A charged particle with charge `q` enters a region of constant, uniform and mututally orthogonal fields `vec(E) and vec(B)` with a velocity `vec(v)` perpendicular to both `vec(E) and vec(B)`, and comes out without any change in magnitude or direction of `vec(v)`. Then
A. `vecv=vecBxxvecE//E^2`
B. `vecv=vecExxvecB//B^2`
C. `vecv=vecBxxvecE//B^2`
D. `vecv=vecExxvecB//E^2`