[proofplan]
The Jacobian is invariant under translating the $G/T$ variable, so it is enough to compute the differential at $(eT,t)$. The quotient density identifies $T_{eT}(G/T)$ with $\mathfrak t^\perp$, and left translation identifies $T_tG$ with $\mathfrak g$, so the differential becomes a block triangular [linear map](/page/Linear%20Map) with identity on the $\mathfrak t$ direction and transverse block $\operatorname{Ad}_{t^{-1}}-\operatorname{id}_{\mathfrak t^\perp}$. Complexifying this transverse block diagonalizes it on the root spaces, and pairing the conjugate root spaces $\alpha$ and $-\alpha$ converts the complex eigenvalues into the real determinant $\prod_{\alpha\in R^+}|1-e^\alpha(t)|^2$.
[/proofplan]
custom_env
admin
[step:Reduce the Jacobian computation to the point $(eT,t)$]
Fix $g_0\in G$ and $t\in T_{\mathrm{reg}}$. Define the left translation map
\begin{align*}
L_{g_0}:G/T\to G/T
\end{align*}
by
\begin{align*}
L_{g_0}(hT):=g_0hT.
\end{align*}
Define the conjugation isometry
\begin{align*}
C_{g_0}:G\to G
\end{align*}
by
\begin{align*}
C_{g_0}(x):=g_0xg_0^{-1}.
\end{align*}
Because $(\cdot,\cdot)_{\mathfrak g}$ is $\operatorname{Ad}(G)$-invariant, left translations and conjugations preserve the Riemannian volume density on $G$, and $L_{g_0}$ preserves the quotient Riemannian density on $G/T$. Moreover,
\begin{align*}
\Phi(L_{g_0}(hT),t)=C_{g_0}(\Phi(hT,t)).
\end{align*}
Taking differentials at $(eT,t)$ gives
\begin{align*}
d\Phi_{(g_0T,t)}\circ (dL_{g_0})_{eT}=d(C_{g_0})_t\circ d\Phi_{(eT,t)}
\end{align*}
on the $G/T$ factor and the identity on the $T$ factor. Since both outside maps are isometries for the relevant densities, the absolute Jacobian satisfies
\begin{align*}
J_\Phi(g_0T,t)=J_\Phi(eT,t).
\end{align*}
Thus it remains to compute $J_\Phi(eT,t)$.
[/step]
custom_env
admin
[step:Identify the differential with a block triangular map on $\mathfrak t^\perp\oplus\mathfrak t$]
Let
\begin{align*}
q:G\to G/T
\end{align*}
be the quotient map. By definition of the quotient Riemannian density, the linear map
\begin{align*}
dq_e|_{\mathfrak t^\perp}:\mathfrak t^\perp\to T_{eT}(G/T)
\end{align*}
is an isometry. We identify $T_{eT}(G/T)$ with $\mathfrak t^\perp$ through this map. We identify $T_tT$ with $\mathfrak t$ by left translation by $t^{-1}$ in $T$, and identify $T_tG$ with $\mathfrak g$ by left translation by $t^{-1}$ in $G$.
Let $X\in\mathfrak t^\perp$ and $Y\in\mathfrak t$. Consider the smooth curve
\begin{align*}
\gamma_{X,Y}:(-\varepsilon,\varepsilon)\to G
\end{align*}
defined for sufficiently small $\varepsilon>0$ by
\begin{align*}
\gamma_{X,Y}(s):=\exp(sX)\exp(sY)t\exp(-sX).
\end{align*}
This curve represents the tangent vector $(X,Y)\in\mathfrak t^\perp\oplus\mathfrak t$ in the domain of $\Phi$ at $(eT,t)$. Left translating its derivative at $s=0$ by $t^{-1}$ gives
\begin{align*}
t^{-1}\gamma_{X,Y}'(0)=(\operatorname{Ad}_{t^{-1}}X)-X+Y.
\end{align*}
Since $T$ is abelian, $\operatorname{Ad}_{t^{-1}}Y=Y$. Since $\operatorname{Ad}_{t^{-1}}$ preserves $\mathfrak t$ and preserves the [inner product](/page/Inner%20Product), it also preserves $\mathfrak t^\perp$. Hence, under the above identifications,
\begin{align*}
d\Phi_{(eT,t)}(X,Y)=(\operatorname{Ad}_{t^{-1}}-\operatorname{id}_{\mathfrak t^\perp})X+Y.
\end{align*}
With respect to the orthogonal decompositions $\mathfrak t^\perp\oplus\mathfrak t$ in the domain and codomain, this map is block triangular, with transverse block $\operatorname{Ad}_{t^{-1}}-\operatorname{id}_{\mathfrak t^\perp}$ and torus block $\operatorname{id}_{\mathfrak t}$.
[/step]
custom_env
admin
[step:Reduce the absolute Jacobian to the transverse determinant]The preceding block triangular form implies
\begin{align*}
J_\Phi(eT,t)=\left|\det_{\mathbb R}(\operatorname{Ad}_{t^{-1}}-\operatorname{id}_{\mathfrak t^\perp})\right|\cdot \left|\det_{\mathbb R}(\operatorname{id}_{\mathfrak t})\right|.
\end{align*}
Since $\det_{\mathbb R}(\operatorname{id}_{\mathfrak t})=1$, we obtain
\begin{align*}
J_\Phi(eT,t)=\left|\det_{\mathbb R}(\operatorname{Ad}_{t^{-1}}-\operatorname{id}_{\mathfrak t^\perp})\right|.
