Observatoire de Paris-PSL CNRS vopdc cdpp Sorbonne Université cnes Université de Paris LESIA

Juno/Waves estimated flux density Collection (Version 02)

Thursday 6 June 2024, by Baptiste Cecconi, Corentin Louis, Philippe Zarka

This collection contains the Version 02 of the Juno/Waves dataset processed using the method described in Louis et al (2021a), applied to version 02 of the Juno/Waves dataset stored at the PDS (Kurth & Piker, 2023)


This collection is a new version of:


Link to data repository

How to display the data

To display this dataset easily, we recommend using the Autoplot software (Faden et al., 2010). Once the software is installed, just load the juno-waves-flux_density_v02.vap file by doing `File>Open .vap file...’

juno-waves_flux_density_v02.vap.zip

Description

This datasets contain the Juno/Waves estimated flux density based on Cassini/RPWS measurements at Jupiter.

How are the flux density estimated?
The pipeline use to calculate this estimated flux density is freely accessible at Louis et al. (2023)

The steps to derive the flux density are the following :

  • Use V02 times series from PDS data in linear scale (Kurth & Piker, 2023).
  • Apply FFT filtering to remove interferences
  • Subtract a background (calculated from dB values) in linear scale
  • For LFR and HFR-High sub-receivers:
    • Correct for 1/R2 dependence
    • Select data intervals of 4 consecutive Jovian rotation with 15° < Latitudemagnetic < 15° and Distance > 30 RJ (same configuration than Cassini)
    • Build median 1% and 50% occurrence spectra and match with Cassini-RPWS and Voyager-PRA ones (Zarka 1992, Zarka et al. 2004) to derive a gain table between 3.5 kHz and 40.5 MHZ.
    • Extrapolate the gains down to 1 kHz
  • For the HFR-Low sub-receiver:
    • No 1/R2 dependence correction
    • Select data acquired during the ±2 hours around perijoves (when signal is observed by this sub-receiver)
    • Use the continuity of the signal between the LFR-High, HFR-Low and HFR-High sub-receiver to determine the HFR-Low gains.

Once the gains have been obtain, the steps to estimate the density flux are the following :

  • Use PDS V02 data in linear scale, resample to 1 second
  • Apply an FFT-filtering by selecting the first eight harmonic of the spacecraft spin—period, with a width of δf=7% of the frequency around the peaks
  • Apply the gains of Table 1 (3rd row) which gives local-estimated flux densities
  • Optionally, correct for 1/R2 dependence to normalize the flux to a constant distance. This should not be done e.g. when studying local wave Electric-field, but should be done when studying the statistical latitudinal distribution of the radio beaming, as in the Louis et al. (2021a) study.
  • Optionally subtract the time-independent background in linear scale of Table 1 (4th row)

A complete description of the methodology used to estimate the flux density can be found in Louis et al. (2021a).

List of Datasets

  • IDL save files
    • dataset at a temporal resolution of 1 second or 15 seconds containing the estimated flux density data with the intensity values in linear (ZLINCAL variable)
  • CDF files
    • dataset at a temporal resolution of 1 second, containing the estimated flux density data with the intensity values in linear (data variable), the gain, the background and the background standard deviation values.
  • Quicklook

Rules of use

  • We kindly request the authors of any communications and publications using these data to let us know about them, include minimal citation to the reference below and appropriate acknowledgements whenever needed.
  • References: Louis et al. (2021a, doi)
  • Acknowledgements: see the acknowledgement field

Link to the data at PDS

Acknowledgements
The MASER Juno/Waves CDR collection has been calculated by C. Louis, P. Zarka, K. Dabidin, P.-A. Lampson, F. Magalhaes, A. Boudouma, M. Marques and B. Cecconi. The authors acknowledge the Observatoire de Paris, CNES, CNRS for funding and supporting this work and B. Kurth and the University of Iowa and the Juno/Waves team for providing access to the Juno/Waves data accessible online from PDS at https://doi.org/10.17189/1520498. The authors thank J. Faden and C. Piker for their work on the Autoplot software.

BC was also supported by PADC and EPN2024-RI. The Europlanet 2024 Research Infrastructure (EPN2024-RI) project has received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement No 871149.

