Detecting Hall viscosity in the absence of inversion or time reversal symmetries

The Hall viscosity is experimentally observed in graphene. The Hall viscosity is characterized by the induced voltage with its polarity opposite to the Hall voltage. A formula is derived for the induced voltage entering from the Hall viscosity for the prototype models of bilayer graphene in the absence of time reversal symmetry and the semiconductor hetrostructures with strong spin orbit coupling. The fault tolerant Hall viscosity is predicted to be observed in the non-local resistance measurement.