J. Klenzing’s research while affiliated with National Aeronautics and Space Administration and other places

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Publications (49)


Resolving the generation mechanisms and electrodynamical effects of Medium Scale Traveling Ionospheric Disturbances (MSTIDs)
  • Article
  • Full-text available

February 2025

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65 Reads

Frontiers in Astronomy and Space Sciences

Jeff Klenzing

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Kate Zawdie

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The term “Medium-Scale Traveling Ionospheric Disturbances” is used to describe a number of different propagating phenomena in ionospheric plasma density with a scale size of hundreds of km. This includes multiple generation mechanisms, including ion-neutral collisions, plasma instabilities, and electromagnetic forcing. Observational limitations can impede characterization and identification of MSTID generation mechanisms. We discuss inconsistencies in the current terminology used to describe these and provide a set of recommendations for description and discussion.

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Top, probability distributions of atmospheric density at GRACE‐B as a function of (a) quiet‐ and storm‐times, (b) quiet‐times and storm main phase, and (c) quiet times and storm recovery phase. Bottom, cumulative distributions of atmospheric density as a function of (d) quiet‐ and storm‐times, (e) quiet‐times and storm main phase, and (f) quiet‐times and storm recovery phase. The green line in the cumulative distributions shows the maximum difference between each plot's quiet‐time distribution and storm distribution. The KS statistic (Max Difference) and p‐value are shown in the legend.
Correlation matrices for atmospheric density and (a) solar indices, (b) the FISM2 data set and (c) solar wind data and geomagnetic indices (y‐axis) as a function of all‐time, quiet‐time, storm‐time and storm main and recovery phases (x‐axis). The color and number indicate the absolute value of the correlation.
Metrics for the three Random Forest models as a function of data set; train, test, and GRACE A and CHAMP out of sample (OOS). (a) The square of the correlation coefficients. (b) The mean absolute error.
The MDA feature importance for the FISM (top) and FISM/GEO models (bottom). In both panels, the features are ranked from most important (top) to least important (bottom).
Select case studies comparing observed density from the out‐of‐sample CHAMP data set, and those derived from the three Random Forest models and the NRLMSIS model along the orbit of CHAMP during a (a) geomagnetically quiet period, (c) small geomagnetic storm, (c) moderate geomagnetic storm, and (d) large geomagnetic storm. From top to bottom, each panel shows (i) Sym‐H, (ii) AE, (iii) CHAMP observed density, (iv) model‐data comparison and (v) the Mean Absolute Error (MAE, lower is better). In panels (iv) and (v) the densities and MAE have been averaged with a 90 min rolling window to make comparisons easier, highlight the background change in density during each storm, and illustrate how the errors (MAE) change throughout each case study. Observed densities are blue, FISM/GEO modeled densities orange, FISM modeled densities green, solar‐modeled densities red, and NRLMSIS densities are purple.

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Understanding and Modeling the Dynamics of Storm‐Time Atmospheric Neutral Density Using Random Forests

January 2025

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22 Reads

Atmospheric neutral density is a crucial component to accurately predict and track the motion of satellites. During periods of elevated solar and geomagnetic activity atmospheric neutral density becomes highly variable and dynamic. This variability and enhanced dynamics make it difficult to accurately model neutral density leading to increased errors which propagate from neutral density models through to orbit propagation models. In this paper we investigate the dynamics of neutral density during geomagnetic storms. We use a combination of solar and geomagnetic variables to develop three Random Forest machine learning models of neutral density. These models are based on (a) slow solar indices, (b) high cadence solar irradiance, and (c) combined high‐cadence solar irradiance and geomagnetic indices. Each model is validated using an out‐of‐sample data set using analysis of residuals and typical metrics. During quiet‐times, all three models perform well; however, during geomagnetic storms, the combined high cadence solar iradiance/geomagnetic model performs significantly better than the models based solely on solar activity. The combined model capturing an additional 10% in the variability of density and having an error up to six times smaller during geomagnetic storms then the solar models. Overall, this work demonstrates the importance of including geomagnetic activity in the modeling of atmospheric density and serves as a proof of concept for using machine learning algorithms to model, and in the future forecast atmospheric density for operational use.


