Well, notice that the impedance of your circuit is given by:
$$\left|\space\underline{\text{Z}}_{\space\text{i}}\right|\left(\omega\right)=\frac{\displaystyle1}{\displaystyle\sqrt{\left(\frac{\displaystyle1}{\displaystyle\text{R}}\right)^2+\left(\omega\text{C}-\frac{\displaystyle1}{\displaystyle\omega\text{L}}\right)^2}}\tag1$$
Now, we can see that \$\$ is at a maximum when:
$$\omega\text{C}-\frac{\displaystyle1}{\displaystyle\omega\text{L}}=0\space\Longrightarrow\space\omega:=\hat{\omega}=\frac{1}{\sqrt{\text{CL}}}\tag2$$
Which gives:
$$\left|\space\underline{\text{Z}}_{\space\text{i}}\right|\left(\hat{\omega}\right)=\text{R}\tag3$$
So, now we can solve for the cut-off frequencies:
$$\left|\space\underline{\text{Z}}_{\space\text{i}}\right|\left(\omega\right)=\frac{\displaystyle\text{R}}{\displaystyle\sqrt{2}}\space\Longrightarrow\space\omega:=\omega_\pm=\frac{\displaystyle1\pm\sqrt{1+\frac{\displaystyle4\text{CR}^2}{\text{L}}}}{\displaystyle2\text{CR}}\tag4$$
So, for the bandwidth we get:
$$\mathcal{B}:=\left|\omega_+-\omega_-\right|=\frac{\displaystyle1}{\displaystyle\text{CR}}\sqrt{1+\frac{\displaystyle4\text{CR}^2}{\displaystyle\text{L}}}\tag5$$
And for the quality factor we get:
$$\mathcal{Q}:=\frac{\displaystyle\hat{\omega}}{\displaystyle\mathcal{B}}=\frac{\displaystyle\frac{1}{\sqrt{\text{CL}}}}{\displaystyle\frac{\displaystyle1}{\displaystyle\text{CR}}\sqrt{1+\frac{\displaystyle4\text{CR}^2}{\displaystyle\text{L}}}}=\text{R}\cdot\sqrt{\frac{\displaystyle\text{C}}{\displaystyle\text{L}+4\text{CR}^2}}\tag6$$
Using your values, we get:
$$\mathcal{Q}=50\cdot\sqrt{\frac{\displaystyle10^{-9}}{\displaystyle10^{-9}+4\cdot10^{-9}\cdot50^2}}=\frac{\displaystyle50}{\displaystyle\sqrt{10001}}\approx0.499975\tag7$$