Unless I am missing something, it seems clear to me that since $t\in (t + \mathcal{L})$, then
$$\lambda_1(t + \mathcal{L}) \leq ||t||_2 .$$
However, this is not particularly useful because $t$ could be very large and still generate a translated "lattice" that is not very far from the original.
I am not sure exactly what you are trying to achieve, but here is an approach that might be of some usefulness: First, remember that you can write a basis of your lattice in matrix form with the basis vectors being the columns of the matrix. Let's assume that the dimension of the matrix is $n$.
If you have more than $n$ vectors, you can have an extended matrix and you could find a basis by doing a Hermite decomposition to bring the matrix to Hermite Normal Form.
With that introduction, here is what you can do:
- Append the vector $t$ as a column to a basis of the lattice.
- Do a Hermite Decomposition of the extended matrix
- The basis that you find will describe a different lattice $\mathcal{L}_2$
- My intuition tells me that $\lambda_1(t + \mathcal{L})=\lambda_1(\mathcal{L}_2)$, but you should try to prove this yourself.
This effectively gives you a way to calculate $\lambda_1(t + \mathcal{L})$ through a different object that is a lattice.
Hope this helps.