-
1
-
-
85038267765
-
-
Within the theory we will present here, the resolution is mainly determined by the size of the electromagnetic cavity formed between the tip and sample. This leads to a resolution limit of the order of 5–10 nm. The 1-nm resolution was obtained in STM light emission experiments by R. Berndt (private communication) that make use of very sharp tips
-
Within the theory we will present here, the resolution is mainly determined by the size of the electromagnetic cavity formed between the tip and sample. This leads to a resolution limit of the order of 5–10 nm. The 1-nm resolution was obtained in STM light emission experiments by R. Berndt (private communication) that make use of very sharp tips.
-
-
-
-
3
-
-
4243849962
-
-
N. Majlis, A. Levy Yeyati, F. Flores, and R. Monreal, Phys. Rev. B52, 12 505 (1995).
-
(1995)
Phys. Rev. B
, vol.52
, pp. 12 505
-
-
Majlis, N.1
Levy Yeyati, A.2
Flores, F.3
Monreal, R.4
-
4
-
-
4243299893
-
-
D T. Pierce, A. Davies, J A. Stroscio, and R J. Celotta, Appl. Phys. A: Mater. Sci. Process.66, S403 (1998).
-
(1998)
Appl. Phys. A: Mater. Sci. Process.
, vol.66
, pp. S403
-
-
Pierce, D.T.1
Davies, A.2
Stroscio, J.A.3
Celotta, R.J.4
-
8
-
-
0032990807
-
-
L. Aigouy, S. Gresillon, A C. Boccara, J C. Rivoal, V. Mathet, C. Chappert, J P. Jamet, and J. Ferre, J. Microsc.194, 295 (1999).
-
(1999)
J. Microsc.
, vol.194
, pp. 295
-
-
Aigouy, L.1
Gresillon, S.2
Boccara, A.C.3
Rivoal, J.C.4
Mathet, V.5
Chappert, C.6
Jamet, J.P.7
Ferre, J.8
-
9
-
-
4143083350
-
-
R. Wiesendanger, H.-J. Güntherodt, G. Güntherodt, R J. Gambino, and R. Ruf, Phys. Rev. Lett.65, 247 (1990).
-
(1990)
Phys. Rev. Lett.
, vol.65
, pp. 247
-
-
Wiesendanger, R.1
J, H.2
Güntherodt, G.3
Gambino, R.J.4
Ruf, R.5
-
10
-
-
0034625659
-
-
S. Heinze, M. Bode, A. Kubetzka, O. Pietzsch, X. Nie, S. Blügel, and R. Wiesendanger, Science288, 1805 (2000).
-
(2000)
Science
, vol.288
, pp. 1805
-
-
Heinze, S.1
Bode, M.2
Kubetzka, A.3
Pietzsch, O.4
Nie, X.5
Blügel, S.6
Wiesendanger, R.7
-
12
-
-
85038289322
-
-
We use a local dielectric function. Nonlocal effects are small, and would not change the results of this calulation in any considerable way. For a more detailed discussion of this, see Sec. IV D of Ref
-
We use a local dielectric function. Nonlocal effects are small, and would not change the results of this calulation in any considerable way. For a more detailed discussion of this, see Sec. IV D of Ref. 15.
-
-
-
-
13
-
-
33744649359
-
-
J. Zak, E R. Moog, C. Liu, and S D. Bader, Phys. Rev. B43, 6423 (1991);
-
(1991)
Phys. Rev. B
, vol.43
, pp. 6423
-
-
Zak, J.1
Moog, E.R.2
Liu, C.3
Bader, S.D.4
-
15
-
-
85038325964
-
-
M. B. Stearns, in, Landolt-Börnstein, New Series, Group III, 19, Pt. a, edited by H.P.J. Wijn (Springer-Verlag, Berlin, 1986), p. 113
-
M. B. Stearns, in Magnetic Properties of Metalds, Landolt-Börnstein, New Series, Group III, Vol. 19, Pt. a, edited by H.P.J. Wijn (Springer-Verlag, Berlin, 1986), p. 113.
-
-
-
-
17
-
-
85038321755
-
-
Note that, strictly speaking, there are contributions in Eqs. (2.38) and (2.39) that are second order in (formula presented). They are, however, negligibly small
-
Note that, strictly speaking, there are contributions in Eqs. (2.38) and (2.39) that are second order in (formula presented). They are, however, negligibly small.
-
-
-
-
18
-
-
85038301420
-
-
The quantity (formula presented) was denoted (formula presented) in Ref
-
The quantity (formula presented) was denoted (formula presented) in Ref. 5.
-
-
-
-
19
-
-
84857756328
-
-
T. Junno, K. Deppert, L. Montelius, and L. Samuelson, Appl. Phys. Lett.66, 3627 (1995).
-
(1995)
Appl. Phys. Lett.
, vol.66
, pp. 3627
-
-
Junno, T.1
Deppert, K.2
Montelius, L.3
Samuelson, L.4
|