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Dive into the research topics where I. P. Robertson is active.

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Featured researches published by I. P. Robertson.


Journal of Geophysical Research | 2001

Temporal variations of geocoronal and heliospheric X-ray emission associated with the solar wind interaction with neutrals

T. E. Cravens; I. P. Robertson; S. L. Snowden

X-ray emission due to charge transfer collisions between heavy solar wind ions and neutrals has been predicted to exist both in the heliosphere and in the geocorona. The heliospheric X-ray emission can account for roughly half of the observed soft X-ray background intensity. It was also suggested that temporal variations in the heliospheric and geocoronal soft X-ray intensities will result from solar wind variations. In this paper, a simple model of the charge exchange X-ray emission mechanism is combined with measured solar wind parameters as a function of time and used to generate predictions of the temporal variation of the X-ray intensity observed at Earth for the time periods 1990–1993 and 1996–1998. Measured solar wind proton fluxes are also directly compared with the “long-term enhancement” part of the soft X-ray background measured by the Rontgen Satellite (ROSAT). A significant positive correlation exists, which supports the existence of X-ray emission associated with the solar wind interaction with either interstellar neutrals and/or with geocoronal neutral hydrogen.


Journal of Geophysical Research | 2010

Dynamical and magnetic field time constants for Titan's ionosphere: Empirical estimates and comparisons with Venus

T. E. Cravens; M. S. Richard; Y. J. Ma; C. Bertucci; J. G. Luhmann; Stephen A. Ledvina; I. P. Robertson; Jan-Erik Wahlund; K. Ågren; J. Cui; I. C. F. Müller-Wodarg; J. H. Waite; M. K. Dougherty; J. M. Bell; Demet Ulusen

plasma flow speed relative to the neutral gas speed is approximately 1 m s −1 near an altitude of 1000 km and 200 m s −1 at 1500 km. For comparison, the thermospheric neutral wind speed is about 100 m s −1 . The ionospheric plasma is strongly coupled to the neutrals below an altitude of about 1300 km. Transport, vertical or horizontal, becomes more important than chemistry in controlling ionospheric densities above about 1200–1500 km, depending on the ion species. Empirical estimates are used to demonstrate that the structure of the ionospheric magnetic field is determined by plasma transport (including neutral wind effects) for altitudes above about 1000 km and by magnetic diffusion at lower altitudes. The paper suggests that a velocity shear layer near 1300 km could exist at some locations and could affect the structure of the magnetic field. Both Hall and polarization electric field terms in the magnetic induction equation are shown to be locally important in controlling the structure of Titan’s ionospheric magnetic field. Comparisons are made between the ionospheric dynamics at Titan and at Venus.


Nature | 2014

The origin of the local 1/4-keV X-ray flux in both charge exchange and a hot bubble

M. Galeazzi; Meng Chiao; M. R. Collier; T. E. Cravens; Dimitra Koutroumpa; K. D. Kuntz; Rosine Lallement; S. T. Lepri; D. McCammon; Kelsey Morgan; F. S. Porter; I. P. Robertson; Steven L. Snowden; Nicholas Thomas; Y. Uprety; Eugenio Ursino; B. M. Walsh

The solar neighbourhood is the closest and most easily studied sample of the Galactic interstellar medium, an understanding of which is essential for models of star formation and galaxy evolution. Observations of an unexpectedly intense diffuse flux of easily absorbed 1/4-kiloelectronvolt X-rays, coupled with the discovery that interstellar space within about a hundred parsecs of the Sun is almost completely devoid of cool absorbing gas, led to a picture of a ‘local cavity’ filled with X-ray-emitting hot gas, dubbed the local hot bubble. This model was recently challenged by suggestions that the emission could instead be readily produced within the Solar System by heavy solar-wind ions exchanging electrons with neutral H and He in interplanetary space, potentially removing the major piece of evidence for the local existence of million-degree gas within the Galactic disk. Here we report observations showing that the total solar-wind charge-exchange contribution is approximately 40 per cent of the 1/4-keV flux in the Galactic plane. The fact that the measured flux is not dominated by charge exchange supports the notion of a million-degree hot bubble extending about a hundred parsecs from the Sun.


