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Dive into the research topics where Tero Raita is active.

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Featured researches published by Tero Raita.


Journal of Geophysical Research | 2004

Complex lithospheric structure under the central Baltic Shield from surface wave tomography

Marianne Bruneton; Helle A. Pedersen; Véronique Farra; Nicholas T. Arndt; Pierre Vacher; U. Achauer; A. Alinaghi; J. Ansorge; G. Bock; W. Friederich; Marek Grad; Aleksander Guterch; Pekka Heikkinen; S.‐E. Hjelt; T. L. Hyvönen; J.‐P. Ikonen; E. Kissling; K. Komminaho; A. Korja; Elena Kozlovskaya; M. V. Nevsky; Hanneke Paulssen; N. I. Pavlenkova; J. Plomerová; Tero Raita; O. Y. Riznichenko; Roland Roberts; S. Sandoval; I. A. Sanina; N. V. Sharov

Complex lithospheric structure under the central Baltic Shield from surface wave tomography


Journal of Geophysical Research | 2015

Van Allen probes, NOAA, GOES, and ground observations of an intense EMIC wave event extending over 12 h in magnetic local time

M. J. Engebretson; J. L. Posch; J. R. Wygant; C. A. Kletzing; M. R. Lessard; C.-L. Huang; Harlan E. Spence; Charles W. Smith; H. J. Singer; Yoshiharu Omura; Richard B. Horne; G. D. Reeves; D. N. Baker; Matina Gkioulidou; K. Oksavik; Ian R. Mann; Tero Raita; K. Shiokawa

Although most studies of the effects of electromagnetic ion cyclotron (EMIC) waves on Earths outer radiation belt have focused on events in the afternoon sector in the outer plasmasphere or plume region, strong magnetospheric compressions provide an additional stimulus for EMIC wave generation across a large range of local times and L shells. We present here observations of the effects of a wave event on 23 February 2014 that extended over 8 h in UT and over 12 h in local time, stimulated by a gradual 4 h rise and subsequent sharp increases in solar wind pressure. Large-amplitude linearly polarized hydrogen band EMIC waves (up to 25 nT p-p) appeared for over 4 h at both Van Allen Probes, from late morning through local noon, when these spacecraft were outside the plasmapause, with densities ~5–20 cm−3. Waves were also observed by ground-based induction magnetometers in Antarctica (near dawn), Finland (near local noon), Russia (in the afternoon), and in Canada (from dusk to midnight). Ten passes of NOAA-POES and METOP satellites near the northern foot point of the Van Allen Probes observed 30–80 keV subauroral proton precipitation, often over extended L shell ranges; other passes identified a narrow L shell region of precipitation over Canada. Observations of relativistic electrons by the Van Allen Probes showed that the fluxes of more field-aligned and more energetic radiation belt electrons were reduced in response to both the emission over Canada and the more spatially extended emission associated with the compression, confirming the effectiveness of EMIC-induced loss processes for this event.


Journal of Geophysical Research | 2007

Energetic particle precipitation into the middle atmosphere triggered by a coronal mass ejection

Mark A. Clilverd; Craig J. Rodger; Robyn Margaret Millan; J. G. Sample; M. Kokorowski; Michael P. McCarthy; Thomas Ulich; Tero Raita; A. J. Kavanagh; E. Spanswick

Precipitation of relativistic electrons into the atmosphere has been suggested as the primary loss mechanism for radiation belt electrons during large geomagnetic storms. Here we investigate the geographical spread of precipitation as a result of the arrival of a coronal mass ejection (CME) on 21 January 2005. In contrast to previous statistical studies we provide one of the first attempts to describe the geographic and temporal variability of energetic particle precipitation on a global scale using an array of instruments. We combine data from subionospheric VLF radio wave receivers, the high-altitude Miniature Spectrometer (MINIS) balloons, riometers, and pulsation magnetometers during the first hour of the event. There were three distinct types of energetic electron precipitation observed, one globally, one on the dayside, and one on the nightside. The most extensively observed form of precipitation was a large burst starting when the CME arrived at the Earth, where electrons from the outer radiation belt were lost to the atmosphere over a large region of the Earth. On the dayside of the Earth (10–15 MLT) the CME produced a further series of precipitation bursts, while on the nightside dusk sector (∼20 MLT) a continuous precipitation event lasting ∼50 min was observed at 2.5 < L < 3.7 along with Pc 1–2 pulsations observed with a ground-based magnetometer. These observations suggest that the generation of energetic electron precipitation at the inner edge of the outer radiation belt from electromagnetic ion cyclotron (EMIC) wave scattering into the loss cone is the most direct evidence to date connecting EMIC activity and energetic precipitation.


