We develop simple mathematical models that lead to order-of-magnitude predi
ctions of the sizes of the electronic, nuclear, and electrostrictive contri
butions to the nonlinear optical susceptibility. We find that all three of
these processes make comparable contributions to the third-order susceptibi
lity, even though the optical-frequency linear susceptibility is dominated
by the electronic response. We also find that when the mathematical express
ions describing these contributions to the third-order susceptibility are w
ritten in terms of fundamental physical constants, they are identical to wi
thin numerical factors of the order of unity and are given in Gaussian unit
s by chi((3)) = (h) over bar(8)/8m(4)e(10) = 4.25 x 10(-16) cm(2) s(-1) V-2
.