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88, 051112, 2006. ,. Charvolin T, de Fornel F. and Hadji. E. , vol. 98, p. 086109, 2005. , “Experimental demonstration of Bloch mode parity change in photonic crystal waveguide”, App. Phys. , vol. 85, no. 14, p. 2682, 2004. Courjon D. , Le champ proche optique: théorie et applications, Springer, 2001. , Salt M. , “Measuring optical phase singularities at subwavelength resolution”, J. Opt. A, vol. 6, p. 189, 2004. , Evanescent Waves, Springer, 2001. , Dumas P. ” Appl. , vol. 35, p. 5583–5594, 1996.
A near-field actuated optical nanocavity”, Opt. , vol. 16, p. 279, 2008a. , Peyrade, D. Rodier J. , Lalanne P. Hadji E. , “Nano-manipulation of confined electromagnetic fields with a near-field probe”, CR Physique, vol. 9, p. 24-30, 2008b. , “Nearfield spectroscopy of low loss waveguide integrated microcavities”, Appl. Phys. , vol. 88, 051112, 2006. ,. Charvolin T, de Fornel F. and Hadji. E. , vol. 98, p. 086109, 2005. , “Experimental demonstration of Bloch mode parity change in photonic crystal waveguide”, App.
For the constant distance mode, the probe scans at a fixed distance from the surface. 4. 1. Description of the experimental set-up The most commonly used method is the constant distance mode. To ensure a constant distance between the probe and the surface, we use either an atomic force microscope (AFM), or a scanning tunneling microscope, for samples and metal probes. Another way of controlling the position of the probe is to use shear force control, which uses shearing forces between the surface and the probe, when it is animated by a periodic movement which is parallel to the surface of the sample.
