Optical second-harmonic (SH) response of a semiconductor quantum dot (QD) e
xcited by the near field of a tip in a near-field scanning-optical microsco
pe is investigated theoretically. Using an anisotropic effective mass appro
ximation, we analyze the frequency- and space-dependent SH nonlinear curren
t density in the midgap frequency region associated with interband and inte
rsubband transitions in the QD system. Both heavy- and light-hole states co
ntribute to the SH signal of the QD system. Assuming that an external field
drives the tip and the tip field excites the QD, and neglecting local-fiel
d effects, we define an effective SH susceptibility tensor of the QD/tip sy
stem in terms of the incident-external field. The second-harmonic generatio
n is allowed because the rapidly varying tip field excites the selection-ru
le breaking transitions in the QD system. For a given size of the metal-coa
ted tip, we performed numerical calculations of the SH susceptibility by sc
anning the tip and varying the frequency. We show that the SH nonlinearity
of the QD/tip system is strongly dependent on the tip position because the
overlap integral of the QD envelope wave functions and the tip field is var
ied by scanning the tip over the QD. Our results also show that the spatial
distribution of the tip field is reflected in the tip-position dependence
of the SH signal. [S0163-1829(99)07103-9].