Obtaining Classical Wiener Space from abstract Wiener measure The question
I'm working on understanding the Abstract Wiener Space construction and wanted to rederive the defining property of the classical counterpart,
$$\require{cancel} \xcancel{\xi_{t+s} - \xi_t}\ B_{t+s} - B_t\sim \mathcal{N}(0, s) \quad(\text{for } s> 0), \tag{1}$$
from the Abstract Wiener Space as constructed on the Wikipedia page and here.

The setup
That is, I assume to know that $\xi \in W^{2,1}_0[0,T] =: \mathcal{H}$, i.e., $\xi: [0,T] \to \mathbb{R}$ is an absolutely continuous path with square-integrable first derivative and $\xi(0) = 0$. The inner product on $\mathcal{H}$ shall be defined as
$$(\xi, \zeta) = \int_0^T \dot{\xi}(t) \dot{\zeta}(t) \,\mathrm{d}t, \tag{a}$$
and from the construction we know there exists a measure $\mu$ which acts on the algebraic dual space $E^a$ and which has the properties (Defs. 20 and 25 of Velhinho)
$$\forall\, \xi \in \mathcal{H}: \quad \chi(\xi) := \int_{E^a} e^{i\phi(\xi)}\, \mathrm{d}\mu(\phi) = e^{-\frac{1}{2}(\xi,\xi)} \tag{b}$$
and (Theorem 11, which I believe is a special case of the cylinder set measure property, correct me if I'm wrong)
$$\forall\, \xi \in \mathcal{H}, A \in \mathcal{B}(\mathbb{R}): \quad \mu_\xi(A) := \mu(\{\phi \in E^a \mid \phi(\xi) \in A \}) = \frac{1}{\sqrt{2\pi (\xi,\xi)}} \int_A e^{-\frac{x^2}{2(\xi,\xi)}} \,\mathrm{d}x. \tag{c}$$

My attempt at a solution (see edit below!)
I have the following idea, but I'm not sure if it's right:
What we want to show in (1) is equivalent to
$$P(\{\xi(t+s) - \xi(t) \in A\}) = \frac{1}{\sqrt{2\pi s}}\int_A e^{-\frac{x^2}{2s}} \,\mathrm{d}x$$
for any Borel set $A \in \mathcal{B}(\mathbb{R})$.
We may note that
$$\xi(t+s) - \xi(t) =  \int_t^{t+s} \dot{\xi}(\tau)\, \mathrm{d}\tau = \int_0^{T} \dot{f}(t) \dot{\xi}(\tau)\, \mathrm{d}\tau \quad \text{with } \dot{f}(\tau) = 1_{[t,t+s]}(\tau).$$
Now, since every $\xi \in \mathcal{H}$ will also have a dual element $\phi_\xi \in E^a$ and $f$ as implicitly defined above is a valid element of $\mathcal{H}$, we can swap the roles of $\xi$ and $f$ to define
$$\xi(t+s) - \xi(t) =: \phi_\xi(f).$$
Then we can apply (c) to find that
$$\mu_f(A) = \frac{1}{\sqrt{2\pi (f,f)}}\int_A e^{-\frac{a^2}{2(f,f)}}\,\mathrm{d}x = \frac{1}{\sqrt{2\pi s}}\int_A e^{-\frac{a^2}{2s}}\,\mathrm{d}x,$$
where we used $(f,f) = s$ via definition (a).
This looks like the right result, but the way there seems a bit odd, and it also glosses over the fact that the set that is measured in (c) includes $\phi$ that are not duals $\phi_\xi$ of some $\xi$. Is it obvious that these will contribute with measure zero?
Feel free to point me to a good introductory text that gives more context, if necessary!

