14 m$_{t}$ ′ ( GeV ) 300 400 500 600 λ s t ′ (0.09 - 2.5) (0.08 - 1.4) (0.06 - 0.9) (0.05 - 0.6) φ ′ s 0 → 80 0 → 80 0 → 80 0 → 80 TABLE IV: Allowed ranges for the parameters, λ s t ′ ( × 10 − $^{2}$) and phase φ ′ s (in degree) for different masses m$_{t}$ ′ ( GeV), that has been obtained from the fitting with the inputs in Table III and allowed by the present experimental bound for CP asymmetry in B$_{s}$ → J/ψφ [15]. III. PREDICTIONS IN THE SM4 FIG. 1: (a) Correlation between S$_{φK}$$_{s}$ and S$_{ψφ}$ (left panel) and (b) Variation of S$_{ψφ}$ with the phase φ ′ s of λ s t ′ (right panel), for m$_{t}$ ′ = 300 (magenta), 400 (red), 500 (green) and 600 (blue) GeV respectively. The horizontal lines (left panel) represent the experimental 1 σ range for S$_{φK}$$_{s}$ whereas the vertical lines (black 1- σ and red 2- σ ) represent that for S$_{ψφ}$ ; in the right panel the horizontal lines are for S$_{ψφ}$ -1 -0.8 -0.6 -0.4 -0.2  0  0.2  0.4  0.6  0.8  1 -80 -60 -40 -20  0  20  40  60  80 S $_{s}$’  0.2  0.3  0.4  0.5  0.6  0.7  0.8  0.9 -1 -0.8 -0.6 -0.4 -0.2  0  0.2  0.4  0.6  0.8  1 S$^{φ}$  K s S Fig. 1 (left panel) shows the correlations between the CP asymmetries in B$_{d}$ → φK$_{s}$ and B$_{s}$ → ψφ whereas right panel shows the variation S$_{ψφ}$ with the new phase φ ′ s $^{1}$; which has already been shown in our previous article [15] for m$_{t}$ ′ = 400 , 500 and 600 GeV ; here, we 1 Soon after we posted version 1 of our paper , [70] appeared which also discusses about the phenomenology of SM4. To facilitate direct comparision with that work we are adding few extra figures in this revised version.