Contact
Any question or request should be addressed to contact.maser@obspm.fr

Appendix

Table 1
Gains (3rd row) and Unique background (4th row) at each frequency calculated from the FFT-filtered-background subtracted data over the whole 3–year interval studied (2016100–2019174). The gains are separately calculated for the LFR and HFR-High sub-receivers and the HFR-Low sub-receiver. The background is computed as a robust mean of the FFT-filtered values expressed in dB (for compressing the dynamic range). It is then converted back to linear values
LFR-Low
Waves channelFrequency (kHz)GainBackground (V2.m-2.Hz-1)
0 0.04883 27.464 7.637e-09
1 0.09766 27.464 5.066e-09
2 0.14648 27.464 2.035e-09
3 0.19531 27.464 6.843e-10
4 0.24414 27.464 2.801e-10
5 0.29297 27.464 1.523e-10
6 0.34180 27.464 9.500e-11
7 0.39062 27.464 6.532e-11
8 0.43945 27.464 6.291e-11
9 0.48828 27.464 1.012e-10
10 0.53711 27.464 6.866e-11
11 0.58594 27.464 3.046e-11
12 0.63477 27.464 2.596e-11
13 0.70801 27.464 1.845e-11
14 0.80566 27.464 1.510e-11
15 0.90332 27.464 1.259e-11
16 1.00100 27.464 1.045e-11
17 1.12300 27.464 6.947e-12
18 1.26950 27.464 5.264e-12
19 1.41600 27.464 5.257e-12
20 1.58690 27.464 2.714e-12
21 1.78220 27.464 1.872e-12
22 2.00200 27.464 1.239e-12
23 2.24610 27.464 8.624e-13
24 2.51470 27.464 5.796e-13
25 2.83200 27.464 4.244e-13
26 3.17380 27.464 2.916e-13
27 3.54000 27.464 2.110e-13
28 3.97950 27.464 1.540e-13
29 4.46780 27.464 1.234e-13
30 5.00490 27.464 9.833e-14
31 5.61520 32.002 9.423e-14
32 6.29880 34.337 8.365e-14
33 7.08010 35.228 7.304e-14
34 7.95900 34.178 6.175e-14
35 8.93550 31.112 5.004e-14
36 10.0100 29.905 4.397e-14
37 11.2300 30.062 4.632e-14
38 12.6220 28.532 4.407e-14
39 14.1600 24.996 3.486e-14
40 15.8690 20.540 2.611e-14
41 17.7980 15.477 2.178e-14
42 19.9710 11.517 2.025e-14
LFR-High
Waves channelFrequency (kHz)GainBackground (V2.m-2.Hz-1)
43 19.9580 17.232 1.161e-14
44 22.3390 16.993 9.766e-15
45 25.0850 16.510 8.758e-15
46 28.1980 16.259 8.003e-15
47 31.6770 14.982 7.354e-15
48 35.5220 13.228 6.495e-15
49 39.9170 11.728 5.093e-15
50 44.8610 9.983 4.179e-15
51 50.1710 8.387 3.363e-15
52 56.2130 7.046 3.040e-15
53 63.1710 5.996 2.437e-15
54 70.8620 5.269 2.138e-15
55 79.4680 4.829 2.034e-15
56 89.1720 5.151 2.199e-15
57 100.160 5.844 2.527e-15
58 112.430 6.332 2.617e-15
59 126.160 8.434 3.290e-15
60 141.540 13.206 4.814e-15
HFR-Low
Waves channelFrequency (kHz)GainBackground (V2.m-2.Hz-1)
61 140.140 13.206 3.931e-11
62 157.230 12.160 3.449e-11
63 177.730 11.196 3.250e-11
64 198.240 10.309 2.945e-11
65 222.170 9.492 2.426e-11
66 249.510 8.740 1.645e-11
67 280.270 8.047 8.565e-12
68 314.450 7.409 5.740e-12
69 352.050 6.822 4.687e-12
70 396.480 6.281 3.774e-12
71 447.750 5.784 2.886e-12
72 502.440 5.325 2.530e-12
73 563.960 4.903 2.050e-12
74 632.320 4.515 1.849e-12
75 707.520 4.157 1.598e-12
76 796.390 3.827 1.486e-12
77 895.510 3.524 1.821e-12
78 1001.50 3.245 2.286e-12
79 1121.10 2.988 3.395e-12
80 1261.20 2.751 2.232e-12
81 1415.00 2.533 8.184e-13
82 1585.90 2.332 1.008e-12
83 1780.80 2.147 7.029e-13
84 1999.50 1.977 7.428e-13
85 2242.20 1.820 1.126e-12
86 2515.60 1.676 5.042e-13
87 2823.20 1.543 2.413e-13
HFR-High
Waves channelFrequency (kHz)GainBackground (V2.m-2.Hz-1)
88 3500.00 1.421 1.275e-15
89 4500.00 1.585 1.251e-15
90 5500.00 1.079 1.477e-15
91 6500.00 1.326 1.969e-15
92 7500.00 3.505 2.262e-15
93 8500.00 2.868 2.425e-14
94 9500.00 2.726 6.316e-15
95 10500.0 3.241 1.052e-14
96 11500.0 2.704 2.507e-15
97 12500.0 3.362 1.236e-14
98 13500.0 2.938 7.924e-15
99 14500.0 3.471 7.334e-15
100 15500.0 2.848 8.573e-15
101 16500.0 4.338 1.373e-14
102 17500.0 4.545 7.451e-15
103 18500.0 4.381 9.723e-15
104 19500.0 3.726 8.740e-15
105 20500.0 0.219 1.662e-14
106 21500.0 0.501 2.631e-14
107 22500.0 9.570 1.788e-14
108 23500.0 9.757 1.725e-14
109 24500.0 9.477 1.669e-14
110 25500.0 5.540 2.448e-14
111 26500.0 6.671 7.649e-15
112 27500.0 5.626 1.491e-14
113 28500.0 2.106 2.177e-14
114 29500.0 4.310 1.656e-14
115 30500.0 3.123 1.965e-14
116 31500.0 0.486 9.543e-15
117 32500.0 2.297 1.502e-14
118 33500.0 2.655 5.850e-15
119 34500.0 0.429 1.172e-14
120 35500.0 0.754 1.088e-14
121 36500.0 0.699 2.165e-15
122 37500.0 0.138 3.066e-15
123 38500.0 0.113 1.899e-15
124 39500.0 0.047 7.823e-16
125 40500.0 0.007 3.477e-16

