You are quite correct that interactions between electrons can cause them to jump a potential barrier. For example thermionic emission is a good example of this. However this is a quite separate process from quantum tunneling.
Consider some collection of electrons - we'll use the electrons in the conduction band of a metal as an example. To get an electron out of the metal requires an energy called the work function, and this energy is typically a few electron volts. The thermal energy available to the electrons is $kT$, but at room temperature $kT$ is only about 0.025 eV. That suggests we would require 40 times room temperature or about 12000K to get thermionic emission, but actually we get emission at only a few hundred degrees C.
The reason for this is that $kT$ is the average energy of the electrons and some electrons have energies lower than this while some have energies higher than this. Electrons scatter off each other in a basically random way and as a result some can get very high energies.
The probability that an electron will have an energy $E$ is given by the Boltzmann distibution:
$$ P \propto e-{E/kT} $$
For energies a lot higher than $kT$ the probability is very small, but then there are a lot of electrons in a metal. The result is that even at relatively low temperatures some electrons will escape.
So interactions between electrons can indeed allow a few of them to jump a potential barrier. However this happens because those few electrons have an energy higher than the barrier. Quantum tunneling is a completely different process and allows an electron to jump a barrier even when it doesn't have enough energy to jump the barrier.