“…However, the most general form of a relationĝ µν =ĝ µν (φ, g µν ) which still complies with physical requirements such as causality, is a so called disformal relation, [4] g µν = C(φ, X)g µν + D(φ, X)φ ,µ φ ,ν , (1.1) that may involve also the derivatives φ ,µ of the scalar field, and even nonlinear dependence upon the metric through the kinetic term X = −g µν φ ,µ φ ,ν /2. Their extended range of phenomenology [5][6][7][8][9][10][11][12][13] and universality in scalar-tensor theories [14][15][16][17][18] have made disformal transformations rather popular in cosmology and modified gravity in recent years [19][20][21][22][23][24] (whilst they have also found novel applications in theory [25][26][27][28][29]).…”