A question to gauge fixing in nonabelian gauge theories

Question

In quantum gauge theories it is usual to fix the gauge with the equation $\partial^\mu A_\mu = 0$ where $A_\mu$ is the gauge connection. From this gauge fixing condition the remaining gauge degree of freedom can be determined.

Unfortunaitly, there is appearing a determinant factor (Faddeev-Popov determinant) in the Feynman path integral coming from the change in the Haar measure due to this gauge fixing condition.

It is clear that without gauge fixing one integrates infinitely many (in the Feynman path integral) over the same contribution $e^{iS}$ since $S$ doesn't change under a gauge transformation. Is it possible to insert a gauge fixing factor $\delta(g-g_0)$ where $g$ is the gauge group and $g_0$ is a constant gauge group in the path integral, i.e. is it possible to restrict the gauge group to only a fixed function such that any other possibilities are not respected?

Or more precisely: What gauge fixing condition must be applied on $A_\mu$ to impose that the gauge group is fixed to only a single function over the spacetime?

EDIT (ATTEMPT): I am thinking about the gauge fixing condition $n^\mu A_\mu = 0$ with $n^\mu$ as a 4-vector function; can it satisfy above conditions? May be the gauge transformation given explicitely by $A_\mu \mapsto A_\mu + \Xi_\mu$ then it must also hold $n^\mu \Xi_\mu = 0$ and then if $\Xi^\mu$ is a fixed function, the 4-vector $n^\mu$ is chosen such that above gauge condition is satisfied.

Answer 1

First, terminology: You are not "determining the gauge group", what you are doing in gauge fixing is determining a smooth choice of (hopefully only) one representant of an equivalence class of field configurations called the gauge orbit. Geometrically, you are seeking a section which intersects each gauge orbit exactly once.

The problem of finding a gauge condition that indeed chooses precisely one representant globally is known as the Gribov problem. Since the gauge principal bundle (or, analogously in the constrained Hamiltonian perspective, the constraint surface) may be topologically non-trivial, global sections may not exist. However, locally, one can always choose gauge conditions that single out a unique point on the gauge orbits, and the regions in which such a thing is possible are known as Gribov regions. This rescues the perturbative application of the path integral - just choose a Gribov region around the configuration you are perturbing around, and restrict the path integral to that. Non-perturbatively, this problem is generally unsolved. If you have a Gribov obstruction to imposing global gauge conditions, the path integral is non-perturbatively ill-defined (or rather, counts configurations multiple times in a in generall not-well-controlled manner)-

For a technical discussion of the gauge fixing choices and how the Gribov ambiguity explicitly arises when trying to solve the gauge fixing condition for the gauge-fixed field configuration, see for example "Gribov Problem for Gauge Theories: a Pedagogical Introduction" (arXiv) by Esposito, Pelliccia and Zaccaria.

As a last remark, a consistency requirement on the gauge condition typically requires it to be of "derivative type", i.e. it has to fulfill a certain differential equation and will typically contain derivatives of the gauge field. A condition like $n^\mu A_\mu = 0$ will usually not even locally choose a unique point in a gauge orbit, and may not be consistently preserved under time evolution.