By generalizing the Holstein-Primakoff realization and the Dyson realization of the Lie algebra SU(2), various realizations of the deformed angular momentum algebra R c 0 ,c 1 ,c 2 q,s , a five-parameter deformed SU(2) by combining Witten's two deformation schemes, are investigated in terms of the single boson and the single inversion boson respectively. For each kind, the unitary realization, the non-unitary realization, and their connection by the corresponding similarity transformation are respectively discussed. Lie algebras have played an exciting and significant role in the development of various branches of physics and many other areas of science and technology [1][2][3][4][5][6][7][8][9][10][11]. In 1983, Kulish et al. [12] showed that the algebra that governs the XXZHeisenberg spin model was a deformation of the Lie algebra SU(2), called nowadays SU q (2). Since then, there are many works devoted to various types of nonlinear algebras, i.e. some specific deformations of the usual Lie algebras obtained by introducing deformation parameters, due to their interesting mathematical structure and possible applications in a broad range of physical phenomena [13][14][15][16][17][18][19][20][21][22][23][24][25][26][27]. The nonlinear algebra to be discussed in this paper is a kind of multiparameter deformed angular momentum algebra, which generalizes Witten's first and second deformation schemes of SU (2) , whose three elements J μ (μ = 3, −, +) satisfy the following commutation relations: in order that the Casimir invariant of the type considered by Polychronakos [15] and Roček [16] exists in the limit of, and(1) reduces to Witten's first deformation, when q = r 2 , s = r 4 , C 0 = r, C 1 = 2r 2 /(1 − r 2 ), and C 2 = 0, eq. (1) to Witten's second deformation. Furthermore, different from the quantum group SU q (2) [13,19] and the polynomial angular momentum algebras [21][22][23][24], both the deformed commutators and the power series of J 3 appear in the algebraic structure (1). When q = s = C 0 = C 1 = C 2 = 1 (or q = s = C 0 = 1 and