Raman spectra of ordinary and extraordinary phonons in LiNbO, and LiTaO, are recorded under a set of angles between wave vector and optic axis with the same backward scattering geometry, which makes all of the extraordinary phonons to appear in one directional-dispersion spectra series, and the directional dispersion is reliably determined. The symmetry and the number of polar phonons in both the crystals are found to be the same, 4AlrThe directional dispersion of extraordinary phonons has thirteen branches with similar coupling in LiNbO, and LiTaO,. C oc060B reoMeTpmeB paccemm ~a a a~ mccnenosaHbI cnewpbi KOM6HHaUMOHHO~O paCCeRHllR 06bIKHOBeHHbIX H HeO6bIKHOBeHHbIX @OHOHOB B LiNbO, II LiTaO, KpllCTaJIJIaX IlpH Cepllll YTJIOB MelKHy BOJIHOBbIM BeKTOPOM II OIITllqeCHOg OCbH). B OHHOfi CepHll CIIeK-TPOB YrJIOBOfi AIICIlepCIIll IlORBHJIllCb BCe IIOJIOCbI HeO6bIKHOBeHHbIX @OHOHOB , II YrJIOBaR ~EiClIepCllR gaCTOT 6bma OIlpeAeJIeHa HaAeWHO. CHMMeTPIIR II YllCJIO IIOJlRpHbIX QOHOHOB B 06011~ xpkicTannax opmaKoBb1, T.e. 4 A 1~ + 4 A 1~ + ~E T + EL. YrnoBa, Hmnep-CIIH HeO6bIKHOBeHHbIX @OHOHOB IIMeeT BeTBbI c n o~o 6~o H CBRBbH) B LiNbO, II LiTaO,. l) Weijin Road 94, Tianjun, The People's Republic of China.