Matches in SemOpenAlex for { <https://semopenalex.org/work/W2144007028> ?p ?o ?g. }
- W2144007028 endingPage "115" @default.
- W2144007028 startingPage "102" @default.
- W2144007028 abstract "Ionospheric scintillation effects encountered in the equatorial anomaly crest, polar cap, and auroral regions have been contrasted to provide information for the design and evaluation of the performance of multifrequency satellite communication links in these regions. The equatorial anomaly region is identified as the most disturbed irregularity environment where the amplitude and phase structures of 250 MHz and <tex xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>L</tex> -band scintillations are primarily dictated by the strength of scattering rather than ionospheric motion. In the anomaly region, the spectra of intense amplitude scintillations at these frequencies are characterized by uniform power spectral density from the lowest frequency (10 MHz) to 4 Hz at 257 MHz and to 1 Hz at <tex xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>L</tex> -band (1541 MHz) and steep rolloff at higher fluctuation frequencies with power law indexes of -5 to -7. Such structures are compatible with intensity decorrelation times of 0.1 and 0.3 s at 257 and 1541 MHz, respectively. The phase spectra at 244 MHz are described by power law variation of psd with frequency with typical spectral indexes of -2.4. The strong scattering at VHF induces extreme phase rates of 200° in 0.1 s. The 90th percentile values of rms phase deviation at 244 MHz with 100 s detrend are found to be 16 rad in the early evening hours, whereas amplitude scintillation can cover the entire dynamic range of 30 dB not only in the 250 MHz band but at <tex xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>L</tex> -band as well. In the polar cap, the 50th and 90th percentile values of rms phase deviation at 250 MHz for 82 s detrend are 3 and 12 rad, respectively, with comparable values being obtained in the auroral oval. The corresponding values for the S <inf xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>4</inf> index of scintillation are 0.5 and 0.8 in the polar cap, which are slightly higher than those recorded in the auroral oval. The power law index of phase scintillation at high latitudes is in the vicinity of -2.3, which is not a result of very strong turbulence as in the equatorial region but is considered to be a consequence of shallow irregularity spectral indexes. The phase rates at auroral locations are an order of magnitude smaller than in the equatorial region and attain values of 100° in 0.5 s. The extreme variability of ionospheric motion in the auroral oval sensitively controls the structure of scintillations. The long-term morphology (period 1979-1984) of intensity scintillations at 250 MHz in the polar cap shows that, in addition to the absence of diurnal variation of scintillations, and the presence of an annual variation with a pronounced minimum during local summer, there exists a marked solar control of scintillation activity such that it abruptly decreases when the solar activity falls below a threshold level." @default.
- W2144007028 created "2016-06-24" @default.
- W2144007028 creator A5003648708 @default.
- W2144007028 creator A5019373231 @default.
- W2144007028 creator A5039458429 @default.
- W2144007028 creator A5065753963 @default.
- W2144007028 creator A5074516494 @default.
- W2144007028 creator A5087010391 @default.
- W2144007028 date "1987-02-01" @default.
- W2144007028 modified "2023-10-02" @default.
- W2144007028 title "250 MHz/GHz Scintillation Parameters in the Equatorial, Polar, and Auroral Environments" @default.
- W2144007028 cites W158214443 @default.
- W2144007028 cites W1657438361 @default.
- W2144007028 cites W1965150733 @default.
- W2144007028 cites W1965804552 @default.
- W2144007028 cites W1976655320 @default.
- W2144007028 cites W1976763434 @default.
- W2144007028 cites W1987067454 @default.
- W2144007028 cites W1990906781 @default.
- W2144007028 cites W2003358819 @default.
- W2144007028 cites W2013591932 @default.
- W2144007028 cites W2016942624 @default.
- W2144007028 cites W2024349183 @default.
- W2144007028 cites W2025898679 @default.
- W2144007028 cites W2027439186 @default.
- W2144007028 cites W2027572881 @default.
- W2144007028 cites W2028328369 @default.
- W2144007028 cites W2038866002 @default.
- W2144007028 cites W2039085133 @default.
