FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2105843450> ?p ?o ?g. }

• W2105843450 endingPage "186" @default.
• W2105843450 startingPage "159" @default.
• W2105843450 abstract "An analytical technique referred to as the propagator ma- trix method (PMM) is presented to study the problem of electromag- netic (EM) waves interacting with the nonuniform magnetized plasma. In this method, the state vector is proposed to describe the characteris- tics of eigen waves in anisotropic medium, and state vectors at two dif- ferent locations are related with each other by the propagator matrix. This method can be used to deal with the phenomenon of the trans- formation of EM wave polarization induced by anisotropic magnetized plasma, besides the conventional propagation characteristics through plasma slab, which overcomes the drawback of other analytical meth- ods introduced in former studies. The EM problem model considered in this work is a steady-state, two-dimensional, nonuniform magne- tized plasma slab with arbitrary magnetic declination angle, which is composed of a number of subslabs. Each subslab has a flxed electron density, and the overall density proflle across the whole slab follows any practical distribution function. Based on PMM, a signiflcant feature of strong transformation of EM wave polarization is addressed when an incident wave normally projects on the slab, which leads to the re- ∞ected or transmitted waves containing two kinds of waves, i.e., the co-polarized wave and the cross-polarized wave. The efiects of vary- ing the plasma parameters on the re∞ected and transmitted powers of co-polarization and cross-polarization, as well as the absorptive power" @default.
• W2105843450 created "2016-06-24" @default.
• W2105843450 creator A5026662660 @default.
• W2105843450 creator A5033572457 @default.
• W2105843450 creator A5051230002 @default.
• W2105843450 creator A5077105583 @default.
• W2105843450 creator A5077386126 @default.
• W2105843450 date "2013-01-01" @default.
• W2105843450 modified "2023-09-27" @default.
• W2105843450 title "ANALYSIS OF PROPAGATION AND POLARIZATION CHARACTERISTICS OF ELECTROMAGNETIC WAVES THROUGH NONUNIFORM MAGNETIZED PLASMA SLAB USING PROPAGATOR MATRIX METHOD" @default.
• W2105843450 cites W140147737 @default.
• W2105843450 cites W1516825310 @default.
• W2105843450 cites W1520664314 @default.
• W2105843450 cites W1990170716 @default.
• W2105843450 cites W2011984638 @default.
• W2105843450 cites W2022129068 @default.
• W2105843450 cites W2028029868 @default.
• W2105843450 cites W2069272529 @default.
• W2105843450 cites W2085208993 @default.
• W2105843450 cites W2091487149 @default.
• W2105843450 cites W2095113283 @default.
• W2105843450 cites W2101623985 @default.
• W2105843450 cites W2105433369 @default.
• W2105843450 cites W2105657162 @default.
• W2105843450 cites W2106941635 @default.
• W2105843450 cites W2125042694 @default.
• W2105843450 cites W2128342191 @default.
• W2105843450 cites W2147699872 @default.
• W2105843450 cites W2150153543 @default.
• W2105843450 cites W2154146748 @default.
• W2105843450 cites W2162104269 @default.
• W2105843450 cites W2168943240 @default.
• W2105843450 cites W2169632038 @default.
• W2105843450 cites W2170977171 @default.
• W2105843450 cites W2491718650 @default.
• W2105843450 doi "https://doi.org/10.2528/pier13010410" @default.
• W2105843450 hasPublicationYear "2013" @default.
• W2105843450 type Work @default.
• W2105843450 sameAs 2105843450 @default.
• W2105843450 citedByCount "15" @default.
• W2105843450 countsByYear W21058434502014 @default.
• W2105843450 countsByYear W21058434502015 @default.
• W2105843450 countsByYear W21058434502016 @default.
• W2105843450 countsByYear W21058434502017 @default.
• W2105843450 countsByYear W21058434502018 @default.
• W2105843450 countsByYear W21058434502020 @default.
• W2105843450 countsByYear W21058434502021 @default.
• W2105843450 crossrefType "journal-article" @default.
• W2105843450 hasAuthorship W2105843450A5026662660 @default.
• W2105843450 hasAuthorship W2105843450A5033572457 @default.
• W2105843450 hasAuthorship W2105843450A5051230002 @default.
• W2105843450 hasAuthorship W2105843450A5077105583 @default.
• W2105843450 hasAuthorship W2105843450A5077386126 @default.
• W2105843450 hasBestOaLocation W21058434501 @default.
• W2105843450 hasConcept C104416048 @default.
• W2105843450 hasConcept C106487976 @default.
• W2105843450 hasConcept C113740112 @default.
• W2105843450 hasConcept C120665830 @default.
• W2105843450 hasConcept C121332964 @default.
• W2105843450 hasConcept C147789679 @default.
• W2105843450 hasConcept C149773537 @default.
• W2105843450 hasConcept C159985019 @default.
• W2105843450 hasConcept C185592680 @default.
• W2105843450 hasConcept C192562407 @default.
• W2105843450 hasConcept C205049153 @default.
• W2105843450 hasConcept C30475298 @default.
• W2105843450 hasConcept C3079626 @default.
• W2105843450 hasConcept C44886760 @default.
• W2105843450 hasConcept C62520636 @default.
• W2105843450 hasConcept C8058405 @default.
• W2105843450 hasConcept C82706917 @default.
• W2105843450 hasConceptScore W2105843450C104416048 @default.
• W2105843450 hasConceptScore W2105843450C106487976 @default.
• W2105843450 hasConceptScore W2105843450C113740112 @default.
• W2105843450 hasConceptScore W2105843450C120665830 @default.
• W2105843450 hasConceptScore W2105843450C121332964 @default.
• W2105843450 hasConceptScore W2105843450C147789679 @default.
• W2105843450 hasConceptScore W2105843450C149773537 @default.
• W2105843450 hasConceptScore W2105843450C159985019 @default.
• W2105843450 hasConceptScore W2105843450C185592680 @default.
• W2105843450 hasConceptScore W2105843450C192562407 @default.
• W2105843450 hasConceptScore W2105843450C205049153 @default.
• W2105843450 hasConceptScore W2105843450C30475298 @default.
• W2105843450 hasConceptScore W2105843450C3079626 @default.
• W2105843450 hasConceptScore W2105843450C44886760 @default.
• W2105843450 hasConceptScore W2105843450C62520636 @default.
• W2105843450 hasConceptScore W2105843450C8058405 @default.
• W2105843450 hasConceptScore W2105843450C82706917 @default.
• W2105843450 hasLocation W21058434501 @default.
• W2105843450 hasOpenAccess W2105843450 @default.
• W2105843450 hasPrimaryLocation W21058434501 @default.
• W2105843450 hasRelatedWork W1968098798 @default.
• W2105843450 hasRelatedWork W2039236113 @default.
• W2105843450 hasRelatedWork W2049583716 @default.
• W2105843450 hasRelatedWork W2086940455 @default.
• W2105843450 hasRelatedWork W2088975965 @default.
• W2105843450 hasRelatedWork W2528221115 @default.
• W2105843450 hasRelatedWork W2807974355 @default.

• next