Gubser flow is an axis-symmetric and boost-invariant evolution in a relativistic quantum field theory which is best studied by mapping $$\textbf{R}^{3,1}$$
R
3
,
1
to $$dS_{3}\times \textbf{R}$$
d
S
3
×
R
when the field theory has conformal symmetry. We show that at late de-Sitter time, which corresponds to large proper time and central region of the future wedge within $$\textbf{R}^{3,1}$$
R
3
,
1
, the holographic conformal field theory plasma can reach a state in which $$\varepsilon = P_T = - P_L$$
ε
=
P
T
=
-
P
L
, with $$\varepsilon $$
ε
, $$P_T$$
P
T
and $$P_L$$
P
L
being the energy density, transverse and longitudinal pressures, respectively. We further determine the full sub-leading behaviour of the energy–momentum tensor at late time. Restricting to flows in which the energy density decays at large transverse distance from the central axis in $$\textbf{R}^{3,1}$$
R
3
,
1
, we show that this decay should be faster than any power law. Furthermore, in this case the energy density also vanishes in $$\textbf{R}^{3,1}$$
R
3
,
1
faster than any power as we go back to early proper time. Hydrodynamic behavior can appear in intermediate time.