Articles | Volume 39, issue 3
https://doi.org/10.5194/angeo-39-455-2021
© Author(s) 2021. This work is distributed under
the Creative Commons Attribution 4.0 License.
the Creative Commons Attribution 4.0 License.
https://doi.org/10.5194/angeo-39-455-2021
© Author(s) 2021. This work is distributed under
the Creative Commons Attribution 4.0 License.
the Creative Commons Attribution 4.0 License.
Ionospheric control of space weather
Office Geophysik, Ogoori, 838-0141, Japan
Related authors
Osuke Saka
EGUsphere, https://doi.org/10.5194/egusphere-2025-716, https://doi.org/10.5194/egusphere-2025-716, 2025
This preprint is open for discussion and under review for Annales Geophysicae (ANGEO).
Short summary
Short summary
Negatively charged solitary potential areas (ion holes) are generated in collisional ionosphere by the incident energetic electrons. Those negative potential regions are ionospheric driver of discrete aurora. When the ion hole becomes sheet-like structure (auroral arc), shear flows develop in the sheet to form spirals.
Osuke Saka
Ann. Geophys. Discuss., https://doi.org/10.5194/angeo-2023-32, https://doi.org/10.5194/angeo-2023-32, 2023
Manuscript not accepted for further review
Short summary
Short summary
Auroral spirals known as northern lights are a spectacular light show in the polar night sky. Internal processes in the polar ionosphere initiate northern lights by producing charge separations along the field lines. Parallel electric fields generated above the ionosphere by charge separations are steady-state electric fields. They occasionally discharge to produce northern lights, analogous to lightning flash in a thunderstorm.
Osuke Saka
Ann. Geophys., 41, 369–373, https://doi.org/10.5194/angeo-41-369-2023, https://doi.org/10.5194/angeo-41-369-2023, 2023
Short summary
Short summary
Transverse electric fields transmitted from the magnetosphere and those generated by the neutral winds yield a local breakdown of the charge neutrality at the boundaries between the thermosphere and mesosphere. The breakdown may create parallel electric fields in the thermosphere to produce spiral auroras and outflows. This explanation supposes an auroral generator located not in a distant space, but rather in our much nearer upper atmosphere.
Osuke Saka
Ann. Geophys. Discuss., https://doi.org/10.5194/angeo-2021-66, https://doi.org/10.5194/angeo-2021-66, 2021
Revised manuscript not accepted
Short summary
Short summary
Auroral spirals known as northern lights are a spectacular light show in the polar night sky. We show that auroral spirals are produced in the polar ionosphere by the internal processes that ensure quasi-neutral equilibrium of the polar ionosphere which is often violated during field line dipolarization. The internal driver produces spiral auroras in a manner different from the field line mapping scenario.
Osuke Saka
Ann. Geophys., 38, 467–479, https://doi.org/10.5194/angeo-38-467-2020, https://doi.org/10.5194/angeo-38-467-2020, 2020
Short summary
Short summary
The first 10 min interval of Pi2 onset is the most active period of substorms composed of field line deformations associated with an increase in curvature radius of flux tubes and their longitudinal expansion. The flux tube deformations were triggered by the ballooning instability of slow magnetoacoustic waves upon arrival of the dipolarization front from the tail. They preceded the classical dipolarization caused by the reduction of cross-tail currents and resulting pileup of the field lines.
Osuke Saka
Ann. Geophys., 37, 381–387, https://doi.org/10.5194/angeo-37-381-2019, https://doi.org/10.5194/angeo-37-381-2019, 2019
Short summary
Short summary
Flow channel extending in north–south directions is produced in the initial pulse of Pi2 pulsations associated with the field line dipolarization. Drifts in the ionosphere of the order of kilometers per second accumulated plasmas at the low-latitude end of the flow channel. The plasma compression in the ionosphere produced field-aligned currents, parallel electric fields, and auroral expansion. We called the compressive ionosphere a "dynamic ionosphere".
