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It should be noted that the method to monitor the fiber–tip interaction with the sample using an optical lever with external laser light reflected from a micromirror glued to the bent tip (in a manner similar to usual AFM with soft levers) has been realized but is not broadly accepted; see, for example, APPLAB
-
It should be noted that the method to monitor the fiber–tip interaction with the sample using an optical lever with external laser light reflected from a micromirror glued to the bent tip (in a manner similar to usual AFM with soft levers) has been realized but is not broadly accepted; see, for example, C. E. Talley, G. A. Cooksey, and R. Dunn, Appl. Phys. Lett. APPLAB 69, 3809 (1996).
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G. T. Shubeita, S. K. Sekatskii, M. Chergui, G. Dietler, and V. S. Letokhov, Appl. Phys. Lett. APPLAB 74, 3453 (1999).
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18
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33748132312
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For a review, see, for example, SOPUAP
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For a review, see, for example, G. N. Flerov and V. S. Barashenkov, Sov. Phys. Usp. SOPUAP 17, 783 (1975).
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Seoul, Korea, 18–23 July 1999 (unpublished).
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S. K. Sekatskii, G. T. Shubeita, and G. Dietler, poster presented at the 10th International STM Conference, Seoul, Korea, 18–23 July 1999 (unpublished).
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poster presented at the 10th International STM Conference
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Shubeita, G.T.2
Dietler, G.3
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20
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0038349696
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Apparent elongation of the holes, similar to the diagonal elongation in Fig. 5, was observed in some series of measurements (cf. Ref. 17). This can be explained by a combination of different reasons, including the peculiarities of nuclear filters preparation procedure (Ref. 16) and interaction of polarized light with the nanoholes in metal films [cf., APPLAB,]; some effect of the piezoscanner drift also cannot be fully excluded.
-
Apparent elongation of the holes, similar to the diagonal elongation in Fig. 5, was observed in some series of measurements (cf. Ref. 17). This can be explained by a combination of different reasons, including the peculiarities of nuclear filters preparation procedure (Ref. 16) and interaction of polarized light with the nanoholes in metal films [cf. C. Sönnichsen, A. C. Duch, G. Steininger, M. Koch, G. von Plessen, and J. Feldmann, Appl. Phys. Lett. APPLAB 76, 140 (2000)]; some effect of the piezoscanner drift also cannot be fully excluded.
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Sönnichsen, C.1
Duch, A.C.2
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Feldmann, J.6
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22
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ULTRD6
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A. G. T. Ruiter, K. O. van der Werf, J. A. Veerman, M. F. Garcia-Parajo, W. H. F. Rensen, and N. F. van Hulst, Ultramicroscopy ULTRD6 71, 149 (1998).
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van Hulst, N.F.6
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23
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A more complicated model, which is given, for example, in, JMICAR, also gives the similar results.
-
A more complicated model, which is given, for example, in A. Naber, J. Microsc. JMICAR 194, 307 (1999), also gives the similar results.
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Naber, A.1
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24
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0003985181
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Any textbook with an introduction to oscillatory motion, for example, 3rd ed. (Harcourt Brace Jovanovich, Orlando, FL)
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Any textbook with an introduction to oscillatory motion, for example, J. B. Marion and S.T. Thornton, Classical Dynamics of Particles and Systems, 3rd ed. (Harcourt Brace Jovanovich, Orlando, FL, 1988).
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Marion, J.B.1
Thornton, S.T.2
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5544251185
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In particular, this implies that the optimal AFM scheme depends on the sample properties, see, for example, JVTBD9, the same is valid for SNOM, and we are going to investigate the problem soon.
-
In particular, this implies that the optimal AFM scheme depends on the sample properties, see, for example, N. A. Burnham, G. Gremaud, A. J. Kulik, P.-J. Gallo, and F. Oulevey, J. Vac. Sci. Technol. B JVTBD9 14, 1308 (1996), the same is valid for SNOM, and we are going to investigate the problem soon.
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Burnham, N.A.1
Gremaud, G.2
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Oulevey, F.5
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D. A. Lapshin, V. N. Reshetov, S. K. Sekatskii, and V. S. Letokhov, JETP Lett. JTPLA2 67, 263 (1998)
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D. A. Lapshin, V. N. Reshetov, S. K. Sekatskii, and V. S. Letokhov, Ultramicroscopy ULTRD6 76, 13 (1999).
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Lapshin, D.A.1
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