We construct a master dynamical system on a $${\text {U}}(n)$$
U
(
n
)
quasi-Poisson manifold, $${\mathcal {M}}_d$$
M
d
, built from the double $${\text {U}}(n) \times {\text {U}}(n)$$
U
(
n
)
×
U
(
n
)
and $$d\ge 2$$
d
≥
2
open balls in $$\mathbb {C}^n$$
C
n
, whose quasi-Poisson structures are obtained from $$T^* \mathbb {R}^n$$
T
∗
R
n
by exponentiation. A pencil of quasi-Poisson bivectors $$P_{\underline{z}}$$
P
z
̲
is defined on $${\mathcal {M}}_d$$
M
d
that depends on $$d(d-1)/2$$
d
(
d
-
1
)
/
2
arbitrary real parameters and gives rise to pairwise compatible Poisson brackets on the $${\text {U}}(n)$$
U
(
n
)
-invariant functions. The master system on $${\mathcal {M}}_d$$
M
d
is a quasi-Poisson analogue of the degenerate integrable system of free motion on the extended cotangent bundle $$T^*\!{\text {U}}(n) \times \mathbb {C}^{n\times d}$$
T
∗
U
(
n
)
×
C
n
×
d
. Its commuting Hamiltonians are pullbacks of the class functions on one of the $${\text {U}}(n)$$
U
(
n
)
factors. We prove that the master system descends to a degenerate integrable system on a dense open subset of the smooth component of the quotient space $${\mathcal {M}}_d/{\text {U}}(n)$$
M
d
/
U
(
n
)
associated with the principal orbit type. Any reduced Hamiltonian arising from a class function generates the same flow via any of the compatible Poisson structures stemming from the bivectors $$P_{\underline{z}}$$
P
z
̲
. The restrictions of the reduced system on minimal symplectic leaves parameterized by generic elements of the center of $${\text {U}}(n)$$
U
(
n
)
provide a new real form of the complex, trigonometric spin Ruijsenaars–Schneider model of Krichever and Zabrodin. This generalizes the derivation of the compactified trigonometric RS model found previously in the $$d=1$$
d
=
1
case.