O. Saka, K. Hayashi, and M. Thomsen
Ann. Geophys., 32, 1011–1023, https://doi.org/10.5194/angeo-32-1011-2014, https://doi.org/10.5194/angeo-32-1011-2014, 2014
Osuke Saka
EGUsphere, https://doi.org/10.5194/egusphere-2025-716, https://doi.org/10.5194/egusphere-2025-716, 2025
This preprint is open for discussion and under review for Annales Geophysicae (ANGEO).
Short summary
Short summary
Negatively charged solitary potential areas (ion holes) are generated in collisional ionosphere by the incident energetic electrons. Those negative potential regions are ionospheric driver of discrete aurora. When the ion hole becomes sheet-like structure (auroral arc), shear flows develop in the sheet to form spirals.
Osuke Saka
Ann. Geophys. Discuss., https://doi.org/10.5194/angeo-2023-32, https://doi.org/10.5194/angeo-2023-32, 2023
Manuscript not accepted for further review
Short summary
Short summary
Auroral spirals known as northern lights are a spectacular light show in the polar night sky. Internal processes in the polar ionosphere initiate northern lights by producing charge separations along the field lines. Parallel electric fields generated above the ionosphere by charge separations are steady-state electric fields. They occasionally discharge to produce northern lights, analogous to lightning flash in a thunderstorm.
Osuke Saka
Ann. Geophys., 41, 369–373, https://doi.org/10.5194/angeo-41-369-2023, https://doi.org/10.5194/angeo-41-369-2023, 2023
Short summary
Short summary
Transverse electric fields transmitted from the magnetosphere and those generated by the neutral winds yield a local breakdown of the charge neutrality at the boundaries between the thermosphere and mesosphere. The breakdown may create parallel electric fields in the thermosphere to produce spiral auroras and outflows. This explanation supposes an auroral generator located not in a distant space, but rather in our much nearer upper atmosphere.
Osuke Saka
Ann. Geophys. Discuss., https://doi.org/10.5194/angeo-2021-66, https://doi.org/10.5194/angeo-2021-66, 2021
Revised manuscript not accepted
Short summary
Short summary
Auroral spirals known as northern lights are a spectacular light show in the polar night sky. We show that auroral spirals are produced in the polar ionosphere by the internal processes that ensure quasi-neutral equilibrium of the polar ionosphere which is often violated during field line dipolarization. The internal driver produces spiral auroras in a manner different from the field line mapping scenario.
Osuke Saka
Ann. Geophys., 38, 467–479, https://doi.org/10.5194/angeo-38-467-2020, https://doi.org/10.5194/angeo-38-467-2020, 2020
Short summary
Short summary
The first 10 min interval of Pi2 onset is the most active period of substorms composed of field line deformations associated with an increase in curvature radius of flux tubes and their longitudinal expansion. The flux tube deformations were triggered by the ballooning instability of slow magnetoacoustic waves upon arrival of the dipolarization front from the tail. They preceded the classical dipolarization caused by the reduction of cross-tail currents and resulting pileup of the field lines.
Osuke Saka
Ann. Geophys., 37, 381–387, https://doi.org/10.5194/angeo-37-381-2019, https://doi.org/10.5194/angeo-37-381-2019, 2019
Short summary
Short summary
Flow channel extending in north–south directions is produced in the initial pulse of Pi2 pulsations associated with the field line dipolarization. Drifts in the ionosphere of the order of kilometers per second accumulated plasmas at the low-latitude end of the flow channel. The plasma compression in the ionosphere produced field-aligned currents, parallel electric fields, and auroral expansion. We called the compressive ionosphere a "dynamic ionosphere".
