Motivated by applications of second-order nonlinear capacitances in semicon
ductor measurements of charge carrier densities, we investigate the profoun
d relationship between the second-order nonlinear emittance and the total a
nd partial local densities of states for tunnelling transport in nanoscale
systems with ac bias. We have derived an explicit formula for the second-or
der nonlinear emittance in the case of low frequencies. The difference betw
een the emittance and capacitance in actual measurements is elaborated; and
we show that the total density of states completely determine the second-o
rder nonlinear emittance. Our study indicates that the second-order nonline
ar emittance equals the second-order nonlinear electrochemical capacitance
when there is no tunnelling current and the density of states is macroscopi
c. Also, in the quantum regime, the second-order emittance does not vanish
even if the pure geometric capacitance equals zero. Based on our results, w
e present an application of the second-order nonlinear emittance in nanosca
le systems.