Algebraic & modulo–2 sumTable for moment calculation
A "clocked" random number generator returns a sequence $\langle x_\nu \rangle$ of binary random numbers.
It is assumed that the binary numbers $0$ and $1$ occur with equal probabilities and that the individual random numbers do not depend on each other.
The random numbers $ x_\nu \in \{0, 1\}$ are entered into the first memory location of a shift register and shifted down one digit with each clock pulse.
Two new random sequences $\langle a_\nu \rangle$ and $\langle m_\nu \rangle$ are formed from the contents of the three-digit shift register. Here denotes:
(2) The table shows that for each preassignment ⇒ $( x_{\nu-1}, x_{\nu-2}) = (0,0), (0,1), (1,0), (1,1)$ the values $m_\nu = 0$ respectively $m_\nu = 1$ are equally likely.
This exactly matches the definition of "statistical independence" ⇒ Answer 1.
2D PDF of $x$ and $m$
(3) Correct are the second and the last suggested solutions.
The 2D PDF consists of four Dirac functions, each with weight $1/4$.
One obtains this result, for example, by evaluating the table on the data page.
Since $f_{xm}(x_\nu, m_\nu)$ is equal to the product $f_{x}(x_\nu) \cdot f_{m}(m_\nu)$ the quantities $x_\nu$ and $m_\nu$ are statistically independent.
Statistically independent random variables, however, are also linearly statistically independent, so they are certainly uncorrelated.
(4) Within the sequence $\langle a_\nu \rangle$ of algebraic sum there are statistical bindings ⇒ Answer 2.
You can see this because the unconditional probability $ {\rm Pr}( a_{\nu} = 0) =1/8$ is,
while, for example ${\rm Pr}(a_{\nu} = 0\hspace{0.05cm}|\hspace{0.05cm}a_{\nu-1} = 3) =0$ holds.
2D PDF of $a$ and $m$
(5) Correct are the first and the last suggested solutions:
As in the subtask (3) there are again four Dirac functions, but this time not with equal momentum weights $1/4$.
The two-dimensional PDF thus cannot be written as a product of the two marginal probability densities.
But this means that statistical bindings must exist between $a_\nu$ and $m_\nu$ .