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Dive into the research topics where Philip J. Erickson is active.

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Featured researches published by Philip J. Erickson.


Journal of Geophysical Research | 2005

Multiradar observations of the polar tongue of ionization

J. C. Foster; Anthea J. Coster; Philip J. Erickson; J. M. Holt; Frank D. Lind; William C. Rideout; M. A. McCready; A. van Eyken; R. J. Barnes; R. A. Greenwald; F. J. Rich

[1] We present a global view of large-scale ionospheric disturbances during the main phase of a major geomagnetic storm. We find that the low-latitude, auroral, and polar latitude regions are coupled by processes that redistribute thermal plasma throughout the system. For the large geomagnetic storm on 20 November 2003, we examine data from the high-latitude incoherent scatter radars at Millstone Hill, Sondrestrom, and EISCAT Tromso, with SuperDARN HF radar observations of the high-latitude convection pattern and DMSP observations of in situ plasma parameters in the topside ionosphere. We combine these with north polar maps of stormtime plumes of enhanced total electron content (TEC) derived from a network of GPS receivers. The polar tongue of ionization (TOI) is seen to be a continuous stream of dense cold plasma entrained in the global convection pattern. The dayside source of the TOI is the plume of storm enhanced density (SED) transported from low latitudes in the postnoon sector by the subauroral disturbance electric field. Convection carries this material through the dayside cusp and across the polar cap to the nightside where the auroral F region is significantly enhanced by the SED material. The three incoherent scatter radars provided full altitude profiles of plasma density, temperatures, and vertical velocity as the TOI plume crossed their different positions, under the cusp, in the center of the polar cap, and at the midnight oval/polar cap boundary. Greatly elevated F peak density (>1.5E12 m 3 ) and low electron and ion temperatures (2500 K at the F peak altitude) characterize the SED/TOI plasma observed at all points along its high-latitude trajectory. For this event, SED/TOI F region TEC (150–1000 km) was 50 TECu both in the cusp and in the center of the polar cap. Large, upward directed fluxes of O+ (>1.E14 m 2 s 1 ) were observed in the topside ionosphere


Publications of the Astronomical Society of Australia | 2013

Science with the Murchison Widefield Array

Judd D. Bowman; Iver H. Cairns; David L. Kaplan; Tara Murphy; Divya Oberoi; Lister Staveley-Smith; W. Arcus; David G. Barnes; G. Bernardi; F. Briggs; Shea Brown; John D. Bunton; Adam J. Burgasser; R. J. Cappallo; Shami Chatterjee; B. E. Corey; Anthea J. Coster; Avinash A. Deshpande; L. deSouza; D. Emrich; Philip J. Erickson; R. Goeke; B. M. Gaensler; L. J. Greenhill; L. Harvey-Smith; B. J. Hazelton; David Herne; Jacqueline N. Hewitt; M. Johnston-Hollitt; J. Kasper

Significant new opportunities for astrophysics and cosmology have been identified at low radio frequencies. The Murchison Widefield Array is the first telescope in the southern hemisphere designed specifically to explore the low-frequency astronomical sky between 80 and 300 MHz with arcminute angular resolution and high survey efficiency. The telescope will enable new advances along four key science themes, including searching for redshifted 21-cm emission from the EoR in the early Universe; Galactic and extragalactic all-sky southern hemisphere surveys; time-domain astrophysics; and solar, heliospheric, and ionospheric science and space weather. The Murchison Widefield Array is located in Western Australia at the site of the planned Square Kilometre Array (SKA) low-band telescope and is the only low-frequency SKA precursor facility. In this paper, we review the performance properties of the Murchison Widefield Array and describe its primary scientific objectives.


Nature | 2014

An impenetrable barrier to ultrarelativistic electrons in the Van Allen radiation belts

D. N. Baker; A. N. Jaynes; V. C. Hoxie; Richard M. Thorne; J. C. Foster; X. Li; J. F. Fennell; J. R. Wygant; Shrikanth G. Kanekal; Philip J. Erickson; W. S. Kurth; W. Li; Q. Ma; Q. Schiller; L. W. Blum; D. M. Malaspina; Andrew J. Gerrard; L. J. Lanzerotti

