FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2897630366> ?p ?o ?g. }

• W2897630366 endingPage "015010" @default.
• W2897630366 startingPage "015010" @default.
• W2897630366 abstract "Monolayers and multilayers of semiconducting transition metal dichalcogenides (TMDCs) offer an ideal platform to explore valley-selective physics with promising applications in valleytronics and information processing. Here we manipulate the energetic degeneracy of the $mathrm{K}^+$ and $mathrm{K}^-$ valleys in few-layer TMDCs. We perform high-field magneto-reflectance spectroscopy on WSe$_2$, MoSe$_2$, and MoTe$_2$ crystals of thickness from monolayer to the bulk limit under magnetic fields up to 30 T applied perpendicular to the sample plane. Because of a strong spin-layer locking, the ground state A excitons exhibit a monolayer-like valley Zeeman splitting with a negative $g$-factor, whose magnitude increases monotonically when thinning the crystal down from bulk to a monolayer. Using the $mathbf{kcdot p}$ calculation, we demonstrate that the observed evolution of $g$-factors for different materials is well accounted for by hybridization of electronic states in the $mathrm{K}^+$ and $mathrm{K}^-$ valleys. The mixing of the valence and conduction band states induced by the interlayer interaction decreases the $g$-factor magnitude with an increasing layer number. The effect is the largest for MoTe$_2$, followed by MoSe$_2$, and smallest for WSe$_2$. Keywords: MoSe$_2$, WSe$_2$, MoTe$_2$, valley Zeeman splitting, transition metal dichalcogenides, excitons, magneto optics." @default.
• W2897630366 created "2018-10-26" @default.
• W2897630366 creator A5014417794 @default.
• W2897630366 creator A5025997810 @default.
• W2897630366 creator A5035269354 @default.
• W2897630366 creator A5046414560 @default.
• W2897630366 creator A5048721757 @default.
• W2897630366 creator A5070787716 @default.
• W2897630366 creator A5080558004 @default.
• W2897630366 creator A5081879320 @default.
• W2897630366 creator A5089123534 @default.
• W2897630366 creator A5090552656 @default.
• W2897630366 date "2018-11-02" @default.
• W2897630366 modified "2023-10-12" @default.
• W2897630366 title "Zeeman spectroscopy of excitons and hybridization of electronic states in few-layer WSe ₂ , MoSe ₂ and MoTe ₂" @default.
• W2897630366 cites W1742662164 @default.
• W2897630366 cites W1850053210 @default.
• W2897630366 cites W1975346569 @default.
• W2897630366 cites W1980451122 @default.
• W2897630366 cites W1983229868 @default.
• W2897630366 cites W2007209834 @default.
• W2897630366 cites W2024927857 @default.
• W2897630366 cites W2044480396 @default.
• W2897630366 cites W2047098795 @default.
• W2897630366 cites W2052256037 @default.
• W2897630366 cites W2056166808 @default.
• W2897630366 cites W2063576642 @default.
• W2897630366 cites W2071376185 @default.
• W2897630366 cites W2071538265 @default.
• W2897630366 cites W2094953717 @default.
• W2897630366 cites W2114318022 @default.
• W2897630366 cites W2130244744 @default.
• W2897630366 cites W2155116009 @default.
• W2897630366 cites W2163620792 @default.
• W2897630366 cites W2331292532 @default.
• W2897630366 cites W2346451233 @default.
• W2897630366 cites W2511538070 @default.
• W2897630366 cites W2539582486 @default.
• W2897630366 cites W2554601732 @default.
• W2897630366 cites W2572983492 @default.
• W2897630366 cites W2579961345 @default.
• W2897630366 cites W2584731490 @default.
• W2897630366 cites W2600335003 @default.
• W2897630366 cites W2730550917 @default.
• W2897630366 cites W2754919420 @default.
• W2897630366 cites W2798085316 @default.
• W2897630366 cites W2800692100 @default.
• W2897630366 cites W2885283935 @default.
• W2897630366 cites W3100638670 @default.
• W2897630366 cites W3104413967 @default.
• W2897630366 cites W3123414937 @default.
• W2897630366 doi "https://doi.org/10.1088/2053-1583/aae7e5" @default.
• W2897630366 hasPublicationYear "2018" @default.
• W2897630366 type Work @default.
• W2897630366 sameAs 2897630366 @default.
• W2897630366 citedByCount "19" @default.
• W2897630366 countsByYear W28976303662019 @default.
• W2897630366 countsByYear W28976303662020 @default.
• W2897630366 countsByYear W28976303662021 @default.
• W2897630366 countsByYear W28976303662022 @default.
• W2897630366 countsByYear W28976303662023 @default.
• W2897630366 crossrefType "journal-article" @default.
• W2897630366 hasAuthorship W2897630366A5014417794 @default.
• W2897630366 hasAuthorship W2897630366A5025997810 @default.
• W2897630366 hasAuthorship W2897630366A5035269354 @default.
• W2897630366 hasAuthorship W2897630366A5046414560 @default.
• W2897630366 hasAuthorship W2897630366A5048721757 @default.
• W2897630366 hasAuthorship W2897630366A5070787716 @default.
• W2897630366 hasAuthorship W2897630366A5080558004 @default.
• W2897630366 hasAuthorship W2897630366A5081879320 @default.
• W2897630366 hasAuthorship W2897630366A5089123534 @default.
• W2897630366 hasAuthorship W2897630366A5090552656 @default.
• W2897630366 hasBestOaLocation W28976303662 @default.
• W2897630366 hasConcept C115260700 @default.
• W2897630366 hasConcept C121332964 @default.
• W2897630366 hasConcept C171250308 @default.
• W2897630366 hasConcept C17729963 @default.
• W2897630366 hasConcept C192562407 @default.
• W2897630366 hasConcept C25227350 @default.
• W2897630366 hasConcept C26873012 @default.
• W2897630366 hasConcept C32891209 @default.
• W2897630366 hasConcept C62520636 @default.
• W2897630366 hasConcept C7070889 @default.
• W2897630366 hasConceptScore W2897630366C115260700 @default.
• W2897630366 hasConceptScore W2897630366C121332964 @default.
• W2897630366 hasConceptScore W2897630366C171250308 @default.
• W2897630366 hasConceptScore W2897630366C17729963 @default.
• W2897630366 hasConceptScore W2897630366C192562407 @default.
• W2897630366 hasConceptScore W2897630366C25227350 @default.
• W2897630366 hasConceptScore W2897630366C26873012 @default.
• W2897630366 hasConceptScore W2897630366C32891209 @default.
• W2897630366 hasConceptScore W2897630366C62520636 @default.
• W2897630366 hasConceptScore W2897630366C7070889 @default.
• W2897630366 hasFunder F4320308269 @default.
• W2897630366 hasFunder F4320320300 @default.
• W2897630366 hasFunder F4320320879 @default.
• W2897630366 hasIssue "1" @default.
• W2897630366 hasLocation W28976303661 @default.

• next