The paper deals with the theoretical investigation of surface polaritons (SP) in weakly disordered superlattice (WDSL), formed of the finite number of 2-dimensional electron systems (2DES). The weak disorderedness consists in the fact that one of the inner 2DES was shifted from the position of periodicity on some distance A . It is shown, that under the integer quantum Hall effect (IQHE) conditions all characteristics of SP are represented by the quantized values. The conditions under which the SP phase and group velocities in the finite WDSL can be considerably less than that in the isolated 2DES are defined.Surface polaritons (SP) in semiconductors with superlattices (SL) possess various and interesting properties. The weakly disordered SLs (WDSLs), which have some defect of SL's periodicity, are the objects of great researcher's interest. That defect consists in the fact that the SL contains one or several irregular 2-dimensional electron systems (2DES). These 2DES are characterizd either by the electron concentration different from that in the other 2DES or by shifting from their periodical position in the SL. Recently SPs were investigated in infinite [1,2,8], semiinfinite [3,4] and finite WDSL[5,6,7]. These papers show that the SP spectrum in WDSL is different considerably from the SP spectrum in the ordered SL. So, the SP spectrum in WDSL contain local modes of the SP, which electromagnetic field is localized in the vicinity of the WDSL's defect of periodicity.We consider the WDSL, formed of the finite number M of infinitely extended 2DES, arranged along z-axis at planes z = z , ( m = 0,. . . , M -1) and imbedded in the uniform dielectric medium with dielectric constant E . The constant quantizing magnetic field B is directed perpendicularly to 2DES along z-axis. We suppose that one of the inner 2DES ( m = 1,. . . , M -2 ) is shifted comparatively to it's periodical position on the distance A . Then the expression for the 2DES positions in the WDSL can be represented in the form: zm = md + Here Sm,q is the Cronecker symbol, d is the distance between the 2DES in the ordered SL; q = 1,. . . , M -2 is the number of shifted 2DES. We suppose that the Landau-level filling factor K is equal in all 2DES (K = rse2 n , e = (cxB)x is magnetic length, n is the electron density in 2DES). The analysis of the SP dispersion properties we will carry out using the formula for 2DES conductivity tensor obtained in [9,10]. Fig.1 presents the SP spectrum (bold solid lines)