Edit: Revised attempt
I found part of the problem:
In (1), $\xi$ was the Brownian motion itself, whereas in (a) through (c), $\xi$ was an element of the Cameron–Martin Hilbert space. However, the Brownian motion sample paths are not elements of the Hilbert space, but rather of the Banach space $E^a$. Thus, I should replace (1) with
$$B_{t+s} - B_t \sim \mathcal{N}(0, s)$$
to make the distinction between $\xi$ and $B$ obvious.
Then the rest of the argument continues as before, i.e.
$$
B(t+s) - B(t) = \int_0^T \dot{B}(\tau) \dot{\xi}(\tau)\, \mathrm{d}\tau \quad \text{with } \dot{\xi}(\tau) = 1_{[t,t+s]}(\tau)
\implies \mu_\xi(A) = \frac{1}{\sqrt{2\pi s}} \int_A e^{-x^2/(2s)} \,\mathrm{d} x,
$$
but we now face a different problem, namely that $B(\tau)$ is a.s. not differentiable and that hence the integral that I just wrote does not exist for a.e. $B$. I've considered interpreting $\dot{B}$ in the distributional sense, but $\xi$ is not a test function, so that doesn't seem to work, I don't know if there's some closure/completion/limiting property that can be used instead.
 A: I still welcome other answers from more knowledgeable people, but I believe I have found the solution to this problem:
In the standard formulation of abstract Wiener spaces, the measure $\mu$ is not on the algebraic dual space explicitly, but just on some Banach space $W$, and the abstract Wiener space itself is said to be the triple $i: \mathcal{H} \to W$.
In the classical case, $W$ is the set of continuous functions $B(t) \in C[0,T]$ with $B(0) = 0$ and $i$ is the inclusion map from $W^{2,1}_0[0,T]$ to $W$. Let $j: W^\ast \to \mathcal{H}$ be the adjoint of $i$, i.e., $(j(\ell), h) = \ell(i(h))\ \forall \ell \in W^\ast, h \in \mathcal{H}$.
On this space, the evaluation functional $\delta_s : B \mapsto B(s)$ is a continuous linear functional and thus an element of the continuous dual space $W^\ast$.
Then $\delta_{t+s} - \delta_t$ is also an element of $W^\ast$, and we may note that $j(\delta_{t+s} - \delta_t) = f$ as given in the question (i.e., the "stopped" ramp function fulfilling $\dot{f}(\tau) = 1_{[t,t+s]}(\tau)$ with $f(0) = 0$).
Now, finally, by definition/construction, the Wiener measure $\mu$ is the radonification of the canonical Gaussian cylinder set measure on $\mathcal{H}$. In particular, this means that any $\ell \in W^\ast$ is distributed as $\mathcal{N}(0, {\|\left(\ell \circ i\right)^\sharp\|_\mathcal{H}}^2) = \mathcal{N}(0, {\|j(\ell)\|_\mathcal{H}}^2)$, where $\left(\ell \circ i\right)^\sharp \in \mathcal{H}$ is the Riesz representative of $\ell \circ i \in \mathcal{H}^\ast$. Thus, since $\delta_{t+s} - \delta_t =: \ell \in W^\ast$ corresponds to the random variable I was looking for and $j(\ell) = f$ as given in the question, we find that
$${\|j(\ell)\|_\mathcal{H}}^2 = \int_0^T \left(1_{[t,t+s]}(\tau) \right)^2 \,\mathrm{d}\tau = s$$
and therefore $B_{t+s} - B_{t} \sim \mathcal{N}(0,s)$ (for $s > 0$).
I wouldn't have figured this out without the help of Nathaniel Eldredge's and David Elworthy's lecture notes (in particular, sections 3 through 6 of the latter).

However, I'm still not entirely sure how this can be translated to the algebraic-dual-space formulation of Velhinho without appealing to the same argument using $i$ and $j$ as I did here.
I have the following idea, which doesn't seem quite satisfactory to me:
For any $s \in [0, T]$, the function $g_s: [0,T] \to \mathbb{R}$ defined by
$$g_s(\tau) = \begin{cases} \tau, & \tau < s\\ s, & \tau \geq s\end{cases}$$
is an element of $\mathcal{H}$. We can somewhat arbitrarily define this to be the evaluation functional on $E^a$—motivated by $\int_0^T \dot{B}(\tau) \dot{g}_s(\tau)\ \mathrm{d}\tau$ when it exists—in the sense that $\delta_s(B) = B(g_s) := B_s$ for $B \in E^a$. Then $g_{t+s} - g_{t}$ is the $f$ from the question with ${\|g_{t+s} - g_t\|_\mathcal{H}}^2 = s$ and hence
$$B(g_{t+s} - g_s) = B_{t+s} - B_s \sim \mathcal{N}(0, s).$$
I still wonder if there is some way to get around the apparent arbitrariness of this way of defining the evaluation functional.
