Journal of Physics Conference Series, Vol. 1100, Journal of Physics Conference Series, 012024

  42. [50]

    Falconer, D. A. 2019, ApJ, 871, 220

  43. [51]

    2015, Nature, 523, 437

    Adams, M. 2015, Nature, 523, 437

  44. [52]

    C., Moore, R

    Sterling, A. C., Moore, R. L., & Panesar, N. K. 2018, ApJ, 864, 68

  45. [53]

    E., Cranmer, S

    Tian, H., DeLuca, E. E., Cranmer, S. R., et al. 2014, Science, 346, 1255711

  46. [54]

    2017, ApJ, 845, 94

    Tian, Z., Liu, Y., Shen, Y., et al. 2017, ApJ, 845, 94

  47. [55]

    2018, ApJ, 863, 180

    Wang, J., Yan, X., Qu, Z., et al. 2018, ApJ, 863, 180

  48. [56]

    1999, ApJL, 520, L71

    Wang, Y.-M. 1999, ApJL, 520, L71

  49. [57]

    Wang, Y.-M., Pick, M., & Mason, G. M. 2006, ApJ, 639, 495

  50. [58]

    R., Socker, D

    Wang, Y.-M., Sheeley, Jr., N. R., Socker, D. G., et al. 1998, ApJ, 508, 899

  51. [59]

    F., & Keppens, R

    Xia, C., Chen, P. F., & Keppens, R. 2012, ApJL, 748, L26

  52. [60]

    F., Keppens, R., & van Marle, A

    Xia, C., Chen, P. F., Keppens, R., & van Marle, A. J. 2011, ApJ, 737, 27

  53. [61]

    2014, ApJL, 792, L38

    Xia, C., Keppens, R., Antolin, P., & Porth, O. 2014, ApJL, 792, L38

  54. [62]

    L., Priest, E

    Yan, X. L., Priest, E. R., Guo, Q. L., et al. 2016, ApJ, 832, 23

  55. [63]

    2015, ApJ, 803, 86

    Yang, B., Jiang, Y., Yang, J., Hong, J., & Xu, Z. 2015, ApJ, 803, 86

  56. [64]

    1995, Nature, 375, 42

    Yokoyama, T., & Shibata, K. 1995, Nature, 375, 42

  57. [65]

    2014, ARA&A, 52, 529

    Yuan, F., & Narayan, R. 2014, ARA&A, 52, 529

  58. [66]

    M., & Ni, L

    Zhang, Q. M., & Ni, L. 2019, ApJ, 870, 113

  59. [67]

    2017, ApJ, 834, 79

    Zhang, Y., & Zhang, J. 2017, ApJ, 834, 79

  60. [68]

    2018, ApJ, 861, 108 An Erupting Mini-filament Driven Two-Sided-Loop Jet 11 Figure 1

    Zheng, R., Chen, Y., Huang, Z., et al. 2018, ApJ, 861, 108 An Erupting Mini-filament Driven Two-Sided-Loop Jet 11 Figure 1. Pre-eruption magnetic configuration. (a) HMI LOS magnetogr am in which bright (black) patches are positive (negative) polarities. (b) GONG H α image shows...

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