I've seen the term been used quite a lot when reading about lattice gauge theory calculations. So far what I've gathered is the following, from this source [1].
Lorentz invariance of the action is broken on a discretized lattice. When calculating any quantity on the lattice, the continuum limit $a\rightarrow 0$ must be extracted, where $a$ is the lattice spacing. However this convergence is often slow, with $O(a)$ error terms, so one way to speed it up is to introduce an $O(a)$ irrelevant operator to the Lagrangian density, and tune its coefficient so that the lattice artifacts disappear in certain physical quantities (masses, cross sections, etc.).
$$\mathcal{L}\rightarrow \mathcal{L}+\int c_{\textrm{sw}}\mathcal{L}_c\, $$
$$\mathcal{L}_c=-\frac{a}{4} \bar \psi \sigma_{\mu\nu}\psi F^{\mu\nu}$$
The tuneable coefficient $c_{\textrm{sw}}$ is called the Sheikholeslami-Wohlert coefficient, and is a function of the lattice spacing through the gauge coupling $g$. The correction term $\mathcal{L}_c$ is called the "clover term".
So this would tell me what the clover-term is, the clover-improved action, but what is a clover fermion?
[1] "Clover fermions in the adjoint representation and simulations of supersymmetric Yang-Mills theory" arXiv:1311.6312 [hep-lat]