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By V. Bellitto

ISBN-10: 9535104144

ISBN-13: 9789535104148

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7, No. Scanning Probe Microscopy of Clay Minerals, pp. (91-138) Wicks, F. , Eby, R. , Hawthorne, F. , Henderson, G. S. and Vrdoljak, G. A. (1993). Imaging the Internal Atomic Structure of Layer Silicates Using the Atomic Force Microscope. Can Mineral, Vol. 31, No. 3, pp. (541-550) Wicks, F. , Kjoller, K. and Henderson, G. S. (1992). Imaging the Hydroxyl Surface of Lizardite at Atomic Resolution with the Atomic Force Microscope. Can. , Vol. 30, No. 1, pp. (83-91), 0008-4476 Wyckoff, R. W. G. (1968).

The unknown magnetic moments as well as the effective probe-sample separation are treated as free parameters to be fitted to experimental data. The force acting on the probe, which is immersed in the near-surface sample microfield, is given by (Hartmann, 1999):     F  0 q  m   H   (5) Magnetic Force Microscopy: Basic Principles and Applications 43  where q and m are the effective monopole and dipole moments of the probe. The point-probe approximation yields satisfactory results in many cases of MFM contrast interpretation.

2. Modelled MFM tip having a magnetic coating on a non-magnetic core. Parameters for integration are indicated (Koch, 2005) 42 Atomic Force Microscopy – Imaging, Measuring and Manipulating Surfaces at the Atomic Scale  The magnetostatic potential s  r  created   by any ferromagnetic sample can be calculated from its magnetization vector field Ms r , (Hartmann, 1999):    ,     2,   Ms r ,  1  d s  Ms r 3, s  r    d r     4   r r, r r,         (4)  where s , is an outward normal vector from the sample surface.

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Atomic Force Microscopy - Imaging, Meas., Manip. Surfs. at the Atomic Scale by V. Bellitto

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