From some field investigations (like Lake Constance and Lake Mead), the shape of a delta is not a Gilbert delta. Slope evolution between foreset and bottomset is not sharp but smooth. Delta foresets are not straight but curved. The appearances of turbidity currents were also observed. Turbidity currents are the subaqueous part of hyperpycnal flows. Hyperpycnal flows appear when a sediment loaded river flows into a lake (or a reservoir). The motion of these density currents leads the depositions at lake shore to form hyperpycnal deltas. Similar to the Gilbert delta, hyperpycnal deltas grow up in self-similar forms. In the thesis, some laboratory experiments were done to explore the processes of hyperpycnal deltas. Two-diffusion description with inclination thresholds were used to model those processes. Self-similar analytical solutions for hyperpycnal deltas were also solved to compare to other known analytical solutions of Gilbert deltas. Finally, experimental data, theory and numerical model were compared to each other.