Demystifier said:
I don't think that it is such a big problem. The Wilson method removes the doublers by a rather simple method. Essentially, one adds to the Lagrangian a discretized version of
$$a\partial^{\mu}\bar{\psi} \partial_{\mu}\psi$$
where ##a## is the lattice spacing. Sure, it violates the chiral symmetry, but so what? Lattice violates also the Lorentz, the rotational and the translational symmetry, and yet nobody gets too excited about it.
Now after reading the excellent review
http://de.arxiv.org/abs/0912.2560 I understand it much better. The Lagrangian density mentioned above really takes the form
$$ra\partial^{\mu}\bar{\psi} \partial_{\mu}\psi$$
where ##r## is a free dimensionless parameter. Through the loop corrections, this term generates a change of fermion mass of the order
$$\delta m\sim \frac{r}{a}$$
The problem is that this correction is
big when ##a## is small, if ##r## takes a "natural" value ##r\sim 1##. To get right phenomenology one must take a much smaller value for ##r##, of the order of
$$r\sim ma$$
or less. But where does such a small number come from? This shows that the problem of chiral fermions on the lattice (with the Wilson term) is really a problem of naturality, known also as a hierarchy problem. The Standard Model of elementary particles has naturality/hierarchy problems even in the continuum limit (e.g. the scalar Higgs mass), and we see that lattice regularization by the Wilson term creates one additional problem of this sort.
But is naturality really a problem? The principle of naturality is really a philosophical problem, based on a vague notion of theoretical "beauty". Some physicists and philosophers argue that it is not really a problem at all
https://www.amazon.com/dp/0465094252/?tag=pfamazon01-20
https://link.springer.com/article/10.1007/s10701-019-00249-zSo if one accepts the philosophy that parameters in the Lagrangian which are not of the order of unity are not a problem, then there is really no problem of chiral fermions on the lattice with the Wilson term.
@atyy I would appreciate your comments.