Journal of Geophysical Research | 2015

Electron precipitation from EMIC waves: a case study from 31 May 2013

Mark A. Clilverd; Roger Duthie; Rachael Hardman; Aaron T. Hendry; Craig J. Rodger; Tero Raita; M. J. Engebretson; M. R. Lessard; D. W. Danskin; David K. Milling

On 31 May 2013 several rising-tone electromagnetic ion-cyclotron (EMIC) waves with intervals of pulsations of diminishing periods (IPDP) were observed in the magnetic local time afternoon and evening sectors during the onset of a moderate/large geomagnetic storm. The waves were sequentially observed in Finland, Antarctica, and western Canada. Co-incident electron precipitation by a network of ground-based Antarctic Arctic Radiation-belt Dynamic Deposition VLF Atmospheric Research Konsortia (AARDDVARK) and riometer instruments, as well as the Polar-orbiting Operational Environmental Satellite (POES) electron telescopes, was also observed. At the same time POES detected 30-80 keV proton precipitation drifting westwards at locations that were consistent with the ground-based observations, indicating substorm injection. Through detailed modelling of the combination of ground and satellite observations the characteristics of the EMIC-induced electron precipitation were identified as: latitudinal width of 2-3° or ΔL=1 Re, longitudinal width ~50° or 3 hours MLT, lower cut off energy 280 keV, typical flux 1×104 el. cm-2 sr-1 s-1 >300 keV. The lower cutoff energy of the most clearly defined EMIC rising tone in this study confirms the identification of a class of EMIC-induced precipitation events with unexpectedly low energy cutoffs of <400 keV.


Journal of Geophysical Research | 2012

Characteristics of precipitating energetic ions/electrons associated with the wave-particle interaction in the plasmaspheric plume

Zhigang Yuan; Ying Xiong; Dedong Wang; Ming Li; Xiaohua Deng; A. G. Yahnin; Tero Raita; Jingfang Wang

In this paper, we present characteristics of precipitating energetic ions/electrons associated with the wave-particle interaction in the plasmaspheric plume during the geomagnetic storm on July 18, 2005 with observations of the NOAA15 NOAA16, IMAGE satellites and Finnish network of search coil magnetometers. Conjugate observations of the NOAA15 satellite and the Finnish network of search coil magnetometers have demonstrated that a sharp enhancement of the precipitating ion flux is a result of ring current (RC) ions scattered into the loss cone by EMIC waves. Those precipitating RC ions lead to a detached subauroral proton arc observed by the IMAGE FUV. In addition, with observations of NOAA15 and NOAA16, the peak of precipitating electron flux was equatorward to that of precipitating proton flux, which is in agreement with the region separation of ELF hiss and EMIC waves observed by the Cluster C1 in the Yuan et al. (2012) companion paper. In combination with the result of the companion paper, we demonstrate the link between the wave activities (ELF hiss, EMIC waves) in plasmaspheric plumes and energetic ion/electron precipitation at ionospheric altitudes. Therefore, it is an important characteristic of the plasmaspheric plumes-RC-ionosphere interaction during a geomagnetic storm that the precipitation of energetic protons is latitudinally separated from that of energetic electrons.


Nature Communications | 2016

Wave-induced loss of ultra-relativistic electrons in the Van Allen radiation belts

Y. Y. Shprits; A. Drozdov; M. Spasojevic; A. C. Kellerman; M. E. Usanova; M. J. Engebretson; Oleksiy V. Agapitov; Irina S. Zhelavskaya; Tero Raita; Harlan E. Spence; D. N. Baker; Hui Zhu; N. A. Aseev

The dipole configuration of the Earths magnetic field allows for the trapping of highly energetic particles, which form the radiation belts. Although significant advances have been made in understanding the acceleration mechanisms in the radiation belts, the loss processes remain poorly understood. Unique observations on 17 January 2013 provide detailed information throughout the belts on the energy spectrum and pitch angle (angle between the velocity of a particle and the magnetic field) distribution of electrons up to ultra-relativistic energies. Here we show that although relativistic electrons are enhanced, ultra-relativistic electrons become depleted and distributions of particles show very clear telltale signatures of electromagnetic ion cyclotron wave-induced loss. Comparisons between observations and modelling of the evolution of the electron flux and pitch angle show that electromagnetic ion cyclotron waves provide the dominant loss mechanism at ultra-relativistic energies and produce a profound dropout of the ultra-relativistic radiation belt fluxes.


