A major challenge in GaN based solar cell design is the lack of holes compared with electrons in the multiple quantum wells (MQWs). We find that GaN based MQW photovoltaic devices with five different Mg-doping concentrations of 0 cm -3 , 5×10 17 cm -3 , 2×10 18 cm -3 , 4×10 18 cm -3 and 7×10 18 cm -3 in GaN barriers can lead to different hole concentrations in quantum wells (QWs). However, when the Mg-doping concentration is over 1×10 18 cm -3 , the crystal quality degrades, which results in the reduction of the external quantum efficiency (EQE), short circuit current density and open circuit voltage. As a result, the sample with a slight Mg-doping concentration of 5×10 17 cm -3 exhibits the highest conversion efficiency.Nowadays, InGaN ternary alloys have drawn great attention in the field of optoelectronics due to their unique physical characteristics, including excellent radiation resistance, good thermal conductivity, large absorption coefficients (~10 5 cm -1 ) [1] and wide band gap (varying from 0.64 eV to 3.4 eV) covering most of the solar spectrum [2][3][4][5][6][7] , which makes them suitable for producing solar cells.Until now, there are several difficulties in the fabrication of InGaN based solar cells with high efficiency. Firstly, the hole mobility in the InGaN material is about 10 cm 2 /(V·s), but the electron mobility in the InGaN material is about 100 cm 2 /(V·s), so there is relatively large lack of holes in InGaN based optoelectronic devices. Secondly, InGaN layers with higher indium (In) proportion are needed to fabricate InGaN-based multijunction solar cells with nearly ideal band gaps for maximum solar energy conversion efficiency. The earlier theoretical calculation indicated that an active material system with power conversion efficiency greater than 50% could be achieved by InGaN alloys with In proportion of about 40% [5] . Unfortunately, the fabrication of solar cells with large In proportion remains a challenge, because of the large lattice mismatch between indium nitride and gallium nitride. When the layer thickness and/or In proportion of InGaN alloys increase, In clusters in InGaN films easily lead to phase separation, which results in the lower open circuit voltages (V oc ) compared with theoretical values, the low fill factors (FFs) and degradation of the short-circuit current density (J sc ) [6][7][8][9][10] .To partially overcome the In incorporation limitation in thick layers, many researchers have adopted multiple quantum wells (MQWs) or superlattice absorbing layers [11][12][13] . InGaN based MQW optical devices can not only obtain higher crystal quality of InGaN absorption layers embedded between GaN barriers, but also optimize V oc and J sc independently by adjusting parameters of quantum barrier and well materials [14] . However, up to now, the energy harvesting efficiency of these devices is not comparable to the theoretical value of devices with a corresponding In mole fraction. To improve the performance of InGaN-based photovoltaic device, it is urgent to implement the in...