We show that a pair of massive relativistic spin-1/2 particles prepared in a maximally entangled spin state in general is not capable of maximally violating the Clauser-Horne-Shimony-Holt (CHSH) version of Bell's inequalities without a post-selection of the particles momenta, representing a major difference in relation to non-relativistic systems. This occurs because the quantization axis of the measurements performed on each particle depends on the particle velocity, such that it is not possible to define a reduced density matrix for the particles spin. We also show that the amount of violation of the CHSH inequality depends on the reference frame, and that in some frames the inequality may not be violated.PACS numbers: 03.65. Ud, 03.65.Ta, 03.30.+p, Special relativity and quantum mechanics were two theories constructed in the last century that completely changed our way to see nature, being the foundations of present-day theoretical physics. One of the most striking features of quantum mechanics is entanglement, that leads to quantum correlations among parties of a system that are stronger than what is allowed by classical physics [1][2][3]. Recently questions regarding the behaviour of the entropy and entanglement of quantum systems in different reference frames gave rise to the field of relativistic quantum information [4][5][6]. Since then, many studies of relativistic effects on spin quantum correlations of massive particles have appeared in the literature [4,[7][8][9][10][11][12][13][14][15][16][17][18][19][20].In the seminal work of Peres, Scudo and Terno [5], they showed that the reduced density matrix for the spin of a relativistic particle, that should give "the statistical predictions for the results of measurements of spin components by an ideal apparatus which is not affected by the momentum of the particle" [5], is not covariant under Lorentz transformations. This occurs because under a Lorentz boost the particle spin undergoes a Wigner rotation [21,22], which correspond to a momentumdependent change of the particle spin state. One aspect extensively studied in the posterior works on relativistic quantum information was the influence of the Wigner rotations on the amount of entanglement of the reduced spin density matrix of a system with two ore more particles in different reference frames [8,10,[15][16][17]19]. However, in our recent work [23] we discussed that since it is not possible to measure the spin of a relativistic particle in a independent way from its momentum, the definition of a reduced density matrix for the particle spin is meaningless. The ideal apparatus which is not affected by the particle momentum conjectured by Peres et al. [5] does not exist, contradicting the assumptions (explicitly or implicitly) made by the cited works [5,6,8,10, 15- * Electronic address: saldanha@df.ufpe.br 17,19,20].A second aspect studied in many of the previous works on the subject is the influence of the dependence of the Pauli-Lubanski (or similar) spin operators with the particles momenta on the amo...