O. Saka, K. Hayashi, and M. Thomsen
Ann. Geophys., 32, 1011–1023, https://doi.org/10.5194/angeo-32-1011-2014, https://doi.org/10.5194/angeo-32-1011-2014, 2014
Related subject area
Subject: Earth's ionosphere & aeronomy | Keywords: Ionosphere–magnetosphere interactions
Ionospheric upwelling and the level of associated noise at solar minimum
Three principal components describe the spatiotemporal development of mesoscale ionospheric equivalent currents around substorm onsets
Parallel electric fields produced by ionospheric injection
A comparison of Jason-2 plasmasphere electron content measurements with ground-based measurements
Multi-instrument observations of polar cap patches and traveling ionospheric disturbances generated by solar wind Alfvén waves coupling to the dayside magnetosphere
Responses of intermediate layers to geomagnetic activity during the 2009 deep solar minimum over the Brazilian low-latitude sector
Whistler waves produced by monochromatic currents in the low nighttime ionosphere
Swarm field-aligned currents during a severe magnetic storm of September 2017
Timothy Wemimo David, Chizurumoke Michael Michael, Darren Wright, Adetoro Temitope Talabi, and Abayomi Ekundayo Ajetunmobi
Ann. Geophys., 42, 349–354, https://doi.org/10.5194/angeo-42-349-2024, https://doi.org/10.5194/angeo-42-349-2024, 2024
Short summary
Short summary
The Earth’s upper atmospheres are dominated by matter also known as plasma. These plasmas can flow from the lower region, the ionosphere, to the further-up region, the magnetosphere, which is described as upwelling. We analyse data for ionospheric upwelling over the solar minimum period. A main finding is that the noise or rejected data in the dataset were predominant around the local evening and in winter and minimum around local noon and in summer.
Liisa Juusola, Ari Viljanen, Noora Partamies, Heikki Vanhamäki, Mirjam Kellinsalmi, and Simon Walker
Ann. Geophys., 41, 483–510, https://doi.org/10.5194/angeo-41-483-2023, https://doi.org/10.5194/angeo-41-483-2023, 2023
Short summary
Short summary
At times when auroras erupt on the sky, the magnetic field surrounding the Earth undergoes rapid changes. On the ground, these changes can induce harmful electric currents in technological conductor networks, such as powerlines. We have used magnetic field observations from northern Europe during 28 such events and found consistent behavior that can help to understand, and thus predict, the processes that drive auroras and geomagnetically induced currents.
Osuke Saka
Ann. Geophys., 41, 369–373, https://doi.org/10.5194/angeo-41-369-2023, https://doi.org/10.5194/angeo-41-369-2023, 2023
Short summary
Short summary
Transverse electric fields transmitted from the magnetosphere and those generated by the neutral winds yield a local breakdown of the charge neutrality at the boundaries between the thermosphere and mesosphere. The breakdown may create parallel electric fields in the thermosphere to produce spiral auroras and outflows. This explanation supposes an auroral generator located not in a distant space, but rather in our much nearer upper atmosphere.
Andrew J. Mazzella Jr. and Endawoke Yizengaw
Ann. Geophys., 41, 269–280, https://doi.org/10.5194/angeo-41-269-2023, https://doi.org/10.5194/angeo-41-269-2023, 2023
Short summary
Short summary
Global Positioning System (GPS) measurements of plasmasphere electron content (PEC) by Jason-2 are compared to PEC for ground-based GPS receivers in Africa. Jason-2 vertical PEC measurements corroborated the ground-based measurements, and its co-aligned slant PEC values were generally close to the ground-based slant PEC values. This correspondence indicates that the Jason-2 PEC measurements could be used to resolve some ambiguities in the determination of the ground-based PEC values.
Paul Prikryl, Robert G. Gillies, David R. Themens, James M. Weygand, Evan G. Thomas, and Shibaji Chakraborty
Ann. Geophys., 40, 619–639, https://doi.org/10.5194/angeo-40-619-2022, https://doi.org/10.5194/angeo-40-619-2022, 2022
Short summary
Short summary
The solar wind interaction with Earth’s magnetic field deposits energy into the upper portion of the atmosphere at high latitudes. The coupling process that modulates the ionospheric convection and intensity of ionospheric currents leads to formation of densely ionized patches convecting across the polar cap. The ionospheric currents launch traveling ionospheric disturbances (TIDs) propagating equatorward. The polar cap patches and TIDs are then observed by networks of radars and GPS receivers.
