Voltage output from a tank circuit
The transfer function is

$$\frac{V_{out}}{V_{in}} = \frac{j\omega \frac{L}{R}}{(1 - \omega^2LC) + j\omega \frac{L}{R} }$$

The Q is given by

$$Q = R\sqrt{\frac{C}{L}}$$

So the Q is proportional to the series resistance \$R\$ and, for your values, is quite high

$$Q = 1k \sqrt{\frac{244.8p}{41.3n}} \approx 77$$

With this high \$Q\$, the transfer function magnitude rapidly changes near the resonance frequency so simulation round off may greatly affect the results.  

I tried \$R=100 \Omega\$ which reduced the \$Q\$ by a factor of 10 and the simulation output is very nearly the input after a number of cycles.



Update:

I adjusted the "step ceiling" parameter for the transient simulation down to \$10^{-12}\$ and I get a good simulation with \$R=1k\Omega\$.