  In quasi-one-dimensional conductors, the conductivity in both one-dimensional
axis and interchain direction shows peaks when magnetic field is tilted at the
magic angles in the plane perpendicular to the conducting chain. Although there
are several theoretical studies to explain the magic angle effect, no
satisfactory explanation, especially for the one-dimensional conductivity, has
been obtained. We present a new theory of the magic angle effect in the
one-dimensional conductivity by taking account of the momentum-dependence of
the Fermi velocity, which should be large in the systems close to a spin
density wave instability. The magic angle effect is explained in the
semiclassical equations of motion, but neither the large corrugation of the
Fermi surface due to long-range hoppings nor hot spots, where the relaxation
time is small, on the Fermi surface are required.
