The asymmetric responses of the system between the external force of right and left directions are called "nonreciprocal". There are many examples of nonreciprocal responses such as the rectification by p-n junction. However, the quantum mechanical wave does not distinguish between the right and left directions as long as the time-reversal symmetry is intact, and it is a highly nontrivial issue how the nonreciprocal nature originates in quantum systems. Here we demonstrate by the quantum ratchet model, i.e., a quantum particle in an asymmetric periodic potential, that the dissipation characterized by a dimensionless coupling constant α plays an essential role for nonlinear nonreciprocal response. The temperature (T ) dependence of the second order nonlinear mobility µ2 is found to be µ2 ∼ T 6/α−4 for α < 1, and µ2 ∼ T 2(α−1) for α > 1, respectively, where αc = 1 is the critical point of the localization-delocalization transition, i.e., Schmid transition. On the other hand, µ2 shows the behavior µ2 ∼ T −11/4 in the high temperature limit. Therefore, µ2 shows the nonmonotonous temperature dependence corresponding to the classical-quantum crossover. The generic scaling form of the velocity v as a function of the external field F and temperature T is also discussed. These findings are relevant to the heavy atoms in metals, resistive superconductors with vortices and Josephson junction system, and will pave a way to control the nonreciprocal responses.