Journal of Geophysical Research | 2015

Long‐term determination of energetic electron precipitation into the atmosphere from AARDDVARK subionospheric VLF observations

Jason J. Neal; Craig J. Rodger; Mark A. Clilverd; Neil R. Thomson; Tero Raita; Thomas Ulich

We analyze observations of subionospherically propagating very low frequency (VLF) radio waves to determine outer radiation belt energetic electron precipitation (EEP) flux magnitudes. The radio wave receiver in Sodankyla, Finland (Sodankyla Geophysical Observatory) observes signals from the transmitter with call sign NAA (Cutler, Maine). The receiver is part of the Antarctic-Arctic Radiation-belt Dynamic Deposition VLF Atmospheric Research Konsortia (AARDDVARK). We use a near-continuous data set spanning November 2004 until December 2013 to determine the long time period EEP variations. We determine quiet day curves over the entire period and use these to identify propagation disturbances caused by EEP. Long Wave Propagation Code radio wave propagation modeling is used to estimate the precipitating electron flux magnitudes from the observed amplitude disturbances, allowing for solar cycle changes in the ambient D region and dynamic variations in the EEP energy spectra. Our method performs well during the summer months when the daylit ionosphere is most stable but fails during the winter. From the summer observations, we have obtained 693 days worth of hourly EEP flux magnitudes over the 2004–2013 period. These AARDDVARK-based fluxes agree well with independent satellite precipitation measurements during high-intensity events. However, our method of EEP detection is 10–50 times more sensitive to low flux levels than the satellite measurements. Our EEP variations also show good agreement with the variation in lower band chorus wave powers, providing some confidence that chorus is the primary driver for the outer belt precipitation we are monitoring.


IEEE Transactions on Geoscience and Remote Sensing | 2015

KAIRA: The Kilpisjärvi Atmospheric Imaging Receiver Array—System Overview and First Results

Derek McKay-Bukowski; Juha Vierinen; Ilkka Virtanen; R. A. Fallows; Markku Postila; Thomas Ulich; O. Wucknitz; M. A. Brentjens; Nico Ebbendorf; Carl-Fredrik Enell; Marchel Gerbers; Teun Grit; Peter Gruppen; Antti Kero; Toivo Iinatti; M. S. Lehtinen; Henri Meulman; M. J. Norden; Mikko Orispää; Tero Raita; Jan Pieter de Reijer; Lassi Roininen; A. Schoenmakers; Klaas Stuurwold; Esa Turunen

The Kilpisjärvi Atmospheric Imaging Receiver Array (KAIRA) is a dual array of omnidirectional VHF radio antennas located near Kilpisjärvi, Finland. It is operated by the Sodankylä Geophysical Observatory. It makes extensive use of the proven LOFAR antenna and digital signal-processing hardware, and can act as a stand-alone passive receiver, as a receiver for the European Incoherent Scatter (EISCAT) very high frequency (VHF) incoherent scatter radar in Tromsø, or for use in conjunction with other Fenno-Scandinavian VHF experiments. In addition to being a powerful observing instrument in its own right, KAIRA will act as a pathfinder for technologies to be used in the planned EISCAT_3-D phased-array incoherent scatter radar system and participate in very long baseline interferometry experiments. This paper gives an overview of KAIRA, its principal hardware and software components, and its main science objectives. We demonstrate the applicability of the radio astronomy technology to our geoscience application. Furthermore, we present a selection of results from the commissioning phase of this new radio observatory.


Dynamics of the Earth's Radiation Belts and Inner Magnetosphere | 2013

Rapid Radiation Belt Losses Occurring During High-Speed Solar Wind Stream–Driven Storms: Importance of Energetic Electron Precipitation

Aaron T. Hendry; Craig J. Rodger; Mark A. Clilverd; Neil R. Thomson; S. K. Morley; Tero Raita

Dynamics of the E Geophysical Mon


Geophysical Research Letters | 2014

Spatial localization and ducting of EMIC waves: Van Allen Probes and ground‐based observations

Ian R. Mann; M. E. Usanova; Kyle R. Murphy; M. T. Robertson; David K. Milling; A. Kale; C. A. Kletzing; J. R. Wygant; S. A. Thaller; Tero Raita

On 11 October 2012, during the recovery phase of a moderate geomagnetic storm, an extended interval (> 18 h) of continuous electromagnetic ion cyclotron (EMIC) waves was observed by Canadian Array for Real-time Investigations of Magnetic Activity and Solar-Terrestrial Environment Program induction coil magnetometers in North America. At around 14:15 UT, both Van Allen Probes B and A (65° magnetic longitude apart) in conjunction with the ground array observed very narrow (ΔL ~ 0.1–0.4) left-hand polarized EMIC emission confined to regions of mass density gradients at the outer edge of the plasmasphere at L ~ 4. EMIC waves were seen with complex polarization patterns on the ground, in good agreement with model results from Woodroffe and Lysak (2012) and consistent with Earths rotation sweeping magnetometer stations across multiple polarization reversals in the fields in the Earth-ionosphere duct. The narrow L-widths explain the relative rarity of space-based EMIC occurrence, ground-based measurements providing better estimates of global EMIC wave occurrence for input into radiation belt dynamical models.

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A. J. Kavanagh

British Antarctic Survey

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M. R. Lessard

University of New Hampshire

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