Matches in SemOpenAlex for { <https://semopenalex.org/work/W4307639710> ?p ?o ?g. }
- W4307639710 abstract "A periodic arrangement of 2D conducting planes is known to host a (bulk) plasmon dispersion that interpolates between the typical, gapped behavior of 3D metals and a gapless, acoustic regime as a function of the out-of-plane wavevector. The semi-infinite system -- the configuration relevant to Electron Energy Loss Spectroscopy (EELS) in a reflection geometry, as in High Resolution EELS (HREELS) -- is known to host a surface plasmon that ceases to propagate below a cutoff wavevector. As the f-sum rule requires a finite response whether or not there exist sharp excitations, we demonstrate that what remains in the surface loss function -- the material response probed by HREELS -- is the contribution from the (bulk) plasmon of the infinite system. In particular, we provide a one-to-one mapping between the plasmon continuum and the spectral weight in the surface loss function. In light of this result, we suggest that HREELS be considered a long wavelength probe of the plasmon continuum in layered materials." @default.
- W4307639710 created "2022-11-04" @default.
- W4307639710 creator A5039385849 @default.
- W4307639710 creator A5051149690 @default.
- W4307639710 creator A5053615432 @default.
- W4307639710 date "2022-10-27" @default.
- W4307639710 modified "2023-10-16" @default.
- W4307639710 title "Probing the bulk plasmon continuum of layered materials through electron energy loss spectroscopy in a reflection geometry" @default.
- W4307639710 cites W1621975979 @default.
- W4307639710 cites W1970019684 @default.
- W4307639710 cites W1971291162 @default.
- W4307639710 cites W1972725328 @default.
- W4307639710 cites W1974960717 @default.
- W4307639710 cites W1976922685 @default.
- W4307639710 cites W1983365824 @default.
- W4307639710 cites W1985093669 @default.
- W4307639710 cites W1989978488 @default.
- W4307639710 cites W1993717238 @default.
- W4307639710 cites W1997213691 @default.
- W4307639710 cites W1999526716 @default.
- W4307639710 cites W2001293637 @default.
- W4307639710 cites W2001670518 @default.
- W4307639710 cites W2004450703 @default.
- W4307639710 cites W2004985552 @default.
- W4307639710 cites W2007629090 @default.
- W4307639710 cites W2009987446 @default.
- W4307639710 cites W2011850650 @default.
- W4307639710 cites W2014548983 @default.
- W4307639710 cites W2026961595 @default.
- W4307639710 cites W2034652820 @default.
- W4307639710 cites W2035555786 @default.
- W4307639710 cites W2038599517 @default.
- W4307639710 cites W2041380529 @default.
- W4307639710 cites W2043081913 @default.
- W4307639710 cites W2044012636 @default.
- W4307639710 cites W2050755420 @default.
- W4307639710 cites W2051820067 @default.
- W4307639710 cites W2062281221 @default.
- W4307639710 cites W2067087973 @default.
- W4307639710 cites W2080468017 @default.
- W4307639710 cites W2082174447 @default.
- W4307639710 cites W2088987835 @default.
- W4307639710 cites W2090433833 @default.
- W4307639710 cites W2141983195 @default.
- W4307639710 cites W2153692118 @default.
- W4307639710 cites W2163415022 @default.
- W4307639710 cites W2183748822 @default.
- W4307639710 cites W2801055049 @default.
- W4307639710 cites W2898901924 @default.
- W4307639710 cites W3037060946 @default.
- W4307639710 cites W3101824406 @default.
- W4307639710 cites W3103444186 @default.
- W4307639710 cites W3103484638 @default.
- W4307639710 cites W3111619366 @default.
- W4307639710 cites W4220666434 @default.
- W4307639710 cites W4231032259 @default.
- W4307639710 cites W4280529108 @default.
- W4307639710 cites W4295727637 @default.
- W4307639710 cites W605439828 @default.
- W4307639710 doi "https://doi.org/10.1103/physrevb.106.155152" @default.
- W4307639710 hasPublicationYear "2022" @default.
- W4307639710 type Work @default.
- W4307639710 citedByCount "2" @default.
- W4307639710 countsByYear W43076397102023 @default.
- W4307639710 crossrefType "journal-article" @default.
- W4307639710 hasAuthorship W4307639710A5039385849 @default.
- W4307639710 hasAuthorship W4307639710A5051149690 @default.
- W4307639710 hasAuthorship W4307639710A5053615432 @default.
- W4307639710 hasBestOaLocation W43076397102 @default.
- W4307639710 hasConcept C10165471 @default.
- W4307639710 hasConcept C109496249 @default.
- W4307639710 hasConcept C110879396 @default.
- W4307639710 hasConcept C120665830 @default.
- W4307639710 hasConcept C121332964 @default.
- W4307639710 hasConcept C136676167 @default.
- W4307639710 hasConcept C146088050 @default.
- W4307639710 hasConcept C150835508 @default.
- W4307639710 hasConcept C178187954 @default.
- W4307639710 hasConcept C192562407 @default.
- W4307639710 hasConcept C199360897 @default.
- W4307639710 hasConcept C26873012 @default.
- W4307639710 hasConcept C32891209 @default.
- W4307639710 hasConcept C41008148 @default.
- W4307639710 hasConcept C41999313 @default.
- W4307639710 hasConcept C62520636 @default.
- W4307639710 hasConcept C6260449 @default.
- W4307639710 hasConcept C65682993 @default.
- W4307639710 hasConceptScore W4307639710C10165471 @default.
- W4307639710 hasConceptScore W4307639710C109496249 @default.
- W4307639710 hasConceptScore W4307639710C110879396 @default.
- W4307639710 hasConceptScore W4307639710C120665830 @default.
- W4307639710 hasConceptScore W4307639710C121332964 @default.
- W4307639710 hasConceptScore W4307639710C136676167 @default.
- W4307639710 hasConceptScore W4307639710C146088050 @default.
- W4307639710 hasConceptScore W4307639710C150835508 @default.
- W4307639710 hasConceptScore W4307639710C178187954 @default.
- W4307639710 hasConceptScore W4307639710C192562407 @default.
- W4307639710 hasConceptScore W4307639710C199360897 @default.
- W4307639710 hasConceptScore W4307639710C26873012 @default.
- W4307639710 hasConceptScore W4307639710C32891209 @default.