Parametric coupling of a high‐frequency electromagnetic wave to whistler and lower‐hybrid waves in the ionosphere
Parametric coupling of a high‐frequency electromagnetic wave to an obliquely propagating whistler or lower‐hybrid wave and a high‐frequency sideband electromagnetic wave have been studied in the ionosphere. The growth rate of the three‐wave resonant interaction process decreases with the frequency o...
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Veröffentlicht in: | Physics of Plasmas 1996-01, Vol.3 (1), p.386-391 |
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description | Parametric coupling of a high‐frequency electromagnetic wave to an obliquely propagating whistler or lower‐hybrid wave and a high‐frequency sideband electromagnetic wave have been studied in the ionosphere. The growth rate of the three‐wave resonant interaction process decreases with the frequency of the lower‐hybrid wave and increases with whistler wave frequency. Growth rate is greater for the whistler wave than the lower‐hybrid wave. The electromagnetic wave is scattered at a larger angle in the case of the lower‐hybrid wave than the whistler wave. |
doi_str_mv | 10.1063/1.871864 |
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K.</creatorcontrib><creatorcontrib>Tripathi, V. K.</creatorcontrib><creatorcontrib>Singh, S. V.</creatorcontrib><title>Parametric coupling of a high‐frequency electromagnetic wave to whistler and lower‐hybrid waves in the ionosphere</title><title>Physics of Plasmas</title><description>Parametric coupling of a high‐frequency electromagnetic wave to an obliquely propagating whistler or lower‐hybrid wave and a high‐frequency sideband electromagnetic wave have been studied in the ionosphere. The growth rate of the three‐wave resonant interaction process decreases with the frequency of the lower‐hybrid wave and increases with whistler wave frequency. Growth rate is greater for the whistler wave than the lower‐hybrid wave. The electromagnetic wave is scattered at a larger angle in the case of the lower‐hybrid wave than the whistler wave.</description><subject>70 PLASMA PHYSICS AND FUSION</subject><subject>DISPERSION RELATIONS</subject><subject>DRIFT WAVES</subject><subject>ELECTRIC DISCHARGES</subject><subject>Electric fields</subject><subject>ELECTROMAGNETIC FIELDS</subject><subject>ELECTRON BEAMS</subject><subject>INSTABILITY GROWTH RATES</subject><subject>IONOSPHERE</subject><subject>LOWER HYBRID WAVES</subject><subject>MAGNETOPLASMA</subject><subject>Q1</subject><subject>WHISTLERS</subject><issn>1070-664X</issn><issn>1089-7674</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1996</creationdate><recordtype>article</recordtype><recordid>eNqd0M1KAzEQB_BFFKxV8BHiRfSwNdlkP3qU4hcU9KDgLWST2W5km6xJ2tKbj-Az-iSmrvgAXpJAfjPDf5LklOAJwQW9IpOqJFXB9pIRwdU0LYuS7e_eJU6Lgr0eJkfev2GMWZFXo2T1JJxYQnBaImlXfafNAtkGCdTqRfv18dk4eF-BkVsEHcjg7FIsDITIN2INKFi0abUPHTgkjEKd3YCLZe22dlr9GI-0QaEFpK2xvm_BwXFy0IjOw8nvPU5ebm-eZ_fp_PHuYXY9TyWtWEhFjYtc5USCUlQViqia1nU2FXlNs6aWMqMiq6SaNlUFmAEwELjMc0oEwyz-jpOzoa_1QXMvdQDZSmtMTMKznLLpzpwPpnc2JvWBL7WX0HXCgF15TvISl_GI8GKA0lnvHTS8d3op3JYTzHe754QPu4_0cqC7kSLE4P-ya-v-HO9VQ78BaE2W_A</recordid><startdate>199601</startdate><enddate>199601</enddate><creator>Sawhney, B. 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V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c384t-ab065d51cedd3d6d1db3bb29a5b32fbcc23a28cd9f88e04ee4ea075531a404c23</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1996</creationdate><topic>70 PLASMA PHYSICS AND FUSION</topic><topic>DISPERSION RELATIONS</topic><topic>DRIFT WAVES</topic><topic>ELECTRIC DISCHARGES</topic><topic>Electric fields</topic><topic>ELECTROMAGNETIC FIELDS</topic><topic>ELECTRON BEAMS</topic><topic>INSTABILITY GROWTH RATES</topic><topic>IONOSPHERE</topic><topic>LOWER HYBRID WAVES</topic><topic>MAGNETOPLASMA</topic><topic>Q1</topic><topic>WHISTLERS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sawhney, B. K.</creatorcontrib><creatorcontrib>Tripathi, V. K.</creatorcontrib><creatorcontrib>Singh, S. 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The growth rate of the three‐wave resonant interaction process decreases with the frequency of the lower‐hybrid wave and increases with whistler wave frequency. Growth rate is greater for the whistler wave than the lower‐hybrid wave. The electromagnetic wave is scattered at a larger angle in the case of the lower‐hybrid wave than the whistler wave.</abstract><cop>United States</cop><doi>10.1063/1.871864</doi><tpages>6</tpages><oa>free_for_read</oa></addata></record> |
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subjects | 70 PLASMA PHYSICS AND FUSION DISPERSION RELATIONS DRIFT WAVES ELECTRIC DISCHARGES Electric fields ELECTROMAGNETIC FIELDS ELECTRON BEAMS INSTABILITY GROWTH RATES IONOSPHERE LOWER HYBRID WAVES MAGNETOPLASMA Q1 WHISTLERS |
title | Parametric coupling of a high‐frequency electromagnetic wave to whistler and lower‐hybrid waves in the ionosphere |
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