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As Dalespan said, it is irrelevant whether a particle has mass or not to fall in a gravitational field according to GR.
To see this clearly consider the equivalence principle. Imagine a photon and a massive particle moving from left to right in flat space. They move in a straight line. Now imagine they are inside a rocket that is accelerating upwards. The photon and massive particle still move in a straight line relative to the flat space but to an accelerating observer inside the rocket the photon and massive particle follow a trajectory that from his point of view curves towards the floor. The photon does not require mass to move in a straight line and it does require mass to appear to curve towards the floor of the accelerating rocket. The same is true in a gravitational field by the equivalence principle. No passive gravitational mass is required. Put another way, particles (with or without mass) follow trajectories called geodesics that are determined by their velocities. The geodesics of particles in Schwarzschild geometry assume the particles have no mass. If the particles have significant active gravitational mass (i.e. they are themselves a source of gravity) then the geometry is no longer described by the exterior Schwarzschild metric because that assumes a vacuum and the presence of mass outside the central gravitational spherical mass (described by the interior Schwarzschild solution) changes the geometry.
It is also known that objects dropped from the same height simultaneously reach the floor simultaneously regardless of their individual masses and in GR this idea extends to objects with zero mass. So if we take an extreme example of dropping a stationary moon sized mass and a 1kg mass to a non rotating Earth sized planet with no atmosphere, they will land at the same time. Now if we drop the moon by itself and carefully time how long it takes to fall we will see that the Moon falls in less time than the 1kg object dropped by itself. This is because the planet is accelerating towards the mass of the Moon faster than the planet falls towards the 1 Kg mass. The active gravitational mass is important in this case and this is an example of a particle with significant mass changing the geometry. The large moon falling is not described by the Schwarzschild metric because it significantly changes the geometry.
In short, objects do not require mass to fall in GR and the Schwarzschild metric assumes falling test particles have no mass so it no mystery why a photon falls whether it has mass or not.
[EDIT] Also, as Dalespam mentioned, it can be seen from the Newtonian equation for gravitational acceleration GM/R^2 there is no variable for the mass of the falling object so a body with no mass can be accelerated downward even in Newtonian gravity.
The variable for the mass of the falling body (m) only appears in the Newtonian equation for the force of gravity GMm/R^2 but in GR no force is considered to be acting on a falling body. The Newtonian equation for gravitational acceleration GM/R^2 assumes a test particle with zero mass. There is a more complicated Newtonian formula for when the falling body has significant mass because you have to allow for the acceleration of the attracting massive body towards the falling body and we get back to radially falling moon sized objects. So even in Newtonian physics, passive gravitational mass is not required for a body to fall. Passive gravitational mass (m) that appears in the gravitational force equation GMm/R^2 does however play a part in GR because when an object is not free falling it does experience a gravitational force that we measure as weight.
So Newtonian physics predicts that the gravitational force acting on a particle with zero rest mass is zero yet it also predicts that the particle will be accelerated downwards. That is in good agreement with GR. No passive gravitational mass or gravitational force is required for a particle to be accelerated downwards in GR or Newtonian physics!
To see this clearly consider the equivalence principle. Imagine a photon and a massive particle moving from left to right in flat space. They move in a straight line. Now imagine they are inside a rocket that is accelerating upwards. The photon and massive particle still move in a straight line relative to the flat space but to an accelerating observer inside the rocket the photon and massive particle follow a trajectory that from his point of view curves towards the floor. The photon does not require mass to move in a straight line and it does require mass to appear to curve towards the floor of the accelerating rocket. The same is true in a gravitational field by the equivalence principle. No passive gravitational mass is required. Put another way, particles (with or without mass) follow trajectories called geodesics that are determined by their velocities. The geodesics of particles in Schwarzschild geometry assume the particles have no mass. If the particles have significant active gravitational mass (i.e. they are themselves a source of gravity) then the geometry is no longer described by the exterior Schwarzschild metric because that assumes a vacuum and the presence of mass outside the central gravitational spherical mass (described by the interior Schwarzschild solution) changes the geometry.
It is also known that objects dropped from the same height simultaneously reach the floor simultaneously regardless of their individual masses and in GR this idea extends to objects with zero mass. So if we take an extreme example of dropping a stationary moon sized mass and a 1kg mass to a non rotating Earth sized planet with no atmosphere, they will land at the same time. Now if we drop the moon by itself and carefully time how long it takes to fall we will see that the Moon falls in less time than the 1kg object dropped by itself. This is because the planet is accelerating towards the mass of the Moon faster than the planet falls towards the 1 Kg mass. The active gravitational mass is important in this case and this is an example of a particle with significant mass changing the geometry. The large moon falling is not described by the Schwarzschild metric because it significantly changes the geometry.
In short, objects do not require mass to fall in GR and the Schwarzschild metric assumes falling test particles have no mass so it no mystery why a photon falls whether it has mass or not.
[EDIT] Also, as Dalespam mentioned, it can be seen from the Newtonian equation for gravitational acceleration GM/R^2 there is no variable for the mass of the falling object so a body with no mass can be accelerated downward even in Newtonian gravity.
The variable for the mass of the falling body (m) only appears in the Newtonian equation for the force of gravity GMm/R^2 but in GR no force is considered to be acting on a falling body. The Newtonian equation for gravitational acceleration GM/R^2 assumes a test particle with zero mass. There is a more complicated Newtonian formula for when the falling body has significant mass because you have to allow for the acceleration of the attracting massive body towards the falling body and we get back to radially falling moon sized objects. So even in Newtonian physics, passive gravitational mass is not required for a body to fall. Passive gravitational mass (m) that appears in the gravitational force equation GMm/R^2 does however play a part in GR because when an object is not free falling it does experience a gravitational force that we measure as weight.
So Newtonian physics predicts that the gravitational force acting on a particle with zero rest mass is zero yet it also predicts that the particle will be accelerated downwards. That is in good agreement with GR. No passive gravitational mass or gravitational force is required for a particle to be accelerated downwards in GR or Newtonian physics!
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