Figure 44

Figure 44: In solid blue, the Zhao–Famaey [508] &tidle;μ(s)-function (Eq. 79View Equation) of TeVeS (Section 7.3 and 7.4), compared to the original Bekenstein one (dashed green) with a discontinuity at s = 0 [33]. The ZF function provides a more natural transition from static systems (the positive side) to cosmology (the negative side).