As previously mentioned in Section 2.3, a n (t) is a band-limited signal around the Doppler frequency, so the peak of (S_{a}^{nn} left ({t;f} right)) can determine the Doppler frequency and the velocity of the target can henceforth be determined.
Don't add spaces around the apostrophe, like "couldn ' t", "couldn 't" or "couldn' t".
The observations y n, g follow a symmetric distribution centred around ŷ n, g = x n T β g with precision φ n, g τ.
The phase locking can be a general (m: n ) locking, with (5) Ψ m, n (t ) = (m φ i (t ) − n φ j (t ) ) mod (2 π ) constrained around a constant value Ψ0, where m and n are integers.
More precisely, the first integral appearing on the rhs of Eq. (9) is solved perturbatively by introducing a polynomial expansion of u i ( t ) around t = t n, u j ( t ) = u n, j + u ˙ n, j δ t + 1 2 u ¨ n, j δ t 2 + 1 6 u … n, j δ t 3 + O ( δ t 4 ).
For beacon sizes around 723 bytes the N D T CP and N D T P are almost equal.
So one might ask: where are the zeros of polynomials like T n ( z ) + z k U n ( z ) or U n ( z ) + z k T n ( z ) around | z | = 1 ?
Denote by (tau_{k}) the required time for the solution ((x_{k}(t),y_{k}(t))) to complete n rotations around the point ((0,1)).
Clearly, each 2π-periodic solution ((x_{k}(t), y_{k}(t))) rotates clockwise strictly n turns around the origin in the interval ([0, 2pi]).
A partial opening of the breach region at the top of s3A and s5A strands occurs around t = 42 ns in the native NS conformer [36], while no similar events were detected in the trajectories of the cleaved and latent NSs.