Ângela M. Santos, Christiano G. M. Brum, Inez S. Batista, José H. A. Sobral, Mangalathayil A. Abdu, and Jonas R. Souza
Ann. Geophys., 40, 259–269, https://doi.org/10.5194/angeo-40-259-2022, https://doi.org/10.5194/angeo-40-259-2022, 2022
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Using the Digisonde data this paper shows that the small variation in the geomagnetic activity during low solar activity can affect both the parameter of height and the frequency of the intermediate layer (ILs) over the low-latitude Brazilian sector. The most expressive responses of the ILs to geomagnetic activity were observed during the summer when the height of the ILs suffered a significant decrease with the increase of the magnetic activity magnetic in the first hours of the day.
Vera G. Mizonova and Peter A. Bespalov
Ann. Geophys., 39, 479–486, https://doi.org/10.5194/angeo-39-479-2021, https://doi.org/10.5194/angeo-39-479-2021, 2021
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The paper discusses the excitation of monochromatic ELF/VLF electromagnetic waves produced by HF heating facility currents in the nighttime ionosphere. The ground-based magnetic field is predominantly located under the source, and the wave has right-hand polarization typical for a whistler but left-hand polarization at large distances from the source. About half of the source energy propagates upward, and approximately 20 % propagates to the Earth–ionosphere waveguide.
Renata Lukianova
Ann. Geophys., 38, 191–206, https://doi.org/10.5194/angeo-38-191-2020, https://doi.org/10.5194/angeo-38-191-2020, 2020
Short summary
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During the most intense storm of solar cycle 24, the magnetosphere–ionosphere interaction, which is primarily associated with field-aligned currents (FACs), was much stronger than usual. Measurements onboard the low-latitude polar-orbiting Swarm satellites have shown that the intensities of FACs increase dramatically during the storm-time substorms. The extreme values of 1 s (7.5 km width) FACs reach 80 μA m−2. The lowest latitude of the FAC region is limited to 49–50 MLat.
Cited articles
Alfven, H. and Falthammar, C.-G.: Cosmical Electrodynamics, 2nd Edn.,
Oxford University Press, New York, 1963.
Artemyev, A. V., Angelopoulos, A., Runov, A., and Zelenyi, L. M.: Earthward
electric field and its reversal in the near-Earth current sheet, J. Geophys.
Res., 121, 10803–10812, https://doi.org/10.1002/2016JA023200, 2016.
Baker, D. N., Pulkkinen, T. I., Angelopoulos, V., Baumjohann, W., and
McPherron, R. L.: Neutral line model of substorms: Past results and present
view, J. Geophys. Res., 101, 12795–130010, 1996.
Birn, J., Hesse, M., Haerendel, G., Baumjohann, W., and Shiokawa, K.: Flow
braking and the substorm current wedge, J. Geophys. Res., 104, 19895–19903,
1999.
Birn, J., Raeder, J., Wang, Y. L., Wolf, R. A., and Hesse, M.: On the propagation of bubbles in the geomagnetic tail, Ann. Geophys., 22, 1773–1786, https://doi.org/10.5194/angeo-22-1773-2004, 2004.
Chiu, Y. T. and Schulz, M.: Self-consistent particle and parallel
electrostatic field distributions in the magnetospheric-ionospheric auroral
region, J. Geophys. Res., 83, 629–642, 1978.
Erickson, G. M., Spiro, R. W., and Wolf, R. A.: The physics of the Harang
discontinuity, J. Geophys. Res., 96, 1633–1645, 1991.
Liu, J., Angelopoulos, V., Zhou, X.-Z., and Runov, A.: Magnetic flux
transport by dipolarizing flux bundles, J. Geophys. Res., 119, 909–926,
https://doi.org/10.1002/2013JA019395, 2014.
Liu, W. W. and Liang, J.: Disruption of magnetospheric current sheet by quasi-electrostatic field, Ann. Geophys., 27, 1941–1950, https://doi.org/10.5194/angeo-27-1941-2009, 2009.
Liu, W. W. and Rostoker, G.: Effects of dawn-dusk pressure asymmetry on
convection in the central plasma sheet, J. Geophys. Res., 96, 11501–11512,
1991.
