In your circuit the op-amp output is connected to the same node where you are trying to produce a fixed reference potential. So this is a fight between the op-amp and the R1/R2 potential divider to apply some potential there.
The op-amp wins. Sure, it has to supply a lot of current to overcome the influence of R1 and R2, but it does win, and it gets to decide \$V_{REF}\$, irrespective of what R1 and R2 have to say about it.
With that in mind, you can see that removing R1 and R2 from the picture altogether will not change the op-amp's behaviour in any way, so you have this:

simulate this circuit – Schematic created using CircuitLab
That is just a voltage follower, so:
$$ V_{OUT} = V_{IN} $$
If it's still not clear why we can ignore R1 and R2, let me redraw your circuit in a way that will may make you face-palm. This circuit is exactly the same as yours:

simulate this circuit
As you said, you just want to "lift" the input potential by 0.3V. You want -300mV in to correspond to 0V out, and +300mV in to result in +600mV out.
One thing is clear; when the input goes up, so does the output, and this immediately places a constraint on the design. The input must drive the non-inverting input of the op-amp, because we do not want inverting behaviour.
Another thing is obvious, that gain is 1. A swing of 1V at the input results in a swing of 1V at the output. In other words, all we want is an offset, with no amplification or attenuation.
So, with those design constraints in mind, there a couple of designs I can think of. The first requires a negative voltage source, which you may not have. Still, it's worth exploring. This is a classic differential amplifier:

simulate this circuit
All resistances are equal, so gain is 1. While I won't derive the relationship here, between inputs OFS, IN and output OUT, it is:
$$ V_{OUT} = 1 \times (V_{IN} - V_{OFS}) $$
That's clearly what you want.
There are caveats to this design. As I said this needs a low impedance source of −300mV, which might not be readily available, but crucially it also requires the op-amp to have a negative supply rail, since inputs can actually go negative.
If you have only supplies of 0V and +5V, for instance, that's a big problem. My next approach tries to solve this issue. I want to use a standard non-inverting amplifier configuration, but I will take care to arrange things such that neither of the op-amp's inputs ever have negative potential.
The first step is to use a potential divider to shift the signal upwards so that it never goes negative. Actually, I have to shift it so that it never dips below 30mV or so, because op-amps that claim they operate down to the negative rail (0V in our case) are lying, and can actually only produce outputs almost down to the negative supply. So I aim to shift up the potential of the signal to have a minimum slightly above ground.
You may notice that a potential divider will always attenuate the signal amplitude, but nothing says that we can't then re-amplify it, to the full 600mV swing.
Here's the divider, followed by a non-inverting amplifier to bump up the amplitude again:

simulate this circuit
First thing to notice is my choice of op-amp. The LM358 works down to its negative supply, 0V, almost.
Secondly, notice that one end of the divider is connected to the positive supply of +5V, instead of ground. This is what causes the positive offset. The formula for the potential at A is (where \$V_{CC}=+5V\$):
$$ V_A = V_{IN} + (V_{CC} - V_{IN})\frac{R_1}{R_1+R_2} $$
I won't do it here, but I found \$R_2\$ by solving this equation with \$R_1=10k\Omega\$, \$V_{CC}=+5V\$, \$V_A=30mV\$ and \$V_{IN}=-300mV\$.
Like any potential divider, this one attenuates amplitude by a factor \$G_1\$:
$$ G_1 = \frac{R_2}{R_1+R_2} = 0.938 $$
I want to reverse this attenuation, so the gain of my amplifier \$G_2\$ should be:
$$ G_2 = \frac{1}{G_1} = \frac{R_1+R_2}{R_2} = \frac{160}{150} = 1.07 $$
Now I choose R3 and R4 that satisfy the classic non-inverting amplifier gain equation:
$$ G_2 = 1+\frac{R_3}{R_4} = 1.07 $$
The circuit has a response like this, input on the X axis, output on Y:

One more thing: since your divider is between +5V and IN, any noise on that +5V supply will be injected straight into your amplifier, and become part of its output. If the +5V supply is noisy (and it's likely to be), then you may have produce a more quiet and stable positive voltage source, that you can connect your divider to. There are a couple of easy ways to go about this:

simulate this circuit
Both will produce a clean and steady +3.6V, free of most of the noise present on the +5V supply.
The zener diode solution, left, won't be exactly 3.6V, but it will be stable. You will need to measure the exact value, to use in the equations from before.
The TL431 is a cheap, amazing device, and will regulate much better. It will be as precise as the resistances R3 and R4 that you use. Seriously, get yourself a few TL431s, they are so useful and versatile.
Obviously, since your divider will be connected to this new +3.6V source, instead of +5V, you'll need to calculate appropriate resistor values for the divider and op-amp feedback accordingly.
my previous attempts have not resulted in ...
is not useful ... please update your post withmy previous attempts resulted in ...
... also, please add your circuit \$\endgroup\$