The Kronecker delta is a discrete-index “indicator” function: at and everywhere else.

This is the discrete analog of the continuous Dirac delta . The two are different objects: is a distribution defined by its integral behavior, while is an ordinary function taking values 0 or 1. Check the argument (continuous parenthesis vs discrete bracket ) to disambiguate.

Stride- Kronecker delta

The course uses a generalization, the Kronecker delta with stride :

So when is an integer multiple of , and 0 otherwise.

  • for every integer — every integer is a multiple of . So is “always 1” and can be dropped from expressions.
  • — only is a multiple of “infinity” (interpreted in the limit). This is just the ordinary discrete delta.
  • picks out even indices: at , zero elsewhere.

Where this shows up

The stride- Kronecker delta appears throughout the Fourier series standard pairs. A signal that is the result of convolving a pulse with a periodic impulse train has Fourier coefficients of the form

where is the integer such that the representation period . The factor masks out the harmonic indices that aren’t multiples of — exactly the indices where the periodic-train spectrum has nonzero coefficients.

Why two notations matter

If you encounter in a time-domain integral, it’s the continuous impulse — use the sifting property. If you encounter in a discrete-index sum, it’s the Kronecker delta — just at . Confusing them produces nonsense, because they have different defining properties (sifting for the continuous one, pointwise values for the discrete one).