R. F. Woodman’s research while affiliated with Instituto Geofísico del Perú and other places

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Publications (125)


Figure 1. A replica of Sputnik 1 at the US National Air and Space Museum. Sputnik 1 was launched by the Soviet Union on 4 October 1957.
Figure 2. (a) William E. Gordon (1918-2010), physicist and astronomer. He proposed the incoherent scatter technique in 1958. (b) Kenneth L. Bowles (1929-2018), electrical engineer and computer scientist. He conducted successfully the first incoherent scatter radar observations in the same year the theory was proposed.
Figure 3. First incoherent scatter radar measurements conducted in October 1958 (adapted from Bowles, 1958). The top panel corresponds to power measurements obtained using a pulse width of 140 µs (21 km) and a bandwidth of 10 kHz. In the bottom panel, the measurements were obtained using a pulse width of 120 µs (18 km) and a bandwidth of 15 kHz.
Figure 4. Inclination of the Earth's magnetic field based on IGRF 1990. The magnetic Equator (I = 0 • ) passes through the central part of Peru. This fact has remained true since the 1960s until today despite the time variation in the magnetic field (adapted from Blakely, 1995).
Figure 5. Site survey -March 1960. Aerial view of the site that became the Jicamarca Radio Observatory (picture taken by Ken Bowles).

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The early history of the Jicamarca Radio Observatory and the incoherent scatter technique
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October 2019

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898 Reads

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12 Citations

History of Geo- and Space Sciences

Ronald F. Woodman

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Donald T. Farley

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The purpose of these historical notes is to present the early history of the Jicamarca Radio Observatory (JRO), a research facility that has been conducting observations and studies of the equatorial ionosphere for more than 50 years. We have limited the scope of these notes to the period of the construction of the observatory and roughly the first decade of its operation. Specifically, this period corresponds to the directorships under Kenneth Bowles, Donald Farley, and Tor Hagfors and the first period of Ronald Woodman, i.e., the years between 1960 and 1974. Within this time frame, we will emphasize observational and instrumental developments which led to define the capabilities of the Jicamarca incoherent scatter (IS) radar to measure the different physical parameters of the ionosphere. At the same time, we partially cover the early history of the IS technique which has been used by many other observatories built since. We will also briefly mention the observatory's early and most important contributions to our understanding of the physical mechanisms behind the many peculiar phenomena that occur at the magnetic Equator. Finally, we will put special emphasis on the important developments of the instrument and its observing techniques that frame the capabilities of the radar at that time.

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High-altitude incoherent-scatter measurements at Jicamarca: HIGH-ALTITUDE ISR

February 2017

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29 Reads

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4 Citations

In an attempt to reproduce experimental results obtained in the early days of operations, electron density profiles have been measured at the Jicamarca Radio Observatory at altitudes reaching L=2. The methodology involves using a combination of pulses, including pulses as long as 4 ms, and processing the data with matched filtering. The modern experiments are complicated by systemic, time-dependent bias in the noise estimators as well as by clutter from satellites and space debris, including a geosynchronous satellite. Ultimately, experiment performance comparable to what was achieved in the original experiments could be achieved and should be surpassed in future experiments when all four of the Jicamarca transmitters will be utilized.


Simultaneous observations of structure function parameter of refractive index using a high-resolution radar and the DataHawk small airborne measurement system

