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23
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85038293241
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Otherwise it is very difficult to define the tip electrostatically: how does one attach charges to the tip apex in a controlled way
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Otherwise it is very difficult to define the tip electrostatically: how does one attach charges to the tip apex in a controlled way?
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26
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85038321892
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In addition, we assume no charges between tip and sample. If charges are present, see the discussion in Ref
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In addition, we assume no charges between tip and sample. If charges are present, see the discussion in Ref. 25.
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27
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85038345644
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For very large distances, the field from the tip is similar to that produced by a point charge in front of a conducting wall. One then finds by the “image method” that (formula presented) is proportional to (formula presented)
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For very large distances, the field from the tip is similar to that produced by a point charge in front of a conducting wall. One then finds by the “image method” that (formula presented) is proportional to (formula presented).
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28
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0001402033
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33
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85038310107
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For the discussion presented here to be valid it is important that the field lines stand perpendicular to the sample so that the approximation used is valid
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For the discussion presented here to be valid it is important that the field lines stand perpendicular to the sample so that the approximation used is valid.
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34
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85038300129
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A global mean voltage under the cantilever is defined through (formula presented)
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A global mean voltage under the cantilever is defined through (formula presented).
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36
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85038307180
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To be more precise, the effective force constant (formula presented) of the system should not vary significantly over the range of cantilever oscillation. This implies that (formula presented) where, is the oscillation amplitude, (formula presented) the second derivative of the force at the mean equilibrium position (formula presented), and (formula presented) the force constant of the cantilever
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To be more precise, the effective force constant (formula presented) of the system should not vary significantly over the range of cantilever oscillation. This implies that (formula presented) where a is the oscillation amplitude, (formula presented) the second derivative of the force at the mean equilibrium position (formula presented), and (formula presented) the force constant of the cantilever.
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37
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85038316415
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We note that, in analogy to the electrostatic force between tip and sample, also the signal corresponding to the frequency shift will have three components: a dc component as well as a component varying with (formula presented) (more precisely: (formula presented) and another one varying with (formula presented) (more precisely: (formula presented). The idea is to adjust (formula presented) so that (formula presented)
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We note that, in analogy to the electrostatic force between tip and sample, also the signal corresponding to the frequency shift will have three components: a dc component as well as a component varying with (formula presented) (more precisely: (formula presented) and another one varying with (formula presented) (more precisely: (formula presented). The idea is to adjust (formula presented) so that (formula presented).
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38
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85038265922
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The exact solution of a (full) sphere over a conduction surface is (formula presented), where the capacitance (formula presented) is determined through an an infinite sum: (formula presented) and (formula presented). See also W.R. Smythe, (McGraw-Hill, New York, 1939), p. 131
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The exact solution of a (full) sphere over a conduction surface is (formula presented), where the capacitance (formula presented) is determined through an an infinite sum: (formula presented) and (formula presented). See also W.R. Smythe, Static and Dynamic Electricity (McGraw-Hill, New York, 1939), p. 131.
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