The full bound rovibrational spectra
E
(
ν
,
L
)
for the ground electronic state
X
1
Σ
+
of the hydrogen bromine HBr and hydrogen iodine HI is calculated in the Born-Oppenheimer approximation. As a starting point an analytical expression for the potential energy curve V(R), valid in the entire domain
R
∈
[
0
,
∞
)
, is obtained in the form of a two-point Padé approximant that correctly reproduces the asymptotic behavior for small
R
→
0
and large
R
→
∞
internuclear distances. Remaining free parameters are fixed by making a fit with the experimental RKR points. In a second stage, the rovibrational spectra
E
(
ν
,
L
)
is obtained by solving the nuclear Schröodinger equation with nuclear interaction V(R). It was found that the potential energy curve for the ground electronic state
X
1
Σ
+
supports a total of 798/748 rovibrational states with maximal vibrational/rotational quantum numbers
v
max
=
19
/
17
and
L
max
=
65
/
66
for hydrogen halides HBr/HI, respectively. Through a simple modification in the nuclear Schröodinger equation, the bound rovibrational spectra
E
(
ν
,
L
)
is obtained for the isotopological species with deuterium (D) and tritium (T) content: DBr/TBr (1575/2329 states in total with
ν
max
=
27
/
34
and
L
max
=
92
/
112
) and DI/TI (1485/2207 states in total with
ν
max
=
25
/
31
and
L
max
=
93
/
114
).