Well, what you have is two resistors in series, which is a potential divider.
In this case one end of the divider is not attached to the "ground", but to some other voltage. You can apply usual potential divider equations, just remember to add your reference voltage (3.0V) to it.
The difference between voltages at ends of the divider is 6V.
Voltage in the middle, referenced to 3V (right end of the divider) is
V_{m(3V)}=6V\frac{2.0\Omega}{6.0\Omega+2.0\Omega}=1.5V
This is referenced to the right end of the divider. If you want it referenced to "ground", i.e. the V_o voltage, just add 3V to it.
You can also reference everything to 9V. Then the divider is powered from -6V, and
V_{m(9V)}=-6V\frac{6.0\Omega}{6.0\Omega+2.0\Omega}=-4.5V
This is referenced to the left end of the divider. To reference it to "ground", add 9V to it.
You will obtain the same answer either way.
The resistive divider "equation" I've used above can be derived from Ohm's and Kirchhof's laws.