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By this approximation, which is valid only in the case of a rectangular window, the effects of computing the DFT on finite-length blocks are neglected.
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The correlation attraction between positively and negatively charged core blocks is neglected in this Poisson Boltzmann-like treatment of electrostatics.
Because the A and T bases alternate within the poly(AT) block, the change of the intensity corresponding to a 1 base pair displacement of the block is, neglecting the end-of-the-block effects, equivalent to moving all A and T nucleotides to the opposite strands of dsDNA.
The covariance matrices for the individual waveforms are arranged along the diagonal, while off-diagonal blocks (cross-covariances) are neglected and hence set to zeros.
Bridges are neglected.
Other siblings are neglected.
Some are neglected.
Connections between events are neglected.
Diffraction effects are neglected.
Viscoelastic effects are neglected.
Thermal effects are neglected.
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