In general, halving of the standard state concentration will not lead to an RT ln 2 term as a(c/2) is not equal to a(c)/2. This only holds for ideal gasses and solutions.
For now, let's focus on ideal solutions please. Let me state my problem more clearly. If we define the standard state concentration as 2
M instead of 1
M, then by
a_i = \gamma_{c,i} c_i/c^{\ominus}\,
we see that the activity is halved, since c^{\ominus}\, has doubled from 1 molar to 2. Now, by
\mu_i = \mu_i^{\ominus} + RT\ln{a_i}
we see that dividing a_i by 2 must result in
\mu_i = \mu_i^{\ominus} + RT\ln{(a_i/2)}
\mu_i = \mu_i^{\ominus} + RT\ln{a_i} - RT\ln{2}
However, I presume that \mu_i and T are independent of the standard state concentration, while \mu_i^{\ominus} takes on a new value. Therefore, to keep \mu_i the same for both sets of equations,
\mu_i = \mu_i^{\ominus} (new) + RT\ln{a_i} - RT\ln{2} = \mu_i^{\ominus} + RT\ln{a_i}
we must have
\mu_i^{\ominus} (new) = \mu_i^{\ominus} + RT\ln{2}
which means doubling c^{\ominus} must have the effect of adding RT ln 2 to \mu_i^{\ominus}. But this is very strange, since T should represent the temperature of the system in consideration, which shouldn't seem to have any bearing on the value of mu at standard state. What's wrong with my reasoning here?