  We construct a model which exhibits resistivity going as a power law in
temperature $T$, as $T^\alpha$ down to the lowest temperature. There is no
residual resistivity because we assume the absence of disorder and momentum
relaxation is due to umklapp scattering. Our model consists of a quantum spin
liquid state with spinon Fermi surface and a hole Fermi surface made out of
doped holes. The key ingredient is a set of singular $2k_F$ modes living on a
ring in momentum space. Depending on parameters, $\alpha$ may be unity (strange
metal) or even smaller. The model may be applicable to a doped organic
compound, which has been found to exhibit linear T resistivity. We conclude
that it is possible to obtain strange metal behavior starting with a model
which is not so strange.