The available MGS MAG data on SPDF. The added data products (when compared to PDS data files) are listed in bold text.
Additions to Space Physics Data Facility and pysatNASA: Increasing Mars Global Surveyor and Mars Atmosphere and Volatile EvolutioN Dataset Utility

November 2024

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12 Reads

The Space Physics Data Facility (SPDF) is a digital archive of space physics data and is useful for the storage, analysis, and dissemination of data. We discuss the process used to create an amended dataset and store it on the SPDF. The operational software to generate the archival data software uses the open-source Python package pysat, and an end-user module has been added to the pysatNASA module. The result is the addition of data products to the Mars Global Surveyor (MGS) magnetometer (MAG) dataset, its archival location on SPDF, and pysat compatibility. The primary and metadata format increases the convenience and efficiency for users of the MGS MAG data. The storage of planetary and heliophysics data in one location supports the use of data throughout the solar system for comparison, while pysat compatibility enables loading data in an identical format for ease of processing. We encourage the use of the outlined process for past, present, and future space science missions of all sizes and funding levels. This includes balloons to Flagship-class missions.


Panel (a): the geometry of a spacecraft orbiting obliquely against Earth's magnetic field lines near the magnetic equator, making an angle α against the field‐line. Panel (b): the spacecraft velocity vector (vsc), and its field‐parallel and field‐perpendicular components (v‖ and v⊥). Note that even though the sketch is 2‐dimensional, we explicitly calculate the full 3D‐angle. Panel (c): Equation 3 for three selected frequencies, as a function of α. Panel (d) shows a crossing of the equator by Swarm A on 25 October 2014, around 01:00 UT, at a solar local time of 21 hr. The observed plasma density (black), a Hermite polynomial fit (red), and a 1‐min median filter applied to the density (gray). The geographic and geomagnetic latitudes of the orbit are displayed on two x‐axes below the panel (using the Solar Magnetic coordinate system, Hapgood, 1992). The three Roman numerals in panel (d) refer to the next three panels. Panels (e–g) show example irregularity spectra that are subject to a statistical analysis in the present paper. The three panels show spectra calculated at denoted by green Roman numerals in Panel (d). The two density perturbation spectra are shown in black and gray, while an absolute density spectrum is shown in red. Nominal and α‐adjusted spatial scales (Equation 3) are indicated along the two lower x‐axes. For a detailed view of this particular crossing of the equator, see Figure S1 in Supporting Information S1.
Overall absolute density variance (RMS) binned by solar local time (panel a). Number of spectra observed per local time bin, with various solar terminators indicated (panel b). Binned median power across 16 frequencies, with frequency indicated (panels c–r). Each of the 16 panels shows median PSD in black (shaded gray region showing upper‐ and lower‐ quartile distributions), with the trace of the overall RMS data shown in a thin red line. Exponential fits (Equation 6) are shown in green, with structure lifetimes τ indicated. For a version of this figure based on relative density (contrast) spectra, see the Figure S4 in Supporting Information S1.
Panel (a): The linear gradient (in LT) of the natural logarithm of the median (absolute density) PSD, after it was binned by α‐adjusted frequency (y‐axis) and LT (x‐axis). The decay rate inferred from this gradient is shown with a colorscale. Panel (b): The exponential decay rates from Figure 2 for all frequencies post‐sunset (green and blue lines). Shaded areas indicate the 95‐percent confidence intervals of the exponential fits. The results from HK97 are plotted with four, thin red lines, representing four different measurements from the AE‐E satellite. An ambipolar diffusion power law is shown in a dashed black line, while a constant 1.4 hr lifetime is shown with a solid black line.
Plasma Structure Decay Rates in the Equatorial Ionosphere Are Strongly Coupled by Turbulence

September 2024

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52 Reads

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1 Citation

Equatorial plasma irregularities in the ionospheric F‐region proliferate after sunset, causing the most apparent radio scintillation “hot‐spot” in geospace. These irregularities are caused by plasma instabilities, and appear mostly in the form of under‐densities that rise up from the F‐region's bottomside. After an irregularity production peak at sunset, the amplitude of the resulting turbulence decays with time. Analyzing a large database of irregularity spectra observed by one of the European Space Agency's Swarm satellites, we have applied a novel but conceptually simple statistical analysis to the data, finding that turbulence in the F‐region tends to decay with a uniform, scale‐independent rate, thereby confirming and extending the results from an earlier case study. We find evidence for two regimes, one valid post‐sunset (1.4 hr decay rate) and one valid post‐midnight (2.6 hr). Our results should be of utility for large‐scale space weather modeling efforts that are unable to resolve turbulent effects.



