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Volumn 87, Issue 8, 2013, Pages

Calibrating atomic-scale force sensors installed at the tip apex of a scanning tunneling microscope

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EID: 84874524695     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.87.081408     Document Type: Article
Times cited : (22)

References (17)
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    • Advances in atomic force microscopy
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    • Giessibl, F.J.1
  • 6
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    • Recipes for cantilever parameter determination in dynamic force spectroscopy: Spring constant and amplitude
    • DOI 10.1088/0957-4484/18/25/255503, PII S095744840746799X
    • G. H. Simon, M. Heyde, and H.-P. Rust, Nanotechnology NNOTER 0957-4484 10.1088/0957-4484/18/25/255503 18, 255503 (2007). (Pubitemid 46996219)
    • (2007) Nanotechnology , vol.18 , Issue.25 , pp. 255503
    • Simon, G.H.1    Heyde, M.2    Rust, H.-P.3
  • 7
    • 85081781014 scopus 로고    scopus 로고
    • The absolute distance between the tip and the surface is not known from the experiment. Instead, we use a relative tip-surface distance scale z. The value of z is defined as the distance by which the tip is approached from its stabilization point towards the surface prior to the respective constant height scan. Although the tip was always stabilized at the same lateral location, the actual tip-surface distance is expected to vary between the different tips. Therefore, the absolute values of the z scales in Figs. , and are not directly comparable.
    • The absolute distance between the tip and the surface is not known from the experiment. Instead, we use a relative tip-surface distance scale z. The value of z is defined as the distance by which the tip is approached from its stabilization point towards the surface prior to the respective constant height scan. Although the tip was always stabilized at the same lateral location, the actual tip-surface distance is expected to vary between the different tips. Therefore, the absolute values of the z scales in Figs., and are not directly comparable.
  • 8
    • 85081781299 scopus 로고    scopus 로고
    • 0 was taken to be equal to 1800 N/m (Ref.).
    • 0 was taken to be equal to 1800 N / m (Ref.).
  • 9
    • 39749147651 scopus 로고    scopus 로고
    • The force needed to move an atom on a surface
    • DOI 10.1126/science.1150288
    • M. Ternes, C. P. Lutz, C. F. Hirjibehedin, F. J. Giessibl, and A. J. Heinrich, Science SCIEAS 0036-8075 10.1126/science.1150288 319, 1066 (2008). (Pubitemid 351300783)
    • (2008) Science , vol.319 , Issue.5866 , pp. 1066-1069
    • Ternes, M.1    Lutz, C.P.2    Hirjibehedin, C.F.3    Giessibl, F.J.4    Heinrich, A.J.5
  • 13
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    • Note that the contrast inversion in the Δf channel occurs at smaller z if compared to F(z). This is to be expected since F(z) â̂∫Δf(z)dz (Ref.).
    • Note that the contrast inversion in the Δ f channel occurs at smaller z if compared to F (z). This is to be expected since F (z) â̂ ∫ Δ f (z) d z (Ref.).
  • 14
    • 85081776638 scopus 로고    scopus 로고
    • As the appearing attractive force shows, the tip-surface interaction cannot be described with a simple two-particle Lennard-Jones type potential. This behavior is not surprising, since the considered junction has more degrees of freedom (e.g., the translational degrees of freedom of the particle adsorbed at the apex), changes of which will influence the interactions in the junction.
    • As the appearing attractive force shows, the tip-surface interaction cannot be described with a simple two-particle Lennard-Jones type potential. This behavior is not surprising, since the considered junction has more degrees of freedom (e.g., the translational degrees of freedom of the particle adsorbed at the apex), changes of which will influence the interactions in the junction.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.