The following is a long and argumentative answer with the first part being somewhat philosophical and the second part being most relevant to the question asked here.
In probability theory, independence is usually
an assumption that is given as part of the problem statement
as in "Let $A$ and $B$ denote independent events" or "Let $X$ and $Y$
denote independent random variables" and this means that the events
or random variables enjoy a property that does not hold for events
or random variables in general. Specifically,
$$P(A\cap B) = P(A)P(B)$$
and
$$P\{X \in \mathcal A, Y \in \mathcal B\} =P\{X \in \mathcal A\}P\{Y \in \mathcal B\}$$
for all sets $\mathcal A$ and $\mathcal B$ in the $\sigma$-algebra. Independence
of random variables $X$ and $Y$
implies the more commonly used statement
$$P\{X \leq a, Y \leq b\} = F_{X,Y}(a,b)
= P\{X \leq a\}P\{Y \leq b\} = F_{X}(a)F_{Y}(b), \forall a, b$$
as well as $p_{X,Y}(a,b) = p_X(a)p_Y(b)~ \forall a, b$ for discrete
random variables and
$f_{X,Y}(a,b) = f_X(a)f_Y(b)~\forall a, b$ for continuous random variables (note that
independence of continuous random variables $X$ and $Y$ implies joint
continuity of $X$ and $Y$). Let us call this the product rule.
In practical applications, where $X$
and $Y$ are random variables modeling physical phenomena,
things are not quite so straightforward. If $X$ and $Y$ are arising
from distinct physically unrelated sources, we take them to be
independent and apply the product rule. Note that there is
no proof of independence, only a general feeling that one
phenomenon does not affect the other and so independence is
a reasonable assumption. In some cases, of course, beauty
might lie in the eye of the beholder (or the author, reviewer,
and editor) but might be completely invisible to the general
reader. But the notion is that physical independence, whether
such independence is assumed or a reasonable argument made in
support thereof, justifies the use of the product rule.
A third form of independence is stochastic independence:
$A$ and $B$ are said to be independent events if $P(A\cap B) = P(A)P(B)$.
Physical independence implies stochastic independence but the
converse need not be true. Here is an example whose underlying
idea might be familiar to the reader in the guise of coin-tossing.
Consider an Exclusive-OR (XOR) circuit whose inputs $X$ and $Y$ are
are physically independent Bernoulli random variables taking on values
$0$ and $1$ with probability $\frac{1}{2}$. Physically independent
because they are coming from physically independent sources, say
from two different data packets sent by two different computers
in two different parts of the country. The output $Z = X \oplus Y$ has value
$1$ exactly when one of $X$ and $Y$ has value $1$ and the other has value
$0$. It is easy to show that $Z$ is also a Bernoulli random variable
with parameter $\frac{1}{2}$. Now, $Z$ is clearly physically dependent
on $X$ -- the output of an XOR circuit should depend on its inputs --
but $Z$ and $X$ are stochastically independent random variables:
$$\begin{align*}
p_{X,Z}(0,0) &= P\{X = 0, Z = 0\} = P\{X = 0, Y = 0\} = p_{X,Y}(0,0) = \frac{1}{4}
= p_X(0)p_Z(0)\\
p_{X,Z}(0,1) &= P\{X = 0, Z = 1\} = P\{X = 0, Y = 1\} = p_{X,Y}(0,1) = \frac{1}{4}
= p_X(0)p_Z(1)\\
p_{X,Z}(1,0) &= P\{X = 1, Z = 0\} = P\{X = 1, Y = 1\} = p_{X,Y}(1,1) = \frac{1}{4}
= p_X(1)p_Z(0)
\\p_{X,Z}(1,1) &= P\{X = 1, Z = 1\} = P\{X = 1, Y = 0\} = p_{X,Y}(1,0) = \frac{1}{4}
= p_X(1)p_Z(1)
\end{align*}$$
Similarly, $Y$ and $Z$ are stochastically independent but physically dependent
random variables.
Thus, stochastic independence does not necessarily mean physical
independence; it might just be an artifact of the probability
assignment. If we re-work the above example with $X$ and $Y$
physically independent Bernoulli random variables with parameter
$p \in (0,1), ~ p \neq \frac{1}{2}$, then we see that $Z$ is no
longer stochastically independent of $X$. Thus, the independence
of $X$ and $Z$ is an artifact of the probability assignment or the
possibility that when the model was being devised, the hypothesis
$p = \frac{1}{2}$ did not get rejected because the test did not
give a statistically significant result!
Currently studies that can be
tarred broadly as saying "Everything is independent unless someone beats
me on the head and says it is not." seem to be in great vogue.
Turning to the OP's edited question,
Random variables: $X_1$, $X_2$, $X_3$, $X_4$ with the following density functions.
$X_1 \sim \mathrm{Bernoulli}(1/2)$
$X_2 \sim \mathrm{Bernoulli}(1/2)$
$X_3 \mid (X_1,X_2) \sim \mathcal N(X_1+X_2,\sigma^2)$
$X_4 \mid X_2 \sim \mathcal N(aX_2+b,1)$
The above specification doesn't necessarily mean that:
$p(x_3,x_4|x_2)=p(x_3|x_2)p(x_4|x_2)$
Note that nothing is said about whether $X_1$ and $X_2$ are
independent, whether physically or stochastically, nor is
anything said about independence or lack thereof of $X_3$ and $X_4$.
Are they all assumed to be independent because everything is
independent?
The conditional joint density of $X_3$ and $X_4$ given
$X_2$ cannot be computed from the given information, and so
whether or not the product rule
$$p(x_3,x_4|x_2)=p(x_3|x_2)p(x_4|x_2)$$
holds or not cannot be determined from the given information.
In any case, there seems to be no obvious reason why the
product rule should hold, and I don't see the faiure as
being indicative of anything except that the assumption of
independence everywhere does not seem to be working here.