Early observations indicated that the Earth’s Van Allen radiation belts could be separated into an inner zone dominated by high-energy protons and an outer zone dominated by high-energy electrons. Subsequent studies showed that electrons of moderate energy (less than about one megaelectronvolt) often populate both zones, with a deep ‘slot’ region largely devoid of particles between them. There is a region of dense cold plasma around the Earth known as the plasmasphere, the outer boundary of which is called the plasmapause. The two-belt radiation structure was explained as arising from strong electron interactions with plasmaspheric hiss just inside the plasmapause boundary, with the inner edge of the outer radiation zone corresponding to the minimum plasmapause location. Recent observations have revealed unexpected radiation belt morphology, especially at ultrarelativistic kinetic energies (more than five megaelectronvolts). Here we analyse an extended data set that reveals an exceedingly sharp inner boundary for the ultrarelativistic electrons. Additional, concurrently measured data reveal that this barrier to inward electron radial transport does not arise because of a physical boundary within the Earth’s intrinsic magnetic field, and that inward radial diffusion is unlikely to be inhibited by scattering by electromagnetic transmitter wave fields. Rather, we suggest that exceptionally slow natural inward radial diffusion combined with weak, but persistent, wave–particle pitch angle scattering deep inside the Earth’s plasmasphere can combine to create an almost impenetrable barrier through which the most energetic Van Allen belt electrons cannot migrate.


Geophysical Research Letters | 2014

Gradual diffusion and punctuated phase space density enhancements of highly relativistic electrons: Van Allen Probes observations

D. N. Baker; A. N. Jaynes; X. Li; M. G. Henderson; S. G. Kanekal; G. D. Reeves; Harlan E. Spence; S. G. Claudepierre; J. F. Fennell; M. K. Hudson; Richard M. Thorne; J. C. Foster; Philip J. Erickson; D. M. Malaspina; J. R. Wygant; A. J. Boyd; C. A. Kletzing; A. Drozdov; Y. Y. Shprits

The dual-spacecraft Van Allen Probes mission has provided a new window into mega electron volt (MeV) particle dynamics in the Earths radiation belts. Observations (up to E ~10 MeV) show clearly the behavior of the outer electron radiation belt at different timescales: months-long periods of gradual inward radial diffusive transport and weak loss being punctuated by dramatic flux changes driven by strong solar wind transient events. We present analysis of multi-MeV electron flux and phase space density (PSD) changes during March 2013 in the context of the first year of Van Allen Probes operation. This March period demonstrates the classic signatures both of inward radial diffusive energization and abrupt localized acceleration deep within the outer Van Allen zone (L ~4.0 ± 0.5). This reveals graphically that both “competing” mechanisms of multi-MeV electron energization are at play in the radiation belts, often acting almost concurrently or at least in rapid succession.


Geophysical Research Letters | 2000

Simultaneous observations of E‐region coherent backscatter and electric field amplitude at F‐region heights with the Millstone Hill UHF Radar

J. C. Foster; Philip J. Erickson

A combined coherent backscatter-incoherent scatter experiment with the Millstone Hill UHF radar provided simultaneous observations of electric field magnitude and coherent backscatter parameters on the same L shell. A carefully-designed geometry used sidelobe coherent contamination from two-stream irregularities at 110 km altitude, appearing at ranges corresponding to F-region altitudes in the main beam, in conjunction with simultaneous uncontaminated F-region observations of the drift velocity in adjacent range gates. Both logarithmic coherent power and the magnitude of the coherent phase velocity Vph vary linearly with . With the assumption that the coherent phase velocity is approximately the perturbed ion sound speed in the heated E region, we find an excellent agreement between the electron temperature inferred from Vph and previous incoherent-scatter results relating E-region Te to E. A maximum value of ∼3100 K has been found for such wave-induced E-region heating.


Geophysical Research Letters | 2014

Prompt energization of relativistic and highly relativistic electrons during a substorm interval: Van Allen Probes observations

J. C. Foster; Philip J. Erickson; D. N. Baker; S. G. Claudepierre; C. A. Kletzing; W. S. Kurth; G. D. Reeves; S. A. Thaller; Harlan E. Spence; Y. Y. Shprits; J. R. Wygant

University of Minnesota (Van Allen Probes subaward to Massachusetts Institute of Technology)


Journal of Geophysical Research | 2016

Highly relativistic radiation belt electron acceleration, transport, and loss: Large solar storm events of March and June 2015

D. N. Baker; A. N. Jaynes; S. G. Kanekal; J. C. Foster; Philip J. Erickson; J. F. Fennell; J. B. Blake; H. Zhao; X. Li; Scot Richard Elkington; M. G. Henderson; Geoff Reeves; Harlan E. Spence; C. A. Kletzing; J. R. Wygant