- W2144007028 cites W2041462866 @default.
- W2144007028 cites W2044135361 @default.
- W2144007028 cites W2051363631 @default.
- W2144007028 cites W2054519737 @default.
- W2144007028 cites W2084766967 @default.
- W2144007028 cites W2096332652 @default.
- W2144007028 cites W2106809543 @default.
- W2144007028 cites W2146701114 @default.
- W2144007028 cites W2154463718 @default.
- W2144007028 cites W2167015626 @default.
- W2144007028 cites W2995722939 @default.
- W2144007028 doi "https://doi.org/10.1109/jsac.1987.1146533" @default.
- W2144007028 hasPublicationYear "1987" @default.
- W2144007028 type Work @default.
- W2144007028 sameAs 2144007028 @default.
- W2144007028 citedByCount "66" @default.
- W2144007028 countsByYear W21440070282012 @default.
- W2144007028 countsByYear W21440070282013 @default.
- W2144007028 countsByYear W21440070282014 @default.
- W2144007028 countsByYear W21440070282015 @default.
- W2144007028 countsByYear W21440070282016 @default.
- W2144007028 countsByYear W21440070282017 @default.
- W2144007028 countsByYear W21440070282018 @default.
- W2144007028 countsByYear W21440070282019 @default.
- W2144007028 countsByYear W21440070282020 @default.
- W2144007028 countsByYear W21440070282021 @default.
- W2144007028 countsByYear W21440070282023 @default.
- W2144007028 crossrefType "journal-article" @default.
- W2144007028 hasAuthorship W2144007028A5003648708 @default.
- W2144007028 hasAuthorship W2144007028A5019373231 @default.
- W2144007028 hasAuthorship W2144007028A5039458429 @default.
- W2144007028 hasAuthorship W2144007028A5065753963 @default.
- W2144007028 hasAuthorship W2144007028A5074516494 @default.
- W2144007028 hasAuthorship W2144007028A5087010391 @default.
- W2144007028 hasBestOaLocation W21440070282 @default.
- W2144007028 hasConcept C102637530 @default.
- W2144007028 hasConcept C108411613 @default.
- W2144007028 hasConcept C10880902 @default.
- W2144007028 hasConcept C115260700 @default.
- W2144007028 hasConcept C116403925 @default.
- W2144007028 hasConcept C120665830 @default.
- W2144007028 hasConcept C121332964 @default.
- W2144007028 hasConcept C1276947 @default.
- W2144007028 hasConcept C12997251 @default.
- W2144007028 hasConcept C168110828 @default.
- W2144007028 hasConcept C180205008 @default.
- W2144007028 hasConcept C191486275 @default.
- W2144007028 hasConcept C26873012 @default.
- W2144007028 hasConcept C29705727 @default.
- W2144007028 hasConcept C30475298 @default.
- W2144007028 hasConcept C41008148 @default.
- W2144007028 hasConcept C44280652 @default.
- W2144007028 hasConcept C62520636 @default.
- W2144007028 hasConcept C72886185 @default.
- W2144007028 hasConcept C76155785 @default.
- W2144007028 hasConcept C8058405 @default.
- W2144007028 hasConcept C94915269 @default.
- W2144007028 hasConceptScore W2144007028C102637530 @default.
- W2144007028 hasConceptScore W2144007028C108411613 @default.
- W2144007028 hasConceptScore W2144007028C10880902 @default.
- W2144007028 hasConceptScore W2144007028C115260700 @default.
- W2144007028 hasConceptScore W2144007028C116403925 @default.
- W2144007028 hasConceptScore W2144007028C120665830 @default.
- W2144007028 hasConceptScore W2144007028C121332964 @default.
- W2144007028 hasConceptScore W2144007028C1276947 @default.
- W2144007028 hasConceptScore W2144007028C12997251 @default.
- W2144007028 hasConceptScore W2144007028C168110828 @default.
- W2144007028 hasConceptScore W2144007028C180205008 @default.
- W2144007028 hasConceptScore W2144007028C191486275 @default.