Inspired by recent remarkable sets of experiments on UTe \(_2\) : discoveries of the fourth horizontal internal transition line running toward a tetra-critical point (TCP) at H = 15 T, the off-axis high-field phases, and abnormally large Knight shift (KS) drop below \(T_\textrm{c}\) for \(H \parallel a\) -magnetic easy axis, we advance further our theoretical work on the field (H)-temperature (T) phase diagram for \(H \parallel b\) -magnetic hard axis which contains a positive sloped \(H_\textrm{c2}\) departing from TCP. A nonunitary spin-triplet pairing with three components explains these experimental facts simultaneously and consistently by assuming that the underlying normal electron system with a narrow bandwidth characteristic to the Kondo temperature \(\sim\) 30 K unsurprisingly breaks the particle-hole symmetry. This causes a special invariant term in Ginzburg–Landau (GL) free energy functional which couples directly with the 5f magnetic system, giving rise to the \(T_\textrm{c}\) splitting and ultimately to the positive sloped \(H_\textrm{c2}\) and the horizontal internal transition line connected to TCP. The large KS drop can be understood in terms of this GL invariance whose coefficient is negative and leads to a diamagnetic response where the Cooper pair spin is antiparallel to the applied field direction. The present scenario also accounts for the observed d-vector rotation phenomena and off-axis phase diagrams with extremely high \(H_\textrm{c2}\) \(\gtrsim\) 70 T found at angles in between the b- and c-axes and between the bc-plane and a-axis, making UTe \(_2\) a fertile playground for a possible topological superconductor.