The possible existence of the bound states of the interacting two-dimensional (2D) magnetoexcitons in the lowest Landau levels (LLLs) approximation was investigated using the Landau gauge description. The magnetoexcitons taking part in the formation of the bound state with resultant wave vector k=0k=0 have opposite in-plane wave vectors kk and −k−k and look as two electric dipoles with the arms oriented in-plane perpendicularly to the corresponding wave vectors. The bound state of two antiparallel dipoles moving with equal probability in any direction of the plane with equal but antiparallel wave vectors is characterized by the variational wave function of the relative motion φn(k)φn(k) depending on the modulus |k||k|. The spins of two electrons and the effective spins of two holes forming the bound states were combined separately in the symmetric or in the antisymmetric forms (↑↓+η↓↑)(↑↓+η↓↑) with the same parameter η=±1η=±1 for electrons and holes. In the case of the variational wave function φ2(k)=(8α3)1/2k2l20exp[−αk2l20]φ2(k)=(8α3)1/2k2l02exp⁡[−αk2l02] the maximum density of the magnetoexcitons in the momentum space representation is concentrated on the in-plane ring with the radius kr=1/(α−−√l0).kr=1/(αl0). The stable bound states of the bimagnetoexciton molecule do not exist for both spin orientations. Instead of them, a deep metastable bound state with the activation barrier comparable with the ionization potential IlIl of the magnetoexciton with k=0k=0 was revealed in the case η=1η=1 and α=0.5α=0.5. In the case η=−1η=−1 and α=3.4α=3.4 only a shallow metastable bound state can appear.