The theory of an atom dipole trap composed of a focused, far red-detuned, t
rapping laser beam, and a pair of red-detuned, counterpropagating, cooling
beams is developed for the simplest realistic multilevel dipole interaction
scheme based on a model of a (3+5)-level atom. The description of atomic m
otion in the trap is based on the quantum kinetic equations for the atomic
density matrix and the reduced quasiclassical kinetic equation for atomic d
istribution function, ft is shown that when the detuning of the trapping fi
eld is much larger than the detuning of the cooling field, and with low sat
uration, the one-photon absorption (emission) processes responsible for the
trapping potential can be well separated from the two-photon processes res
ponsible for sub-Doppler cooling atoms in the trap. Two conditions are deri
ved that are necessary and sufficient for stable atomic trapping. The condi
tions show that stable atomic trapping in the optical dipole trap can be ac
hieved when the trapping field has no effect on the two-photon cooling proc
ess and when the cooling field does not change the structure of the trappin
g potential but changes only the numerical value of the trapping potential
well. It is concluded that the separation of the trapping and cooling prece
sses in a pure optical dipole trap allows one to cool trapped atoms down to
a minimum temperature close to the recoil temperature, keeping simultaneou
sly a deep potential well.