In this study we present theoretical predictions concerning the third-order
nonlinear optical properties of semiconductor carbon nanotubes for photon
energies well below the fundamental absorption edge. Both virtual interband
pi-electron transitions and combined intraband-interband ones are assumed
to be the basic microscopic mechanisms of optical nonlinearities in this sp
ectral region. Resting upon simple dimensional considerations and using onl
y model-independent properties of the K-election energy spectrum near the c
onduction and valence-band edges, we obtain theoretical estimations for the
low-frequency third-order susceptibility chi e((3))(0) due to these two me
chanisms, which sheds light on the relationship between the non-resonant no
nlinear optical response of nanotubes and their geometrical and electronic
structure. This result derived in physically interpretable terms is in good
agreement with that obtained in our recent study on the basis of a systema
tic analytical approach. We find that single-shell 'zig-zag' nanotubes disp
lay positive chi e((3))(0) values, which is due to the positive contributio
n from combined pi-electron transitions dominating the negative contributio
n from purely interband transitions. We also find that the increase of the
nanotube radius R results in a strong enhancement (proportional to R-4) of
chi e((3))(0), which can reach values larger by several orders of magnitude
than those reported for the fullerene molecules C-60 and C-70 We draw a co
nclusion that the modification of the geometrical structure of nanotubes pr
ovides an efficient means for the engineering of novel nonlinear-optical ma
terials with high cubic susceptibilities.