Lui, A. T. Y.: Current disruption in the Earth's magnetosphere: Observations
and models, J. Geophys. Res., 101, 13067–13088, 1996.
McPherron, R. L., Russell, C. T., and Aubry, M. P.: Satellite studies of
magnetospheric substorms on August 15, 1968: 9. Phenomenological model for
substorms, J. Geophys. Res., 78, 3131–3148, 1973.
Nagai, T.: An empirical model of substorm-related magnetic field variations
at synchronous orbit, Magnetospheric substorms, Geophysical Monograph, 64,
edited by: Kan, J. R., Potemra, T. A., Kokubun, S., and Iijima, T., 91–95, American Geophysical Union, Washington DC, 1991.
Newell, P. T., Meng, C. I., and Lyons, K. M.: Suppression of discrete aurorae
by sunlight, Nature, 381, 766–767, 1996.
Nielsen, E. and Greenwald, R. A.: Variations in ionospheric currents and
electric fields in association with absorption spikes during substorm
expansion phase, J. Geophys. Res., 83, 5645–5654, 1978.
Oguti, T.: Similarity between global auroral deformations in DAPP
photographs and small scale deformations observed by a TV camera, J. Atmos.
Terr. Phys., 37, 1413–1418, 1975a.
Oguti, T.: Metamorphoses of aurora, Memoirs of NIPR, series A, 12, National Institute of Polar Research, Tokyo, 1975b.
Persson, H.: Electric field along a magnetic line of force in a low-density
plasma, Phys. Fluids, 6, 1756–1759, 1963.
Roux, A., Perraut, S., Robert, P., Morane, A., Pedersen, A., Korth, A.,
Kremser, G., Aparicio, B., Rodgers, D., and Pellinen, R.: Plasma sheet
instability related to the westward traveling surge, J. Geophys. Res., 96,
17697–17714, 1991.
Runov, A., Angelopoulos, V., Zhou, X.-Z., Zhang, X.-J., Li, S., Plaschke,
F., and Bonnell, J.: A THEMIS multicase study of dipolarization fronts in
the magnetotail plasma sheet, J. Geophys. Res., 116, A05216,
https://doi.org/10.1029/2010JA016316, 2011.
Saka, O.: A new scenario applying traffic flow analogy to poleward expansion of auroras, Ann. Geophys., 37, 381–387, https://doi.org/10.5194/angeo-37-381-2019, 2019.
Saka, O.: The increase in the curvature radius of geomagnetic field lines preceding a classical dipolarization, Ann. Geophys., 38, 467–479, https://doi.org/10.5194/angeo-38-467-2020, 2020.
Saka, O., Hayashi, K., and Thomsen, M.: First 10 min intervals of Pi2 onset
at geosynchronous altitudes during the expansion of energetic ion regions in
the nighttime sector, J. Atmos. Sol.-Terr. Phy., 72, 1100–1109, 2010.
Stern, D. P.: One-dimensional models of quasi-neutral parallel electric
fields, J. Geophys. Res., 86, 5839–5860, 1981.
Tanaka, T., Nakamizo, A., Yoshikawa, A., Fujita, S., Shinagawa, H., Shimazu,
H., Kikuchi, T., and Hashimoto, K.: Substorm convection and current system
deduced from the global simulation, J. Geophys. Res., 115, A05220,
https://doi.org/10.1029/2009JA014676, 2010.
Wahlund, J.-E., Opgenoorth, H. J., Haggstrom, I., Winser, K. J., and Jones,
G. O.: EISCAT observations of topside ionospheric outflows during auroral
activity: revisited, J. Geophys. Res., 97, 3019–3017, 1992.
Short summary
The ionosphere is a partly ionized medium above the atmosphere. Because of its anisotropic properties, the imposed electric fields from the magnetosphere produce space charge. Polarization electric fields induced in the ionosphere by this process generate ion drifts (Pedersen currents) and plasma evaporation along the field lines, thus achieving a quasi-neutral equilibrium of the ionosphere. The evaporation grows as a large-scale parallel potential structure in the magnetosphere.
The ionosphere is a partly ionized medium above the atmosphere. Because of its anisotropic...