Journal of Geophysical Research | 2015

An empirical approach to modeling ion production rates in Titan's ionosphere I: Ion production rates on the dayside and globally

M. S. Richard; T. E. Cravens; C. Wylie; D. Webb; Q. Chediak; R. Perryman; K. Mandt; J. H. Westlake; J. H. Waite; I. P. Robertson; B. A. Magee; Niklas J. T. Edberg

Titans ionosphere is created when solar photons, energetic magnetospheric electrons or ions, and cosmic rays ionize the neutral atmosphere. Electron densities generated by current theoretical models are much larger than densities measured by instruments on board the Cassini orbiter. This model density overabundance must result either from overproduction or from insufficient loss of ions. This is the first of two papers that examines ion production rates in Titans ionosphere, for the dayside and nightside ionosphere, respectively. The first (current) paper focuses on dayside ion production rates which are computed using solar ionization sources (photoionization and electron impact ionization by photoelectrons) between 1000 and 1400 km. In addition to theoretical ion production rates, empirical ion production rates are derived from CH4, CH3+, and CH4+ densities measured by the INMS (Ion Neutral Mass Spectrometer) for many Titan passes. The modeled and empirical production rate profiles from measured densities of N2+ and CH4+ are found to be in good agreement (to within 20%) for solar zenith angles between 15 and 90°. This suggests that the overabundance of electrons in theoretical models of Titans dayside ionosphere is not due to overproduction but to insufficient ion losses.


The Astrophysical Journal | 2009

Observation of Solar Wind Charge Exchange Emission from Exospheric Material in and Outside Earth's Magnetosheath 2008 September 25

S. L. Snowden; M. R. Collier; T. E. Cravens; K. D. Kuntz; S. T. Lepri; I. P. Robertson; L. Tomas

A long XMM-Newton exposure is used to observe solar wind charge exchange (SWCX) emission from exospheric material in and outside Earth s magnetosheath. The light curve of the O VII (0.5-0.62 keV) band is compared with a model for the expected emission, and while the emission is faint and the light curve has considerable scatter, the correlation is significant to better than 99.9%. This result demonstrates the validity of the geocoronal SWCX emission model for predicting a contribution to astrophysical observations to a scale factor of order unity (1.36). The results also demonstrate the potential utility of using X-ray observations to study global phenomena of the magnetosheath which currently are only investigated using in situ measurements.


Journal of Geophysical Research | 2014

On Lunar Exospheric Column Densities and Solar Wind Access Beyond the Terminator from ROSAT Soft X-Ray Observations of Solar Wind Charge Exchange

M. R. Collier; Steven L. Snowden; Menelaos Sarantos; Mehdi Benna; J. A. Carter; T. E. Cravens; W. M. Farrell; Shahab Fatemi; H. Kent Hills; R. Richard Hodges; M. Holmström; K. D. Kuntz; F. Scott Porter; A. M. Read; I. P. Robertson; S. Sembay; D. G. Sibeck; T. J. Stubbs; P. Travnicek; B. M. Walsh

We analyze the Rontgen satellite (ROSAT) position sensitive proportional counter soft X-ray image of the Moon taken on 29 June 1990 by examining the radial profile of the surface brightness in three wedges: two 19 ◦ wedges (one north and one south) 13-32 ◦ off the terminator toward the dark side and one wedge 38 ◦ wide centered on the antisolar direction. The radial profiles of both the north and the south wedges show significant limb brightening that is absent in the 38 ◦ wide antisolar wedge. An analysis of the soft X-ray intensity increase associated with the limb brightening shows that its magnitude is consistent with that expected due to solar wind charge exchange (SWCX) with the tenuous lunar atmosphere based on lunar exospheric models and hybrid simulation results of solar wind access beyond the terminator. Soft X-ray imaging thus can independently infer the total lunar limb column density including all species, a property that before now has not been measured, and provide a large-scale picture of the solar wind-lunar interaction. Because the SWCX signal appears to be dominated by exospheric species arising from solar wind implantation, this technique can also determine how the exosphere varies with solar wind conditions. Now, along with Mars, Venus, and Earth, the Moon represents another solar system body at which SWCX has been observed.


SOLAR WIND TEN: Proceedings of the Tenth International Solar Wind Conference | 2001

Temporal and Spatial Variations of Heliospheric x-ray Emissions Associated with Charge Transfer of the Solar Wind with Interstellar Neutrals

I. P. Robertson; T. E. Cravens; S. L. Snowden

A simple model has been developed that demonstrates that heliospheric X-ray emission can account for about 25%–50% of observed soft X-ray background intensities. Similar to cometary soft X-ray emission, these X-rays are thought to be produced in the heliosphere due to charge transfer collisions between heavy solar wind ions and interstellar neutrals. A more complex model has now been developed to take into account temporal and spatial variations of the solar wind and interstellar neutrals. Measured time histories of the solar wind proton flux are used in the model and the results are compared with the ‘long-term enhancements’ in the soft X-ray background measured by ROSAT for the same time period.


