You can rewrite your equation as
$$\langle \vec 1 + s\cdot \vec g, \vec t\rangle > 0$$
Where $\vec 1$ is the vector of all 1's, $\vec g\sim\mathcal{N}(0, I_n)$ is standard gaussian, and $\vec t := (\sin(t_1),\dots, \sin(t_n))$ is your vector. I will only use that $\vec t$ is in the positive orthant.
We can simplify this equation to
$$\langle \vec 1, \vec t\rangle + s\langle \vec t, \vec g\rangle > 0$$
As $\vec t$ is in the positive orthant, we have that $\langle \vec 1, \vec t\rangle = \lVert \vec t\rVert_1$.
It is a standard computation that $s\langle \vec t, \vec g\rangle \sim \mathcal{N}(0,s^2\lVert \vec t\rVert_2^2)$.
Therefore (by symmetry), you reduce to showing the 1D gaussian tail-bound $1 > g'$ for $g'\sim\mathcal{N}(0, s^2\frac{\lVert \vec t\rVert_2^2}{\lVert \vec t\rVert_1^2})$. You should be able to do this with standard bounds, depending on what your standard of "high probability" is.