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Volumn 138, Issue 7, 2013, Pages

Imaging single electron spin in a molecule trapped within a nanocavity of tunable dimension

Author keywords

[No Author keywords available]

Indexed keywords

DIAMAGNETIC STATE; INELASTIC SPIN; KONDO STATE; MAGNETIC CENTERS; MANY BODY; NANO SCALE; NANO-CAVITIES; PARAMAGNETIC STATE; PORPHINE; SCANNING TUNNELING MICROSCOPES; SINGLE ELECTRON SPIN; SINGLE MOLECULE; SPATIAL IMAGING; SPECTROSCOPIC IMAGES; SPIN-FLIP SCATTERING; TUNNELING GAP; UNPAIRED ELECTRONS; ZEEMAN LEVELS;

EID: 84874519484     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.4790704     Document Type: Article
Times cited : (9)

References (24)
  • 1
    • 0002941533 scopus 로고
    • 10.1143/PTP.32.37
    • J. Kondo, Prog. Theor. Phys. 32, 37 (1964). 10.1143/PTP.32.37
    • (1964) Prog. Theor. Phys. , vol.32 , pp. 37
    • Kondo, J.1
  • 9
    • 84858011448 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.108.106803
    • U. Ham and W. Ho, Phys. Rev. Lett. 108, 106803 (2012). 10.1103/PhysRevLett.108.106803
    • (2012) Phys. Rev. Lett. , vol.108 , pp. 106803
    • Ham, U.1    Ho, W.2
  • 11
    • 44349118337 scopus 로고    scopus 로고
    • 10.1021/jp7114548
    • The energy diagram of charging and discharging processes is shown in the following paper: S. W. Wu, N. Ogawa, G. V. Nazin, and W. Ho, J. Phys. Chem. C 112, 5241 (2008). 10.1021/jp7114548
    • (2008) J. Phys. Chem. C , vol.112 , pp. 5241
    • Wu, S.W.1    Ogawa, N.2    Nazin, G.V.3    Ho, W.4
  • 15
    • 4544370376 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.93.236802
    • -1 caused by division of the applied bias between the vacuum and the oxide, where ε is the dielectric constant of the aluminum oxide layer: S. W. Wu, G. V. Nazin, X. Chen, X. H. Qiu, and W. Ho, Phys. Rev. Lett. 93, 236802 (2004). Typically, this factor is ∼0.85. In the case of a magnetic impurity buried in or adsorbed on a metallic substrate, the impurity is strongly coupled to the substrate. The bias voltage is applied only across the vacuum gap. The magnetic impurity and the substrate are at the same potential. Here, the magnetic impurity is between two Fermi levels separated by the applied bias, forming a steady-state (non-equilibrium) transport configuration. 10.1103/PhysRevLett.93.236802
    • (2004) Phys. Rev. Lett. , vol.93 , pp. 236802
    • Wu, S.W.1    Nazin, G.V.2    Chen, X.3    Qiu, X.H.4    Ho, W.5
  • 16
    • 0032511039 scopus 로고    scopus 로고
    • 10.1126/science.280.5370.1732
    • B. C. Stipe, M. A. Rezaei, and W. Ho, Science 280, 1732 (1998). 10.1126/science.280.5370.1732
    • (1998) Science , vol.280 , pp. 1732
    • Stipe, B.C.1    Rezaei, M.A.2    Ho, W.3
  • 21
    • 33744702875 scopus 로고
    • 10.1103/PhysRevB.49.11040
    • N. S. Wingreen and Y. Meir, Phys. Rev. B 49, 11040 (1994). 10.1103/PhysRevB.49.11040
    • (1994) Phys. Rev. B , vol.49 , pp. 11040
    • Wingreen, N.S.1    Meir, Y.2
  • 22
  • 23
    • 0034298454 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.85.2997
    • N. Lorente and M. Persson, Phys. Rev. Lett. 85, 2997 (2000). 10.1103/PhysRevLett.85.2997
    • (2000) Phys. Rev. Lett. , vol.85 , pp. 2997
    • Lorente, N.1    Persson, M.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.