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Volumn 80, Issue 15, 2009, Pages

Quantum size effects in competing charge and spin orderings of dangling bond wires on Si(001)

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EID: 72449142217     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.155329     Document Type: Article
Times cited : (26)

References (21)
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    • J.-H. Choi and J.-H. Cho, Phys. Rev. Lett. 102, 166102 (2009). 10.1103/PhysRevLett.102.166102
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    • Choi, J.-H.1    Cho, J.-H.2
  • 12
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    • Spin-polarized DFT calculations of 10.1016/S0039-6028(03)00399-6
    • Spin-polarized DFT calculations of C. F. Bird and D. R. Bowler, Surf. Sci. 531, L351 (2003) predicted the NM and AF ground states for even- and odd-numbered DBs, respectively. In order to explain the disparity between STM measurements and simulations for even-numbered DB wires, Bird and Bowler speculated the flipping motion of buckled dimers to produce time-averaging STM images 10.1016/S0039-6028(03)00399-6
    • (2003) Surf. Sci. , vol.531 , pp. 351
    • Bird, C.F.1    Bowler, D.R.2
  • 13
    • 3342985512 scopus 로고
    • However, noting that thermally activated flipping motion of buckled dimers becomes frozen at ∼100K [e.g., 10.1103/PhysRevLett.68.2636
    • However, noting that thermally activated flipping motion of buckled dimers becomes frozen at ∼100K [e.g., A. Wolkow, Phys. Rev. Lett. 68, 2636 (1992)], it is most likely that the observed bright protrusion of each DB in even-number DB wires can be associated with their static geometries of the AF configuration rather than the flipping motion of buckled dimers of the NM configuration. 10.1103/PhysRevLett.68.2636
    • (1992) Phys. Rev. Lett. , vol.68 , pp. 2636
    • Wolkow, A.1
  • 14
    • 72449127046 scopus 로고    scopus 로고
    • Using the 2×10 unit-cell calculations with the plane-wave-basis cutoff of 30 Ry, we found that the energy difference between the NM and AF configurations and the heights of dangling bonds (in Table) change by a few meV/DB and less than a hundredth of angstroms, respectively.
    • Using the 2×10 unit-cell calculations with the plane-wave-basis cutoff of 30 Ry, we found that the energy difference between the NM and AF configurations and the heights of dangling bonds (in Table) change by a few meV/DB and less than a hundredth of angstroms, respectively.
  • 15
    • 72449184497 scopus 로고    scopus 로고
    • The exchange coupling constant J for the DB- n wire can be evaluated by J= EFM-AF / (n-1), where EFM-AF is the energy difference per unit cell between the FM and AF configurations. For DB- , n=2.
    • The exchange coupling constant J for the DB- n wire can be evaluated by J= EFM-AF / (n-1), where EFM-AF is the energy difference per unit cell between the FM and AF configurations. For DB-, n=2.
  • 16
    • 72449178903 scopus 로고    scopus 로고
    • We found that the formation energy of NMsym, defined as the energy cost of desorbing H atoms from the H-terminated Si(001) surface, is 3.426, 3.433, 3.414, 3.411, 3.404, 3.400, and 3.380 eV per dangling bond for DB-2, DB-3, DB-4, DB-5, Db-6, DB-7, and DB- , respectively.
    • We found that the formation energy of NMsym, defined as the energy cost of desorbing H atoms from the H-terminated Si(001) surface, is 3.426, 3.433, 3.414, 3.411, 3.404, 3.400, and 3.380 eV per dangling bond for DB-2, DB-3, DB-4, DB-5, Db-6, DB-7, and DB-, respectively.
  • 17
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    • The buckling patterns of DUD, DUDUD, and DUDUDUD in DB-3, DB-5, and DB-7 are less stable than UDU, UDUDU, and UDUDUDU by 9, 5, 3 meV/DB, respectively.
    • The buckling patterns of DUD, DUDUD, and DUDUDUD in DB-3, DB-5, and DB-7 are less stable than UDU, UDUDU, and UDUDUDU by 9, 5, 3 meV/DB, respectively.
  • 18
  • 19
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.