Open maincold2 opened 7 months ago
as tforpoly^0 is 1. the means3D at the right of equaiton is the b_i_0
means3D = means3D*(tforpoly^0) + pc._motion[:, 0:3] * tforpoly^1 + pc._motion[:, 3:6] * tforpoly ^2 + pc._motion[:, 6:9] * tforpoly ^3
there is a special case when tforpoly=0
(t=trbfcenter). as we can get the initial position of each point at its corresponding time (although the position generated by colmap may not be accurate).
a spacetime point can be obeserved at position means3D
with highest possibility (trbf output is maximized) when t= trbfcenter.
Okay, I see, but the paper says b \in R, which I understand would be \in R^3. Would you please explain some about this?
that should be a small typo. for 3-dimension data like position, R is R^3, for 4-d quaternion, R is R^4.
Thank you for sharing your nice work!
I have a question about the polynomial equations in the paper. Eq.8 (omitting i): mu(t) = sum_k{b_k(t - mu^tau)^k}, where b \in R.
But referring to the code below, I understand the formulation would be: mu(t) = mu + sum_k{b_k(t - mu^tau)^k}, where b \in R^3.
Although b_0 could be mu, I hardly understand why b is a scalar.
https://github.com/oppo-us-research/SpacetimeGaussians/blob/c04db700a49fe67c94cbd2a6cff2f7d9c518aba8/thirdparty/gaussian_splatting/renderer/__init__.py#L90
I wonder what I missed and your explanation, thanks!