Abstract Two of the largest geomagnetic storms of the last decade were witnessed in 2015. On 17 March 2015, a coronal mass ejection‐driven event occurred with a Dst (storm time ring current index) value reaching −223 nT. On 22 June 2015 another strong storm (Dst reaching −204 nT) was recorded. These two storms each produced almost total loss of radiation belt high‐energy (E ≳ 1 MeV) electron fluxes. Following the dropouts of radiation belt fluxes there were complex and rather remarkable recoveries of the electrons extending up to nearly 10 MeV in kinetic energy. The energized outer zone electrons showed a rich variety of pitch angle features including strong “butterfly” distributions with deep minima in flux at α = 90°. However, despite strong driving of outer zone earthward radial diffusion in these storms, the previously reported “impenetrable barrier” at L ≈ 2.8 was pushed inward, but not significantly breached, and no E ≳ 2.0 MeV electrons were seen to pass through the radiation belt slot region to reach the inner Van Allen zone. Overall, these intense storms show a wealth of novel features of acceleration, transport, and loss that are demonstrated in the present detailed analysis.


Journal of Geophysical Research | 2015

Shock-induced prompt relativistic electron acceleration in the inner magnetosphere

J. C. Foster; J. R. Wygant; M. K. Hudson; A. J. Boyd; D. N. Baker; Philip J. Erickson; Harlan E. Spence

We present twin Van Allen Probes spacecraft observations of the effects of a solar wind shock impacting the magnetosphere on 8 October 2013. The event provides details both of the accelerating electric fields associated with the shock and the response of inner magnetosphere electron populations across a broad range of energies. During this period, the two Van Allen Probes observed shock effects from the vantage point of the dayside magnetosphere at radial positions of L = 3 and L = 5, at the location where shock-induced acceleration of relativistic electrons occurs. The extended (~1 min) duration of the accelerating electric field across a broad extent of the dayside magnetosphere, coupled with energy-dependent relativistic electron gradient drift velocities, selects a preferred range of energies (3–4 MeV) for the initial enhancement. Those electrons—whose drift velocity closely matches the azimuthal phase velocity of the shock-induced pulse—stayed in the accelerating wave as it propagated tailward and received the largest increase in energy. Drift resonance with subsequent strong ULF waves further accentuated this range of electron energies. Phase space density and positional considerations permit the identification of the source population of the energized electrons. Observations detail the promptness (<20 min), energy range (1.5–4.5 MeV), energy increase (~500 keV), and spatial extent (L* ~3.5–4.0) of the enhancement of the relativistic electrons. Prompt acceleration by impulsive shock-induced electric fields and subsequent ULF wave processes therefore comprises a significant mechanism for the acceleration of highly relativistic electrons deep inside the outer radiation belt as shown clearly by this event.


Geophysical Research Letters | 2015

Thermospheric poleward wind surge at midlatitudes during great storm intervals

Shun-Rong Zhang; Philip J. Erickson; J. C. Foster; John M. Holt; Anthea J. Coster; Jonathan J. Makela; John Noto; John W. Meriwether; Brian J. Harding; Juanita Riccobono; Robert B. Kerr

United States. National Aeronautics and Space Administration (Living with a Star NNX15AB83G)


Geophysical Research Letters | 2014

Storm time observations of plasmasphere erosion flux in the magnetosphere and ionosphere

J. C. Foster; Philip J. Erickson; Anthea J. Coster; S. A. Thaller; J. Tao; J. R. Wygant; J. W. Bonnell

Plasmasphere erosion carries cold dense plasma of ionospheric origin in a storm-enhanced density plume extending from dusk toward and through the noontime cusp and dayside magnetopause and back across polar latitudes in a polar tongue of ionization. We examine dusk sector (20 MLT) plasmasphere erosion during the 17 March 2013 storm (Dst ~ −130 nT) using simultaneous, magnetically aligned direct sunward ion flux observations at high altitude by Van Allen Probes RBSP-A (at ~3.0 Re) and at ionospheric heights (~840 km) by DMSP F-18. Plasma erosion occurs at both high and low altitudes where the subauroral polarization stream flow overlaps the outer plasmasphere. At ~20 UT, RBSP-A observed ~1.2E12 m−2 s−1 erosion flux, while DMSP F-18 observed ~2E13 m−2 s−1 sunward flux. We find close similarities at high and low altitudes between the erosion plume in both invariant latitude spatial extent and plasma characteristics.

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J. C. Foster

Massachusetts Institute of Technology

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Anthea J. Coster

Massachusetts Institute of Technology

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Frank D. Lind

Massachusetts Institute of Technology

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Larisa P. Goncharenko

Massachusetts Institute of Technology

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Shun-Rong Zhang

Massachusetts Institute of Technology

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D. N. Baker

University of Colorado Boulder

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William C. Rideout

Massachusetts Institute of Technology

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J. R. Wygant

University of Minnesota

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John M. Holt

Massachusetts Institute of Technology

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