-
2
-
-
0000345877
-
-
10.1103/PhysRevLett.82.4034
-
T. Hitosugi, S. Heike, T. Onogi, T. Hashizume, S. Watanabe, Z.-Q. Li, K. Ohno, Y. Kawazoe, T. Hasegawa, and K. Kitazawa, Phys. Rev. Lett. 82, 4034 (1999). 10.1103/PhysRevLett.82.4034
-
(1999)
Phys. Rev. Lett.
, vol.82
, pp. 4034
-
-
Hitosugi, T.1
Heike, S.2
Onogi, T.3
Hashizume, T.4
Watanabe, S.5
Li, Z.-Q.6
Ohno, K.7
Kawazoe, Y.8
Hasegawa, T.9
Kitazawa, K.10
-
3
-
-
0001221256
-
-
10.1103/PhysRevB.54.R17308
-
S. Watanabe, Y. A. Ono, T. Hashizume, and Y. Wada, Phys. Rev. B 54, R17308 (1996). 10.1103/PhysRevB.54.R17308
-
(1996)
Phys. Rev. B
, vol.54
, pp. 17308
-
-
Watanabe, S.1
Ono, Y.A.2
Hashizume, T.3
Wada, Y.4
-
4
-
-
36449004659
-
-
10.1063/1.111722
-
J. W. Lyding, T.-C. Shen, J. S. Hubacek, J. R. Tucker, and G. C. Abeln, Appl. Phys. Lett. 64, 2010 (1994). 10.1063/1.111722
-
(1994)
Appl. Phys. Lett.
, vol.64
, pp. 2010
-
-
Lyding, J.W.1
Shen, T.-C.2
Hubacek, J.S.3
Tucker, J.R.4
Abeln, G.C.5
-
10
-
-
34547397460
-
-
10.1103/PhysRevLett.98.246101;
-
J.-H. Choi and J.-H. Cho, Phys. Rev. Lett. 98, 246101 (2007) 10.1103/PhysRevLett.98.246101
-
(2007)
Phys. Rev. Lett.
, vol.98
, pp. 246101
-
-
Choi, J.-H.1
Cho, J.-H.2
-
11
-
-
65549119171
-
-
10.1103/PhysRevLett.102.166102
-
J.-H. Choi and J.-H. Cho, Phys. Rev. Lett. 102, 166102 (2009). 10.1103/PhysRevLett.102.166102
-
(2009)
Phys. Rev. Lett.
, vol.102
, pp. 166102
-
-
Choi, J.-H.1
Cho, J.-H.2
-
12
-
-
0038219579
-
-
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
-
-
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
-
-
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
-
-
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
-
-
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
-
-
72449157043
-
-
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.
-
-
-
-
21
-
-
60349092987
-
-
10.1103/PhysRevLett.102.046805
-
M. B. Haider, J. L. Pitters, G. A. DiLabio, L. Livadaru, J. Y. Mutus, and R. A. Wolkow, Phys. Rev. Lett. 102, 046805 (2009). 10.1103/PhysRevLett.102. 046805
-
(2009)
Phys. Rev. Lett.
, vol.102
, pp. 046805
-
-
Haider, M.B.1
Pitters, J.L.2
Dilabio, G.A.3
Livadaru, L.4
Mutus, J.Y.5
Wolkow, R.A.6
|