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3
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5544277233
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A. Hammiche, D. J. Hourston, H. M. Pollock, M. Reading, and M. Song, J. Vac. Sci. Technol. B 14, 1486 (1996).
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J. Vac. Sci. Technol. B
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Hammiche, A.1
Hourston, D.J.2
Pollock, H.M.3
Reading, M.4
Song, M.5
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4
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0028493250
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O. Probst, S. Grafstrom, J. Fritz, S. Dey, J. Kowalski, R. Neumann, M. Wortge, and G. zu Putlitz, Appl. Phys. A: Solids Surf. 59, 109 (1994).
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(1994)
Appl. Phys. A: Solids Surf.
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Probst, O.1
Grafstrom, S.2
Fritz, J.3
Dey, S.4
Kowalski, J.5
Neumann, R.6
Wortge, M.7
Zu Putlitz, G.8
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6
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0032534434
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J. Bolte, F. Niebisch, J. Pelzl, P. Stelmaszyk, and A. D. Wieck, J. Appl. Phys. 84, 6917 (1998).
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Bolte, J.1
Niebisch, F.2
Pelzl, J.3
Stelmaszyk, P.4
Wieck, A.D.5
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10
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0013288566
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note
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Transmission of the light through the (hollow) tip, of refractive index ∼2, was found not to significantly change the diameter of the (approximately Gaussian) optical spot at the sample relative to that above the tip. We use subpicosecond optical pulses with 82 MHz repetition rate, but we checked this had no influence on the sub-10 MHz dynamics here.
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11
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0013288665
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note
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TM Microscopes, Sharp Uncoated Microlever E. It is V shaped, of thickness 0.6 μm, length 140 μm, width of a V branch 18 μm, and is inclined to the sample at 15°.
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12
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0000132115
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K. Inagaki, O. V. Kolosov, G. A. D. Briggs, and O. B. Wright, Appl. Phys. Lett. 76, 1836 (2000).
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(2000)
Appl. Phys. Lett.
, vol.76
, pp. 1836
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Inagaki, K.1
Kolosov, O.V.2
Briggs, G.A.D.3
Wright, O.B.4
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14
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0037091454
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O. B. Wright, R. Li Voti, O. Matsuda, M. C. Larciprete, C. Sibilia, and M. Bertolotti, J. Appl. Phys. 91, 5002 (2002).
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(2002)
J. Appl. Phys.
, vol.91
, pp. 5002
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Wright, O.B.1
Li Voti, R.2
Matsuda, O.3
Larciprete, M.C.4
Sibilia, C.5
Bertolotti, M.6
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16
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0013228081
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(unpublished). Δy is also proportional to a term involving stiffness and damping parameters
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O. B. Wright and M. Tomoda (unpublished). Δy is also proportional to a term involving stiffness and damping parameters.
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Wright, O.B.1
Tomoda, M.2
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17
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0013232327
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The local stress penetration is a few times a, the tip-sample contact radius (where a ∼ 1 nm)
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The local stress penetration is a few times a, the tip-sample contact radius (where a ∼ 1 nm).
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19
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0013278424
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note
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Based on the calculated 3D temperature field only. In the Cr and Al films used, κ may be less than the bulk values assumed.
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20
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0000615748
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B. Li, J. P. Roger, L. Pottier, and D. Fourier, J. Appl. Phys. 86, 5314 (1999).
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(1999)
J. Appl. Phys.
, vol.86
, pp. 5314
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Li, B.1
Roger, J.P.2
Pottier, L.3
Fourier, D.4
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21
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0013317823
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note
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1 equal to μαΔT ∼ 3 pm, assuming periodic temperature variations equal to that of the sample (ΔT ∼ 5 K). However, the smaller OHFM signal observed for the one-layer region of the sample, where ΔT is larger, suggests that tip expansion is not dominant.
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