Do clocks run slower in a field of gravity? Does that question even make sense? Let's say that it does, and that the answer is yes. I can only interpret that as saying that a clock in a field of gravity runs slower than it would be running if the field of gravity wasn't there. I don't know how to compare those two situations, and I'm not at all convinced that it makes sense in general. (As I was writing this post, I figured out one way to make sense of it in a specific case. See the stuff at the end).
The relevant comparison is between two clocks held at different but constant altitudes in the same gravitational "field". I don't think "gravitational field" is a well-defined concept in GR, so let's be more specific. I'm talking about e.g. two clocks held at different but constant r coordinates in a Schwarzschild spacetime. In this case, the reason why their ticking rates are different is that they are accelerating by different amounts.
The situation is similar to the case of two clocks attached to opposite ends of the same solid rod in SR. Accelerate the rod gently, and it will get shorter in the original rest frame, because of Lorentz contraction (or maybe I should say "because solids behave in a way that's consistent with the Lorentz contraction formula when they are accelerated gently along a geodesic"). This means that the rear is accelerating faster than the front. What a clock measures is the proper time of the curve in spacetime that represents its motion. In an inertial frame, proper time can be expressed as the integral of \sqrt{dt^2-dx^2} along the curve, and because of the greater acceleration at the rear, there will be a greater contribution from dx along that curve. That makes the proper time smaller, so the clock at the rear ticks slower.
Here's a way to make sense of the phrase "a clock ticks slower in a gravitational field", at least in the specific case of a Schwarzschild spacetime. If we go far away from the spherical mass distribution, a Newtonian description of gravity gets more accurate. In particular, the concept of gravitational field makes more sense at greater distances from the mass. In the limit where the distance goes to infinity, the description in terms of the "gravitational field" becomes exact, and in that limit there's no field at all. So what we're really talking about is the relative ticking rates of two clocks at different altitudes, but one of them is at a finite altitude, and the other is infinitely far away.