\end{align*}[/step]
custom_env
admin
[guided]The point of the quotient-measure convention is used exactly here. The domain tangent space at $(eT,t)$ is identified isometrically with $\mathfrak t^\perp\oplus\mathfrak t$: the first summand comes from the quotient map $q:G\to G/T$, and the second summand comes from left translation on $T$. The target tangent space at $t\in G$ is identified isometrically with $\mathfrak g=\mathfrak t^\perp\oplus\mathfrak t$ by left translation by $t^{-1}$.
In these coordinates the differential is
\begin{align*}
(X,Y)\mapsto (\operatorname{Ad}_{t^{-1}}-\operatorname{id}_{\mathfrak t^\perp})X+Y.
\end{align*}
The first term belongs to $\mathfrak t^\perp$ because $\operatorname{Ad}_{t^{-1}}$ preserves both $\mathfrak t$ and the inner product, hence preserves the orthogonal complement $\mathfrak t^\perp$. The second term belongs to $\mathfrak t$. Therefore the matrix of the differential relative to the [orthogonal decomposition](/theorems/436) $\mathfrak t^\perp\oplus\mathfrak t$ is block triangular. Its diagonal blocks are
\begin{align*}
\operatorname{Ad}_{t^{-1}}-\operatorname{id}_{\mathfrak t^\perp}:\mathfrak t^\perp\to\mathfrak t^\perp
\end{align*}
and
\begin{align*}
\operatorname{id}_{\mathfrak t}:\mathfrak t\to\mathfrak t.
\end{align*}
The determinant of a block triangular linear map is the product of the determinants of its diagonal blocks. Thus
\begin{align*}
J_\Phi(eT,t)=\left|\det_{\mathbb R}(\operatorname{Ad}_{t^{-1}}-\operatorname{id}_{\mathfrak t^\perp})\right|\cdot \left|\det_{\mathbb R}(\operatorname{id}_{\mathfrak t})\right|.
\end{align*}
The identity map on $\mathfrak t$ has determinant $1$, so the entire Jacobian comes from the directions transverse to $T$:
\begin{align*}
J_\Phi(eT,t)=\left|\det_{\mathbb R}(\operatorname{Ad}_{t^{-1}}-\operatorname{id}_{\mathfrak t^\perp})\right|.
\end{align*}
This also explains why no Weyl group factor appears: we are computing a pointwise differential determinant, not counting how many points of $G/T\times T$ map to the same [conjugacy class](/page/Conjugacy%20Class).[/guided]
custom_env
admin
[step:Diagonalize the transverse operator on the complex root spaces]
Complexify the real [vector space](/page/Vector%20Space) $\mathfrak t^\perp$ and the real linear map
\begin{align*}
A_t:=\operatorname{Ad}_{t^{-1}}-\operatorname{id}_{\mathfrak t^\perp}.
\end{align*}
The standard root-space decomposition for a compact connected Lie group gives
\begin{align*}
(\mathfrak t^\perp)_{\mathbb C}=\bigoplus_{\alpha\in R}\mathfrak g_{\mathbb C,\alpha}.
\end{align*}
For $Z\in\mathfrak g_{\mathbb C,\alpha}$, the defining convention for $e^\alpha$ gives
\begin{align*}
\operatorname{Ad}_{t^{-1}}Z=e^{-\alpha}(t)Z.
\end{align*}
Therefore the complexified map $(A_t)_{\mathbb C}$ acts on $\mathfrak g_{\mathbb C,\alpha}$ by multiplication by
\begin{align*}
e^{-\alpha}(t)-1.
\end{align*}
Since each root space $\mathfrak g_{\mathbb C,\alpha}$ is one-dimensional, the complex determinant is
\begin{align*}
\det_{\mathbb C}((A_t)_{\mathbb C})=\prod_{\alpha\in R}(e^{-\alpha}(t)-1).
\end{align*}
[/step]
custom_env
admin
[step:Pair opposite roots to compute the real determinant]
Because $A_t$ is a real linear map, its real determinant equals the complex determinant of its complexification:
\begin{align*}
\det_{\mathbb R}(A_t)=\det_{\mathbb C}((A_t)_{\mathbb C}).
\end{align*}
Pairing the two factors corresponding to $\alpha$ and $-\alpha$ gives
\begin{align*}
(e^{-\alpha}(t)-1)(e^\alpha(t)-1).
\end{align*}
Since $e^\alpha(t)\in U(1)$, we have $e^{-\alpha}(t)=\overline{e^\alpha(t)}$. Hence
\begin{align*}
|(e^{-\alpha}(t)-1)(e^\alpha(t)-1)|=|1-e^\alpha(t)|^2.
\end{align*}
Taking the product over all positive roots gives
\begin{align*}
\left|\det_{\mathbb R}(A_t)\right|=\prod_{\alpha\in R^+}|1-e^\alpha(t)|^2.
\end{align*}
The assumption $t\in T_{\mathrm{reg}}$ says exactly that $e^\alpha(t)\neq 1$ for every $\alpha\in R$, so none of these factors vanishes and the differential is nonsingular at $(eT,t)$. Combining this determinant computation with the reduction above yields, for every $gT\in G/T$,
\begin{align*}
J_\Phi(gT,t)=\prod_{\alpha\in R^+}|1-e^\alpha(t)|^2.
\end{align*}
This is the claimed formula.
[/step]