Kinetic Modeling of Ionospheric Outflows in Pressure Cooker Environments

December 2023

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39 Reads

Plasma escape from the high‐latitude ionosphere (ion outflow) serves as a significant source of heavy plasma to the magnetospheric plasma sheet and ring current regions. Outflows alter mass density and reconnection rates, hence global responses of the magnetosphere. A new fully kinetic and semi‐kinetic model, KAOS (Kinetic model of Auroral ion OutflowS), is constructed from first principles which traces large numbers of individual O⁺ ion macro‐particles along curved magnetic field lines, using a guiding‐center approximation, in order to facilitate calculation of ion distribution functions and moments. Particle forces include mirror and parallel electric field forces, a self‐consistent ambipolar electric field, and a parameterized source of ion cyclotron resonance wave heating, thought to be central to the transverse energization of ions. The model is initiated with a steady‐state ion density altitude profile and Maxwellian velocity distribution and particle trajectories are advanced via a direct simulation Monte Carlo scheme. This outlines the implementation of the kinetic outflow model, demonstrates the model's ability to achieve near‐hydrostatic equilibrium necessary for simulation spin‐up, and investigates L‐shell dependent wave heating and pressure cookers scenarios. This paper illustrates the model initialization process and numerical investigations of L‐shell dependent outflows and pressure cooker environments and serves to advance our understanding of the drivers and particle dynamics in the auroral ionosphere.


The importance of recruitment and retention in Heliophysics: it’s not just a pipeline problem

August 2023

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80 Reads

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1 Citation

Frontiers in Astronomy and Space Sciences

A major obstacle in cultivating a robust Heliophysics (and broader scientific) community is the lack of diversity throughout science, technology, engineering, and mathematics (STEM) fields. For many years, this has been understood as a “leaky pipeline” analogy, in which predominately minority students initially interested in STEM gradually fall (or are pushed) out of the field on their way to a scientific research position. However, this ignores critical structural and policy issues which drive even later career Ph.D.s out of a career in Heliophysics. We identify here several systemic problems that inhibit many from participating fully in the Heliophysics community, including soft money pressure, lack of accessibility and equity, power imbalances, lack of accountability, friction in collaboration, and difficulties in forming mentorship bonds. We present several recommendations to empower research-supporting organizations to help create a culture of inclusion, openness, and innovative science.


Statistical analysis of Low latitude Spread F at the American, Atlantic and Pacific sectors using digisonde observations

August 2023

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64 Reads

Digisonde data from three different longitude sectors from Jicamarca (12°S, 76.8°W, -2.5° declination angle) from 2001–2016, Ascension Island (7.9°S, 14.4°W, -15.09° declination angle) from 2000–2014, Kwajalein (8.71°N, 167.7°E, 7.5° declination angle) from 2004–2012, has been processed and analyzed to determine statistical studies of equatorial spread F, a diagnostic of irregular plasma structure in the ionosphere. A new method of spread F detection for low latitude region is used to determine solar and seasonal variation over these three sites. An algorithm has been developed to detect the foF2 and hmF2 values from an ionogram and this has been validated using manually scaled ionograms, as well as comparisons to the SAMI2 and IRI models.



Citations (27)


... It involves particle precipitation, which creates beams of electrons that modulate conductivity (ionization) and electric fields [63]. Those modulations produce gradientdrift unstable structures [56], whose imminent decay into smaller and smaller pieces, the turbulent cascade, systematically breaks apart structures smaller in size than around 1-10 km [64,65]. The shapes, or rather, their stochastic features, are subsequently repeated in a selfsimilar pattern that reaches as small as meter-scale in magnification, at which point the initial perturbations will have seeded the Farley-Buneman instability and saturating its growth rates (see Figure 5 for a schematic illustration of this cascading process). ...

Reference:

A Characteristic Signature of Magnetospheric Wave-Particle Interactions Found in the Turbulent E-region
Plasma Structure Decay Rates in the Equatorial Ionosphere Are Strongly Coupled by Turbulence

... Beyond giving RSEs credit, a good model-sharing practice is to standardize their roles and enable their career development [57]. This requires a more fundamental shift in how RSEs are evaluated in the workplace, as applying traditional academic norms to this emerging role is driving them away from research contexts and depleting the sciences of the skills and experience needed to tackle complex problems [58]. ...

Advocating for Equality of Contribution: The Research Software Engineer (RSE)

... The situation is worse for those with multiple marginalized identities because intersectionality compounds the inequalities (e.g., Clancy et al., 2017;Kozlowski et al., 2022). Following the ten simple rules towards healthier research labs of Maestre (2019), Halford et al. (2023) give many ways in which space scientists can improve the workplace. This includes thinking beyond our normal close-knit colleagues when forming a new team. ...