The Astrophysical Journal | 2015

THE SOLAR WIND CHARGE-EXCHANGE PRODUCTION FACTOR FOR HYDROGEN

K. D. Kuntz; Yaireska M. Collado-Vega; M. R. Collier; H. K. Connor; T. E. Cravens; Dimitra Koutroumpa; F. S. Porter; I. P. Robertson; David G. Sibeck; S. L. Snowden; Nicholas Thomas; B. M. Walsh

The mean production factor, or broadband averaged cross-section, for solar wind charge-exchange (SWCX) with hydrogen producing emission in the ROSAT 1/4 keV (R12) band is (3.8 ± 0.2) x 10-20 count degree−2 cm4. The production factor is expected to be temporally variable, and that variation is roughly 15%. These values are derived from a comparison of the long-term (background) enhancements in the ROSAT All-Sky Survey with magnetohysdrodynamic simulations of the magnetosheath. This value is 1.8–4.5 times higher than values derived from limited atomic data, suggesting that those values may be missing a large number of faint lines. This production factor is important for deriving the exact amount of 1/4 keV band flux that is due to the Local Hot Bubble, for planning future observations in the 1/4 keV band, and for evaluating proposals for remote sensing of the magnetosheath. The same method cannot be applied to the 3/4 keV band as that band, being composed primarily of the oxygen lines, is far more sensitive to the detailed abundances and ionization balance in the solar wind. We also show, incidentally, that recent efforts to correlate XMM-Newton observing geometry with magnetosheath SWCX emission in the oxygen lines have been, quite literally, misguided. Simulations of the inner heliosphere show that broader efforts to correlate heliospheric SWCX with local solar wind parameters are unlikely to produce useful results.


The Astrophysical Journal | 2014

Pressure Equilibrium Between The Local Interstellar Clouds And The Local Hot Bubble

Steven L. Snowden; Meng Chiao; M. R. Collier; F. S. Porter; Nicholas Thomas; T. E. Cravens; I. P. Robertson; M. Galeazzi; Y. Uprety; Eugenio Ursino; Dimitra Koutroumpa; K. D. Kuntz; Rosine Lallement; Lucky Puspitarini; S. T. Lepri; D. McCammon; Kelsey Morgan; B. M. Walsh

Three recent results related to the heliosphere and the local interstellar medium (ISM) have provided an improved insight into the distribution and conditions of material in the solar neighborhood. These are the measurement of the magnetic field outside of the heliosphere by Voyager 1, the improved mapping of the three-dimensional structure of neutral material surrounding the Local Cavity using extensive ISM absorption line and reddening data, and a sounding rocket flight which observed the heliospheric helium focusing cone in X-rays and provided a robust estimate of the contribution of solar wind charge exchange emission to the ROSAT All-Sky Survey 1/4?keV band data. Combining these disparate results, we show that the thermal pressure of the plasma in the Local Hot Bubble (LHB) is P/k = 10, 700?cm?3?K. If the LHB is relatively free of a global magnetic field, it can easily be in pressure (thermal plus magnetic field) equilibrium with the local interstellar clouds, eliminating a long-standing discrepancy in models of the local ISM.


THE LOCAL BUBBLE AND BEYOND II: Proceedings of the International#N#Conference | 2009

The Lunar X‐ray Observatory (LXO)/Magnetosheath Explorer in X‐rays (MagEX)

M. R. Collier; Tony Abbey; Nigel P. Bannister; J. A. Carter; M. Choi; T. E. Cravens; Mike Evans; George W. Fraser; H. K. Hills; K. D. Kuntz; J. Lyons; N. Omidi; F. S. Porter; A. M. Read; I. P. Robertson; P. Rozmarynowski; S. Sembay; D. G. Sibeck; Steven L. Snowden; T. J. Stubbs; Pavel M. Travnicek

X‐ray observations of solar wind charge exchange (SWCX) emission, a nuisance to astrophysicists, will dramatically enhance our ability to determine the structure and variability of the Earth’s magnetosheath. Such observations could be made from the lunar surface or an Earth‐orbiting spacecraft and will resolve key controversies about magnetopause physics as well as better characterize SWCX emission with the aim of avoiding or removing it from astrophysical observations.

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J. H. Waite

University of Michigan

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K. D. Kuntz

Johns Hopkins University

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J. G. Luhmann

University of California

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M. R. Collier

Goddard Space Flight Center

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J.-E. Wahlund

Swedish Institute of Space Physics

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Steven L. Snowden

Goddard Space Flight Center

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