sneaky666 said:
ok i see, but i looked on wikipedia and for the bounoulli dist. and geometric dist. i thought it was
PX(X=1) = θ
PX(X=0) = 1-θ
PX(X=x) = 0 otherwise
PY(Y=y>=0) = θ(1-θ)^y
PY(Y=y) = 0 otherwise
or is this basically what you have? and why did you also add those extra functions in them?, I don't understand how your getting those functions from what i have...
Yes, your functions and mine are equivalent. I added the extra functions so I don't have to express them as individual cases (x = 1, x = 0, otherwise) as you did.
To see that mine are the same as yours, just plug in various values of [itex]k[/itex].
For example, if
[tex]b(k) = (1 - \theta)\delta(k) + \theta\delta(k-1)[/tex]
then notice that [itex]\delta(k)[/itex] is zero except when [itex]k = 0[/itex], and [itex]\delta(k-1)[/itex] is zero except when [itex]k = 1[/itex].
Thus [itex]b(0) = (1 - \theta)(1) + 0 = (1 - \theta)[/itex] and [itex]b(1) = 0 + \theta(1) = \theta[/itex] and [itex]b(k) = 0[/itex] if [itex]k[/itex] is neither 0 nor 1.
Similarly with the geometric distribution.
The point is that it makes it possible to write a one-line expression that is valid for all [itex]k[/itex], which in turn makes it easier to express the convolution sum.
By the way, this isn't some weird invention of mine - it's a standard thing to do when working with functions defined in pieces, and the notation ([itex]\delta(k)[/itex] and [itex]u(k)[/itex]) are quite standard as well.