Matches in SemOpenAlex for { <https://semopenalex.org/work/W2011476422> ?p ?o ?g. }
- W2011476422 abstract "The spin order of the nickel oxide (001) surface is resolved, employing noncontact atomic force microscopy at 4.4 K using bulk Fe and SmCo tips mounted on a qPlus sensor that oscillates at sub-50 pm amplitudes. The spin-dependent signal is hardly detectable with Fe tips. In contrast, SmCo tips yield a height contrast of 1.35 pm for Ni ions with opposite spins. SmCo tips even show a small height contrast on the O atoms of 0.5 pm within the $2ifmmodetimeselsetexttimesfi{}1$ spin unit cell, pointing to the observation of superexchange. We attribute the increased signal-to-noise ratio to the increased magnetocrystalline anisotropy energy of SmCo, which stabilizes the magnetic moment at the apex. Atomic force spectroscopy on the $mathrm{Ni}ensuremath{uparrow}$, $mathrm{Ni}ensuremath{downarrow}$, and O lattice site reveals a magnitude of the exchange energy of merely 1 meV at the closest accessible distance with an exponential decay length of ${ensuremath{lambda}}_{mathrm{exc}}=18text{ }text{ }mathrm{pm}$." @default.
- W2011476422 created "2016-06-24" @default.
- W2011476422 creator A5022279814 @default.
- W2011476422 creator A5040144752 @default.
- W2011476422 date "2013-06-24" @default.
- W2011476422 modified "2023-10-17" @default.
- W2011476422 title "Spin Resolution and Evidence for Superexchange on NiO(001) Observed by Force Microscopy" @default.
- W2011476422 cites W1963766014 @default.
- W2011476422 cites W1963924260 @default.
- W2011476422 cites W1964805269 @default.
- W2011476422 cites W1965424173 @default.
- W2011476422 cites W1967445304 @default.
- W2011476422 cites W1968248628 @default.
- W2011476422 cites W1971057239 @default.
- W2011476422 cites W1973996986 @default.
- W2011476422 cites W1980745639 @default.
- W2011476422 cites W1985169272 @default.
- W2011476422 cites W1986055204 @default.
- W2011476422 cites W1986191169 @default.
- W2011476422 cites W1987128427 @default.
- W2011476422 cites W1987832809 @default.
- W2011476422 cites W1991940160 @default.
- W2011476422 cites W1997262856 @default.
- W2011476422 cites W2005095018 @default.
- W2011476422 cites W2006247054 @default.
- W2011476422 cites W2035613081 @default.
- W2011476422 cites W2047205370 @default.
- W2011476422 cites W2048865587 @default.
- W2011476422 cites W2051001465 @default.
- W2011476422 cites W2056253937 @default.
- W2011476422 cites W2061713670 @default.
- W2011476422 cites W2064605029 @default.
- W2011476422 cites W2064811347 @default.
- W2011476422 cites W2072959343 @default.
- W2011476422 cites W2076111440 @default.
- W2011476422 cites W2084547658 @default.
- W2011476422 cites W2089428077 @default.
- W2011476422 cites W2091383175 @default.
- W2011476422 cites W2091438580 @default.
- W2011476422 cites W2107289599 @default.
- W2011476422 cites W2111395596 @default.
- W2011476422 cites W2264187979 @default.
- W2011476422 cites W3150248096 @default.
- W2011476422 cites W4230748214 @default.
- W2011476422 doi "https://doi.org/10.1103/physrevlett.110.266101" @default.
- W2011476422 hasPubMedId "https://pubmed.ncbi.nlm.nih.gov/23848902" @default.
- W2011476422 hasPublicationYear "2013" @default.
- W2011476422 type Work @default.
- W2011476422 sameAs 2011476422 @default.
- W2011476422 citedByCount "47" @default.
- W2011476422 countsByYear W20114764222013 @default.
- W2011476422 countsByYear W20114764222014 @default.
- W2011476422 countsByYear W20114764222015 @default.
- W2011476422 countsByYear W20114764222016 @default.
- W2011476422 countsByYear W20114764222017 @default.
- W2011476422 countsByYear W20114764222018 @default.
- W2011476422 countsByYear W20114764222019 @default.
- W2011476422 countsByYear W20114764222020 @default.
- W2011476422 countsByYear W20114764222021 @default.
- W2011476422 countsByYear W20114764222022 @default.
- W2011476422 countsByYear W20114764222023 @default.
- W2011476422 crossrefType "journal-article" @default.
- W2011476422 hasAuthorship W2011476422A5022279814 @default.
- W2011476422 hasAuthorship W2011476422A5040144752 @default.
- W2011476422 hasBestOaLocation W20114764222 @default.
- W2011476422 hasConcept C115260700 @default.
- W2011476422 hasConcept C120665830 @default.
- W2011476422 hasConcept C121332964 @default.
- W2011476422 hasConcept C14179194 @default.
- W2011476422 hasConcept C155355069 @default.
- W2011476422 hasConcept C161790260 @default.
- W2011476422 hasConcept C184779094 @default.
- W2011476422 hasConcept C185592680 @default.
- W2011476422 hasConcept C186370098 @default.
- W2011476422 hasConcept C192562407 @default.
- W2011476422 hasConcept C26873012 @default.
- W2011476422 hasConcept C2778113609 @default.
- W2011476422 hasConcept C2778870898 @default.
- W2011476422 hasConcept C2780320949 @default.
- W2011476422 hasConcept C32546565 @default.
- W2011476422 hasConcept C32938098 @default.
- W2011476422 hasConcept C42704618 @default.
- W2011476422 hasConcept C46141821 @default.
- W2011476422 hasConcept C55493867 @default.
- W2011476422 hasConcept C56803174 @default.
- W2011476422 hasConcept C62520636 @default.
- W2011476422 hasConcept C74575197 @default.
- W2011476422 hasConcept C8010536 @default.
- W2011476422 hasConcept C85725439 @default.
- W2011476422 hasConcept C97355855 @default.
- W2011476422 hasConceptScore W2011476422C115260700 @default.
- W2011476422 hasConceptScore W2011476422C120665830 @default.
- W2011476422 hasConceptScore W2011476422C121332964 @default.
- W2011476422 hasConceptScore W2011476422C14179194 @default.
- W2011476422 hasConceptScore W2011476422C155355069 @default.
- W2011476422 hasConceptScore W2011476422C161790260 @default.
- W2011476422 hasConceptScore W2011476422C184779094 @default.
- W2011476422 hasConceptScore W2011476422C185592680 @default.
- W2011476422 hasConceptScore W2011476422C186370098 @default.
- W2011476422 hasConceptScore W2011476422C192562407 @default.