Nugatory said:
Torque is indeed defined in terms of force, but we can have torque even when there is no net force. An example might be spinning a wheel on a shaft by placing my hands on opposite sides of the wheel and pushing with one hand, pulling with other. The center of mass of the wheel stays put so we know that there's no net force on the wheel, but it starts to spin telling us that there is a net torque on the wheel.
Even when there is only one force there's still torque (in general - we can always choose a point about which to calculate the torque in such a way that it comes out zero). If there is only one force involved then the net force is necessarily non-zero and the center of mass will accelerate along with any rotation caused by the torque
Yes, a pure torque resulting in pure angular acceleration with no net translation of the CoM of the body to which the forces are applied is always generated by a balance of (at least two) forces, sum total in anyone axis being zero.
Some very complicated answers here that I think miss the question about the door, because it is not a pure angular acceleration. I think the point you were asking is whether the vector sum of forces from a) the door handle, and b) the hinge, are zero?
Answer; not exactly but close. (answer to you title is 'both')
There are two forces on the door when you push/pull the handle; 1) that force, and 2) the force from the hinge. The magnitude and vector direction of the two forces are not quite precisely equal while the vector direction is not quite opposite.
The reason is that the door not
only receives a torque sending it into a spin but also receives a translating acceleration as its CoM begins to accelerate. The force on the handle is always very slightly greater than the force on the hinge if the door has angular acceleration greater than the torque-friction is inducing at the hinge.
Take the case of a slammed door; at the instant the door slams shut, there is a force from the retaining edge of the door which is equal and opposite to the forces from the hinge that result in torque. However, the door also has translational inertia too, perpendicular to the aperture, and there has to be an EXTRA impulse from the door edge and hinge which are both in the same direction to decelerate the translational motion.
This then adds summatively to one force negatively and one force being positively (in some datum direction) giving two forces. When a door slams, the force is greater on the closing edge than the hinge, the delta between the two being the force which decelerates the door motion in the direction perpendicular to the opening.
If you watch a door with a loose hinge being slammed, you may notice the hinge jumps 'outwards' momentarily, this being the reversal of the force vector from one direction when being pushed closed then at the moment of the 'slam' through zero and then the force other direction.
A revolving door is quite different as there is no translational momentum. The forces on the central pivot of a revolving door are always equal and opposite at all times as its CoM never moves, unlike a domestic door.