For a low-pass filter configuration, the output of the above circuit should be measured across the capacitor C1.
Let's denote the input as Vi(s), the output as Vo(s), the resistance as R and capacitive impedance as 1/sC.
Then,
Vo(s)/Vi(s) = (1/sC) / (R + 1/sC)
or, Vo(s)/Vi(s) = 1/(1 + sRC)
or, Vo(w)/Vi(w) = 1/(1 + jwRC)
This is the transfer function of a low-pass filter whose mgnitude is maximum at w = 0, [Vo(0)/Vi(0) = 1/(1 + 0) = 1]
Thus the 3dB corner frequency will be the frequence at which
Vo(w0)/Vi(w0) = 1/sqrt(2)
or, AMP[1/(1 + jw0RC)] = 1/sqrt(2)
or, 1/sqrt(1+w02R2C2) = 1/sqrt(2)
or, 1+w02R2C2 = 2
or, w02 = 1/(R2C2)
or, w0 = 1/(RC)
or, f0 = 1/(2.pi.RC)
The phase can be calculated as follows-
ARG[Vo(w)/Vi(w)] = ARG[1/(1 + jwRC)]
= ARG[(1 - jwRC) / (1 + w2R2C2)]
= arctan(-wRC/1) = -arctan(wRC)
At, w = w0, phase = -arctan(w0RC) = -arctan((1/RC) . RC) = -arctan(1) = -45 degrees
To answer your last question, the corner frequencies are called HALF-POWER POINTS, because the output power at that frequency is half the input power. But output voltage may not be half of input voltage!