September 2016

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12 Citations

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The SOUSY (SOUnding SYstem) radar was relocated to the Jicamarca Radio Observatory (JRO) near Lima, Peru, in 2000, where the radar controller and acquisition system were upgraded with state-of-the-art parts to take full advantage of its potential for high-resolution atmospheric sounding. Due to its broad bandwidth (4 MHz), it is able to characterize clear-air backscattering with high range resolution (37.5 m). A campaign conducted at JRO in July 2014 aimed to characterize the lower troposphere with a high temporal resolution (8.1 Hz) using the DataHawk (DH) small unmanned aircraft system, which provides in situ atmospheric measurements at scales as small as 1 m in the lower troposphere and can be GPS-guided to obtain measurements within the beam of the radar. This was a unique opportunity to make coincident observations by both systems and to directly compare their in situ and remotely sensed parameters. Because SOUSY only points vertically, it is only possible to retrieve vertical radar profiles caused by changes in the refractive index within the resolution volume. Turbulent variations due to scattering are described by the structure function parameter of refractive index Cn². Profiles of Cn² from the DH are obtained by combining pressure, temperature, and relative humidity measurements along the helical trajectory and integrated at the same scale as the radar range resolution. Excellent agreement is observed between the Cn² estimates obtained from the DH and SOUSY in the overlapping measurement regime from 1200 m up to 4200 m above sea level, and this correspondence provides the first accurate calibration of the SOUSY radar for measuring Cn².



Fine-Scale Characteristics of Temperature, Wind, and Turbulence in the Lower Atmosphere (0–1,300 m) Over the South Peruvian Coast

April 2012

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321 Reads

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37 Citations

Boundary-Layer Meteorology

We report results of preliminary high-resolution in situ atmospheric measurements through the boundary layer and lower atmosphere over the southern coast of Perú. This region of the coast is of particular interest because it lies adjacent to the northern coastal edge of the sub-tropical south-eastern Pacific, a very large area of ocean having a persistent stratus deck located just below the marine boundary layer (MBL) inversion. Typically, the boundary layer in this region during winter is topped by a quasi-permanent, well-defined, and very large temperature gradient. The data presented herein examine fine-scale details of the coastal atmosphere at a point where the edge of this MBL extends over the coastline as a result of persistent onshore flow. Atmospheric data were gathered using a recently-developed in-house constructed, GPS-controlled, micro-autonomous-vehicle aircraft (the DataHawk). Measured quantities include high-resolution profiles of temperature, wind, and turbulence structure from the surface to 1,300 m.


First simultaneous measurements of thermospheric winds and zonal ion drifts from the Jicamarca Radio Observatory

January 2010

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31 Reads

The first simultaneous observations of thermospheric winds and zonal ion drifts have been ob-tained at the Jicamarca Radio Observatory using a new Fabry-Perot interferometer observatory installed on a mountain ridge overlooking the valley where the JRO radar is located. The re-sults show that the neutral winds and ion drifts generally have the same speed and temporal variation characteristics. These results illustrate the simultaneous detection of the midnight temperature maximum as well. The paper will also describe efforts to obtain common volume measurements of thermospheric winds and temperatures utilizing the FPI Arequipa observatory which is located 4 degrees south of the geomagnetic equator.


Naturally enhanced ion-line spectra around the equatorial 150-km region

March 2009

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287 Reads

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19 Citations

For many years strong radar echoes coming from 140–170 km altitudes at low latitudes have been associated to the existence of field-aligned irregularities (FAIs) (the so called 150-km echoes). In this work, we present frequency spectra as well as angular distribution of 150-km echoes. When the 150-km region is observed with beams perpendicular to the magnetic field (B) the observed radar spectra are very narrow with spectral widths between 3–12 m/s. On the other hand, when few-degrees off-perpendicular beams are used, the radar spectra are wide with spectral widths comparable to those expected from ion-acoustic waves at these altitudes (>1000 m/s). Moreover the off-perpendicular spectral width increases with increasing altitude. The strength of the received echoes is one to two orders of magnitude stronger than the expected level of waves in thermal equilibrium at these altitudes. Such enhancement is not due to an increase in electron density. Except for the enhancement in power, the spectra characteristics of off-perpendicular and perpendicular echoes are in reasonable agreement with expected incoherent scatter spectra at these angles and altitudes. 150-km echoes are usually observed in narrow layers (2 to 5). Bistatic common volume observations as well as observations made few kilometers apart show that, for most of the layers, there is very high correlation on power fluctuations without a noticeable time separation between simultaneous echoes observed with Off-perpendicular and Perpendicular beams. However, in one of the central layers, the echoes are the strongest in the perpendicular beam and absent or very weak in the off-perpendicular beams, suggesting that they are generated by a plasma instability. Our results indicate that most echoes around 150-km region are not as aspect sensitive as originally thought, and they come from waves that have been enhanced above waves in thermal equilibrium.