The importance of recruitment and retention in Heliophysics: it’s not just a pipeline problem

Frontiers in Astronomy and Space Sciences

... This involves promoting a culture that values and celebrates diversity, where all members of the community feel safe, respected, and supported (Adamu, 2013: Groggins, & Ryan, 2013. Cultivating such a climate requires proactive efforts to address biases, stereotypes, and discriminatory behaviors (Halford et al., 2023). ...

Cultivating a culture of inclusivity in heliophysics

Frontiers in Physics

... The understanding of these impacts is also important for robust high frequency (HF) communication, over-the-horizon radar operation and for the need of accurate predictions of ionospheric state for precise pointing positioning applications (Paziewski et al., 2022;Timoté et al., 2020). Likewise, these waves may also favor the seeding of plasma irregularities at low-latitude region, which, in turn, may results in the disruption of satellite navigation and communication (Huba & Liu, 2020;Klenzing et al., 2023). ...

A system science perspective of the drivers of equatorial plasma bubbles

Frontiers in Astronomy and Space Sciences

... It models the plasma along the geomagnetic field lines including ion inertia in the ion momentum equation for motion along the dipole field line (Zhan & Rodrigues, 2018). The SAMI2 model calculates the evolution of the low-to mid-latitude ionosphere in the altitude range 85 to 20,000 km (Klenzing et al., 2022). This corresponds to a latitudinal extent of ±62.5°about the magnetic equator. ...

sami2py—Overview and applications

Frontiers in Astronomy and Space Sciences

... Many questions remain about the generation, propagation, and effects of MSTIDs. A recent paper describes many of the outstanding problems for TIDs driven by Atmospheric Gravity Waves (AGWs) (Zawdie et al., 2022). While the Zawdie et al. (2022) paper describes questions related to AGW driven TIDs, there are also remaining questions about other types of TIDs. ...

Impacts of acoustic and gravity waves on the ionosphere

Frontiers in Astronomy and Space Sciences

... Since the early 20th century, the LTI has been studied extensively using ground-based remote sensing facilities such as ionosondes and radars, but in all aspects requiring in situ observations, it remains underexplored territory. Rocket flights (e.g., Sangalli et al., 2009;Pfaff et al., 2022a) can offer only local and temporally confined information. Major technical challenges have so far prevented a satellite mission to the deep, dense part of the LTI, despite scientific interest, community proposals, and feasibility studies by major space agencies (e.g., Grebowsky and Gervin, 2001;Pfaff et al., 2022b). ...

Dual Sounding Rocket and C/NOFS Satellite Observations of DC Electric Fields and Plasma Density in the Equatorial E‐ and F‐Region Ionosphere at Sunset

... While magnetospheric parallel electric fields have long been associated with auroral particle acceleration and precipitation (Marklund, 1993;Paschmann et al., 2003;Shelley, 1995), static current closure models predict parallel electric fields from the ionospheric F-region to the E-region to be orders of magnitude weaker than perpendicular 10.1029/2023GL106073 9 of 11 fields (μV/m rather than mV/m) (e.g., Farley Jr, 1959). Ionospheric electric field measurements routinely assume zero parallel electric field when deriving a full vector perpendicular field from two-dimensional measurements (Pfaff et al., 2021). However, satellite measurements of enhanced downward currents and modeling of the ionospheric response suggest significant parallel fields in the collisional base of the D and E regions (Karlsson & Marklund, 1998;Marklund et al., 1997), but to our knowledge, no measurements have probed the existence of these fields. ...

The Vector Electric Field Investigation (VEFI) on the C/NOFS Satellite

Space Science Reviews

... Intriguingly, the growth rate of GRT instability has been found to display similar uncertainty (e.g., Aa et al., 2023;Das et al., 2021;Shinagawa et al., 2018). Since the EPD occurrence shows a large variability both in small-and large-longitudinal scales (e.g., Kil & Heelis, 1998a;Kil et al., 2009;Martinis et al., 2021;Singh et al., 1997;Stolle et al., 2008;Tsunoda et al., 2018;Tsunoda & White, 1981), predicting EPD occurrence becomes even more challenging. Now, it is fairly well understood that missing understanding of the spatio-temporal behavior of EPDs, that is, growth, zonal movement and decay of EPDs, along with the paucity of continuous measurements of ionospheric parameters is the cause for the challenge in predicting the day-to-day occurrence variability of EPDs (e.g., Das et al., 2021;Hysell et al., 2021;Li et al., 2021;Patra & Das, 2023). ...

Longitudinal Variation of Postsunset Plasma Depletions From the Global‐Scale Observations of the Limb and Disk (GOLD) Mission