References

  • Faden, J.B., Weigel, R.S., Merka, J. et al. Autoplot: a browser for scientific data on the web. Earth Sci Inform 3, 41–49 (2010), doi: 10.1007/s12145-010-0049-0.
  • Kurth, W.S., and Piker C.W., JUNO E/J/S/SS WAVES CALIBRATED SURVEY FULL RESOLUTION V2.0, JNO-E/J/SS-WAV-3-CDR-SRVFULL-V2.0, NASA Planetary Data System, 2022, doi: 10.17189/1520498.
  • Louis, C. K., Zarka, P., Dabidin, K., Lampson, P.-A., Magalhães, F. P., Boudouma, A., et al. (2021a). Latitudinal beaming of Jupiter’s radio emissions from Juno/Waves flux density measurements. Journal of Geophysical Research: Space Physics, 126, e2021JA029435, doi: 10.1029/2021JA029435.
  • Louis, C. K., Zarka, P., Cecconi, B. (2021b). Juno/Waves estimated flux density Collection (Version 01) [Data set], PADC, doi: 10.25935/6jg4-mk86
  • Zarka, P. (1992). The auroral radio emissions from planetary magnetospheres: What do we know, what don’t we know, what do we learn from them? Advances in Space Research, 12(8), 99–115, doi: 10.1016/0273-1177(92)90383-9.
  • Zarka, P., Cecconi, B., & Kurth, W. S. (2004). Jupiter’s low-frequency radio spectrum from Cassini/Radio and Plasma Wave Science (RPWS)
    absolute flux density measurements. Journal of Geophysical Research, 109, A09S15, doi: 10.1029/2003JA010260.