We investigate the Hawking radiation of massive spin-1 vector particles, which are 9 coupled to vacuum fluctuations of a quantum field, from Rindler modified Schwarzschild black hole. 10 Rindler acceleration is used to produce the post-general relativistic theory of gravity for the distant 11 field of a point mass. The gravitational lensing problem of the Rindler modified Schwarzschild 12 black hole is also studied. We compute the deflection angle for the IR region (large distance limit as 13 infrared ) by using the Gaussian curvature of the optical metric of this back hole. Our investigations 14 clarify how the Rindler acceleration plays a role on the Hawking radiation and gravitational lensing. 15 16 p-1 arXiv:1702.04636v2 [physics.gen-ph] 9 Aug 2017 Sakalli et al.the correlations between the HR and the background geometry [9]. It is worth noting that 38 correlations account for the information stored in the BH with the collapsing matter. Since 39 the original studies of BH emission [1, 2], works on the HR have been still continuing. To 40 date, HR was verified by various methods for many different types of particles having spin 41 s = 0, 1/2, 1, 3/2, 2, ... [10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][89][90][91][92]. HR studies include the lower and higher dimensional 42 BHs, wormholes, and black strings [25, 26,[29][30][31][32][33][34]. Recent studies [35][36][37] have claimed that 43 HR has been observed in the laboratory environment. Those experiments about HR were 44 conducted by Steinhauer, who used a sonic (or the so-called analogue) BH in an atomic 45 Bose-Einstein condensate [38] so that a state, where gas bosons are cooled to temperatures 46 very close to absolute zero (that is, very near 0K or −273.16 • C). Thus, the sonic BH 47 could mimic a real cosmic event horizon. At this stage, Steinhauer managed to observe the 48 particles of sound (phonons) at the BH's event horizon and found that sound waves in the 49 Bose-Einstein condensate obey Hawking's theory [37]. However, many physicists are still 50 cautious about these results. Other experiments are needed to support the experiment of 51 Steinhauer.52 In particle physics, spin-1 particles are called vector particles. The most well-known 53 massive spin-1 particles, which are described by a three-dimensional spin vector are the weak 54 intermediate vector bosons Z and W ± , and the mesons Υ, J/Ψ, φ, and ρ [39]. Photons 55 are the massless spin-1 particles, which can only be directed parallel or anti-parallel to their 56 direction of motion. Free massive spin-1 fields are governed by the Proca field equation, 57 and massless spin-1 fields are governed by the Maxwell field equation. Compelling evidence 58 suggests that the spin-1 fields are potential dark matter candidates [40-42]. In recent years, 59 HR of the spin-1 particles have attracted considerable interest [43-49]. 60 In this study, we consider the Rindler modified Schwarzchild BH (RMSBH) [50,51], which 61 was initially proposed by Grumiller to explain the mysterious attract...