Figure 1. (a) Geomagnetic field intensity, (b) gyroperiod and (c) aspect angle as a function of range along the radar line-of-sight. 
Ion gyroresonance observations at Jicamarca revisited

July 2007

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42 Reads

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1 Citation

1] This paper presents recent observations of the proton gyroresonance over Jicamarca. In October 2006, a single-polarization double-pulse experiment was set up to measure the first gyroresonance peak in the incoherent scatter (IS) auto-correlation function (ACF). Despite the clutter caused by Spread-F and artificial satellites, it was possible to measure the first proton gyroresonance peak of the ACF in the topside ionosphere. For the first time, least-squares fits of theoretical IS ACFs to gyroresonance measurements are reported. Theoretical ACFs that best fit the measurements were found using the H + fraction and temperature (assuming T e = T i) as fitting parameters. Uncertainties for the estimated fraction of H + were as low as 12%, while uncertainties for estimated temperatures were around 30%. These are the first successful gyroresonance measurements since the early observations of Farley (1967), and it is the first time measurements of this type have been used to obtain least squares estimates of ion composition and temperatures. An edited version of this paper was published by AGU. Copyright 2007 American Geophysical Union. To view the published open abstract, go to http://dx.doi.org and enter the DOI.


Sporadic meteor sources as observed by the Jicamarca high-power VHF radar

May 2007

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34 Reads

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67 Citations

Icarus

We present, for the first time, the main sources of sporadic meteors as inferred from meteor-head echoes obtained by a high-power large-aperture radar (HPLAR). Such results have been obtained at the Jicamarca HPLAR (11.95° S, 76.87° W, 1° dip angle). Observations are based on close to 170,000 meteors detected in less than 90 h spread over 14 days, between November 2001 and February 2006. Meteors with solar orbits are observed to come from basically six previously known sources, i.e., North and South Apex, Helion, Anti-Helion, and North and South Toroidal, representing ∼91% of the observations. The other ∼9% represents meteors with observed velocities greater than the Sun's escape velocity at 1 AU, most of them of extra-solar origin. Results are given before and after removing the Earth's velocity and the sources are modeled with two-dimensional Gaussian distributions. In general, our results are in very good agreement with previously known sources reported by Jones and Brown [Jones, J., Brown, P.G., 1993. Mon. Not. R. Astron. Soc. 265, 524–532] using mainly specular meteor radar (SMR) data gathered over many years and different sites. However, we find slightly different locations and widths, that could be explained on the basis of different sensitivities of the two techniques and/or corrections needed to our results. For example, we find that the North and South Apex sources are well defined and composed each of them of two collocated Gaussian distributions, one almost isotropic with ∼10° width and the other very narrow in ecliptic longitude and wide in ecliptic latitude. This is the first time these narrow-width sources are reported. A careful quantitative analysis is needed to be able to compare the strengths of meteor sources as observed with different techniques. We also present speed and initial altitude distributions for selected sources. Using a simple angular sensitivity function of the combined Earth–atmosphere–radar instrument, and an altitude selection criteria, the resulting meteor sources are in better qualitative agreement with the results obtained with SMRs.


