R1 and R2 may be considered "pull-down" resistors, but that's a poor description of their purpose. They are converting the current that flows around the loop consisting of the transformer winding and these resistances into a potential difference; two potential differences to be exact.
It's a simple application of Ohm's law, and the term "pull-down" is a misleading description. Sure, when winding current is zero, the voltages across R1 and R2 are also zero, but a better description would be that at all times, the voltages across R1 and R2 are proportional to winding current, by Ohm's law.
The center point of those potential differences is forced to adopt the sensing circuit's own ground potential, 0V, by literally connecting it to ground. The two potentials "seen" by the differential amplifier are then guaranteed to lie within that amplifier's own acceptable range of input potentials, instead of "floating" at some "random" potential relative to the circuit's ground. This also has the benefit of bringing the common mode potential to zero, which would help mitigate error caused by any non-zero common-mode rejection in the amplifier.
You could certainly use a single current sense resistance, and amplify the voltage across it using a single-ended amplifier, but there are a couple of advantages to splitting the sense voltage in two and using a differential amplifier to subtract one from the other.
The first advantage is that in this subtraction operation is an inherent noise cancellation. Any noise present common to both signals will disappear as a result of the subtraction. This will be particularly important if the current transformer is physically located far from the amplifier.
A second advantage might be that the output from a differential amplifier will naturally be ground-referenced, regardless of any common-mode offset present in the pair of potentials.