Figure 4. Shape of the transmitter pulse (amplitude) processed by the receiving system. The top panel shows the pulse using the 600 kW final stage for different excitations, the bottom panel shows the same but using the 20 kW driver stage and only 250 nsec modes. The secondary peak is due to a local strong reflection. 
The MPI-SOUSY-VHF Radar at Jicamarca: High Altitude-Resolution Capabilities

January 2007

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98 Reads

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11 Citations

The MPI-SOUSY radar has been moved from its original location at the Harz Mountains, Germany, to the Jicamarca Observatory. Two main modifications have been made to the system: 1) The antenna array now consist of 126 Yagis deployed in an square array of 16x16, 4 element Yagis, similar to the original ones, and 2) the control and data acquisition system has been modernized as described later on. The phase steering system has not been implemented yet, but is planned for the future. Figure 1 shows schematically the disposition of the Yagis and their interconnexion in the array. For the particular application described in this paper, they are all connected with the same phase, therefore the full array is practically pointing towards the zenith. Figure 2 shows a picture of the same in context with the Jicamarca main antenna. One of the objectives of the move was to take advantage of the wider bandwidth of the SOUSY transmitter to obtain higher altitude-resolution radar measurements than it had been obtained at VHF frequencies in the past (50 MHz range in particular), at both atmospheric and ionospheric heights. Very stringent frequency allocation bandwidth at the Harz had limited its operation to 150 meter Gaussian shape pulses.


Citations (79)


... The Jicamarca Radio Observatory (JRO), located near Lima, Peru, is home to one of the world's premier Incoherent Scatter Radars (ISR), known for its high-resolution ionospheric measurements. It plays a pivotal role in advancing the understanding of the equatorial ionosphere, a region with complex and dynamic plasma processes [18]. ...

Reference:

Investigating the Applicability of the Peak Density Thickness Parameter over the Equatorial Region
The early history of the Jicamarca Radio Observatory and the incoherent scatter technique

History of Geo- and Space Sciences

... The long pulses are transmitted using a single circular polarization with 1 MW of power per transmitter employed and with a negligeable power droop (Hysell et al., 2017). Although samples were acquired at a rate of 40 kHz, digital boxcar filtering for the long pulse experiment reduces the sampling interval to 50 μs, still twice the rate used in previous experiments (e.g., Hysell et al., 2015). ...

High-altitude incoherent-scatter measurements at Jicamarca: HIGH-ALTITUDE ISR
  • Citing Article
  • February 2017

... During some days, however, scintillation occurred until 02:00 LT. Figure 4b summarizes the magnetic zonal irregularity drift results. The drifts show a behavior that indeed is similar to what would be expected for background nighttime ionospheric plasma drifts at low latitudes (Fejer et al., 1991(Fejer et al., , 2005. The drifts are predominantly eastward, with larger values (120-200 m s −1 ) during the early evening, gradually decreasing to 20-80 m s −1 by midnight and into the postmidnight sector. ...

Average vertical and zonal F-region plasma drifts over Jicamarca
  • Citing Article
  • January 1991

Journal of Geophysical Research Atmospheres

... It is important to characterize this parameter throughout the atmosphere, the boundary layer, and above for the evaluation of laser atmospheric transmission. Measurement techniques, such as radar, scintillometers, ultrasonic anemometers, and micro-thermometers, have been used to measure C 2 n [4][5][6][7][8][9]. Since almost all methods of obtaining C 2 n using instruments are limited in the spatial-temporal domains, developing a less expensive and more convenient alternative is necessary. ...

Simultaneous observations of structure function parameter of refractive index using a high-resolution radar and the DataHawk small airborne measurement system

... A plasma drift velocity vortex in the zonal-vertical plane during the post-sunset period at equatorial latitudes was excellently imaged using Jicamarca incoherent scatter radar 6 . Post-sunset height gradients (vertical shears) in F-region zonal plasma drifts inferred from earlier Barium cloud release and coherent backscatter radar experiments [7][8][9] as well as the height gradients in F-region vertical plasma drifts 10,11 also appear to be associated with the evening velocity vortex. From Jicamarca radar observations, the velocity vortex is centered about 250 km altitude and about 2000-3000 km east of the sunset terminator. ...

Barium cloud observations of shear flow in the post sunset equatorial F-layer (abstract)
  • Citing Article
  • January 1980

Eos Transactions American Geophysical Union

... Cooperative synchronous observations ofwinds and tides were done at the end of November 1981, using the VHF radars at Jicamarca and Arecibo [9]. It was found that the lower stratospheric diurnal tide was similar, consistent with models, at locations symmetrical north (A0) and south (JRO) of the equator. ...

A Cooperative Synchronous Observation of Winds and Tides in the Tropical Lower Stratosphere and Mesosphere Using VHF Radars at Jicamarca and Arecibo
  • Citing Article
  • January 1986

Journal of geomagnetism and geoelectricity

... Previous studies over many years employing radar, lidar, airglow and cloud imaging, and in situ measurements of winds, temperatures, radar backscatter, airglow brightness, and cloud structures have provided evidence of KHI from the stable atmospheric boundary layer into the MLT [e.g., Witt, 1962;Ludlam, 1967;Hardy et al., 1969;Atlas et al., 1970;Browning, 1971;Gossard et al., 1971;Browning et al., 1973;Röttger and Schmidt, 1979;Klostermeyer and Ruster, 1981;Fritts and Rastogi, 1985;Eaton et al., 1995;Chapman and Browning, 1997;Chilson et al., 1997;Blumen et al., 2001;Hecht, 2004;Hecht et al., 2005;Kelley et al., 2005;Li et al., 2005aLi et al., , 2005bLehmacher et al., 2007;Luce et al., 2007Luce et al., , 2008Luce et al., , 2010Luce et al., , 2012Woodman et al., 2007;Pfrommer et al., 2009;Fukao et al., 2011]. A number of these studies attempted to quantify the KHI scales, characteristics, and environments. ...

The MPI-SOUSY-VHF Radar at Jicamarca: High Altitude-Resolution Capabilities

... Some observations presented by Djuth et al. (1994, see plates 1 and 2) demonstrate that the overshoot in the HFPL occurs~2 s after the pump is initially switched on, and thereafter, the HFPL becomes weaker in intensity with increasing time. Some explanations claim that the overshoot may be caused either by the pump inducing field-aligned irregularities, which scatter the pump before the pump can arrive at the parametric resonance altitude (Das & Fejer, 1979;Fejer, 1979;Fejer et al., 1983;Showen & Kim, 1978), or by the anomalous absorption of the pump attributed to the excitation of small-scale field-aligned irregularities beneath the parametric resonance altitude (Fejer, 1979;Fejer & Kopka, 1981;Gurevich, 2007). Additionally, Muldrew (1978) suggested that the overshoot may be due to the effects of ionospheric heating on the ducts and on the ambient plasma. ...

Observations of the HF-enhanced plasma line with a 46.8-MHz Radar and reinterpretation of previous observations with the 430-MHz radar
  • Citing Article
  • March 1983

Journal of Geophysical Research Atmospheres

... Equatorial spread-F free F-region vertical plasma drifts during the 2002 and 2004 storms were derived from Jicamarca ISR measurements with a 5-min integration time, following the procedure by Woodman (1970) and data processing techniques by Kudeki et al. (1999). The drift measurement accuracy ranged from ∼1 m/s during the day to ∼10 m/s at night. ...

A new approach in incoherent scatter F region E×B drift measurements at Jicamarca
  • Citing Article
  • December 1999

Journal of Geophysical Research Atmospheres

... For the purpose of the ABLH measurements reported in this paper, the WPR was operated in low mode, with a pulse length of 1 µs, which allows the lower troposphere to be sampled from 0.15 to 5.7 km a.g.l., with a vertical resolution of 150 m. The methodology applied to determine the ABLH relies on the identification of a distinctive strong peak in the WPR time-height reflectivity plot (Gage et al., 1990), which is associated with turbulence-generated radio refractive index fluctuations and associated atmospheric thermodynamic parameter fluctuations, though the strength of this peak may depend also on other factors. Wind profiling radars are sensitive to turbulence scales equal to half the radar wavelength. ...

A trans-Pacific network of wind-profiling Doppler radars for tropical atmospheric research
  • Citing Article
  • August 1989