Solar cell based on vacuum separation type p-n junction n-type variable doping GaN-based anode
Technical Field
The invention belongs to the technical field of solar cells, and particularly relates to an n-type GaN-based anode solar cell based on a vacuum separation type p-n junction.
Background
Photovoltaic power generation utilizes the photon effect of short-wave photons of solar radiation to excite electrons in materials so as to realize photoelectric conversion. In 2010, the U.S. Stanford university J.W.Schwede et al proposed a "Photon Enhanced Thermionic Emission (PETE)" solar cell technology, overcoming the disadvantage of the traditional photovoltaic power generation technology that efficiency decreases with increasing temperature, and achieving energy conversion at higher temperatures. The PETE solar cell device adopts a cathode and anode separated structure, the cathode absorbs solar radiation to emit electrons, and the electrons are received by the anode to form current so as to complete photoelectric conversion. The current research on PETE batteries mainly focuses on the photoelectric conversion efficiency of a photocathode, and the research on anodes is limited to phosphorus-doped diamond. The phosphorus-doped diamond anode has the defects of complex manufacturing process, low electron collection efficiency and the like, and the energy conversion efficiency of the solar cell adopting the phosphorus-doped diamond is not high.
Disclosure of Invention
The invention aims to provide a solar cell based on a vacuum separation type p-n junction n-type variable doping GaN-based anode so as to improve the energy conversion efficiency of the solar cell.
The technical scheme for realizing the purpose of the invention is as follows: a solar cell based on a vacuum separation type p-n junction n-type variable doping GaN-based anode comprises a GaAs photocathode, a vacuum cavity and an anode, and is characterized in that the anode is made of a GaN-based material, and a substrate layer, an AlN buffer layer and an n-type variable doping GaN receiving layer are sequentially arranged on the anode from the top layer to the position close to the vacuum cavity.
Preferably, the substrate layer is a sapphire substrate.
Preferably, the AlN buffer layer is grown on the substrate layer to a thickness of 50-75 nm.
Preferably, the n-type variable doping GaN-based receiving layer grows on the AlN buffer layer by MOCVD method, the thickness is 200-300nm, and the doping concentration range is 1 × 1018-1×1019cm3The doping concentration decreases from near the AlN buffer layer to the outermost surface.
Preferably, the n-type variable doping GaN-based receiving layer comprises 4 layers from the position close to the AlN buffer layer to the outermost surface, the thickness of the first layer is 50-75nm, the doping concentration is 1 multiplied by 1019cm-3(ii) a The second layer has a thickness of 50-75nm and a doping concentration of 5 × 1018cm-3(ii) a The thickness of the third layer is 50-75nm, and the doping concentration is 2.5 × 1018cm-3(ii) a The thickness of the fourth layer is 50-75nm, and the doping concentrationIs 1 × 1018cm-3。
Preferably, the surface of the n-type variable doping GaN-based receiving layer is treated by adopting an ultrahigh vacuum activation process.
Compared with the prior art, the invention has the following advantages: 1) the n-type GaN-based material adopts a heavy doping technology to ensure that the Fermi level is close to the bottom of the conduction band; 2) the n-type GaN-based anode structure disclosed by the invention is based on a semiconductor material doping technology and an ultrahigh vacuum surface activation technology, realizes a low electron affinity n-type variable doping GaN-based anode structure, obtains a GaN-based anode structure with low work function, high electron transport efficiency and high electron collection efficiency, and realizes higher energy conversion efficiency of a solar cell; 3) the n-type GaN-based material provided by the invention has a simple preparation process, the work function of the anode is effectively reduced, and the higher energy conversion efficiency of the PETE solar cell is realized; 4) the invention adopts the variable doping technology, and a built-in electric field is formed inside the anode, thereby improving the transport efficiency of electrons inside the anode and inhibiting the noise current of the n-type GaN-based material.
Drawings
FIG. 1 is a schematic structural view of an n-type metamorphic doped GaN-based anode.
Fig. 2 is a graph of energy conversion efficiency for different anode material work functions.
Detailed Description
As shown in figure 1, the n-type variable doping GaN-based anode solar cell based on the vacuum separation type p-n junction comprises a GaAs photocathode, a vacuum cavity and an anode, wherein the anode is made of a GaN-based material, and the anode sequentially comprises a substrate layer 1, an AlN buffer layer 2 and an n-type variable doping GaN receiving layer 3 from the top layer to the position close to the vacuum cavity.
The GaAs photoelectric cathode is connected with the GaN anode by adopting a cylindrical ceramic cavity, sealing treatment is carried out by an indium sealing material, and a vacuum cavity is formed between the GaAs photoelectric cathode and the GaN anode, so that the vacuum separation type p-n junction solar cell is formed.
The substrate layer 1 is a sapphire substrate, and the AlN buffer layer 2 grows on the upper surface of the sapphire substrate in an MOCVD mode and has the thickness of 50-75 nm.
The n-type variable doped GaN-based junctionThe cladding layer 3 is grown on the AlN buffer layer 2 by MOCVD method with a thickness of 200-300nm and a doping concentration range of 1 × 1018-1×1019cm3The doping concentration decreases from near the AlN buffer layer 2 toward the outermost surface.
In some embodiments, the n-type variation doped GaN-based receiving layer 3 includes 4 layers from the vicinity of the AlN buffer layer 2 to the outermost surface, the first layer having a thickness of 50 to 75nm and a doping concentration of 1X 1019cm-3(ii) a The second layer has a thickness of 50-75nm and a doping concentration of 5 × 1018cm-3(ii) a The thickness of the third layer is 50-75nm, and the doping concentration is 2.5 × 1018cm-3(ii) a The thickness of the fourth layer is 50-75nm, and the doping concentration is 1 × 1018cm-3。
And activating the surface of the n-type variable doping GaN receiving layer 3 by utilizing an ultrahigh vacuum activation process to obtain the n-type GaN-based receiving layer 3 with low electron affinity.
Due to the difference of the doping concentration of the GaN-based material, a built-in electric field pointing from outside to inside is formed inside the anode, and the built-in electric field is favorable for improving the transport rate of carriers inside the anode, enhancing the electron collection efficiency of the anode and inhibiting the noise current of the n-type GaN-based material.
The GaN-based anode with low electron affinity is obtained through surface activation treatment, the work function of the GaN-based anode is reduced, the output voltage of the solar cell is increased, and the energy conversion efficiency of the solar cell is improved.
As shown in fig. 2, a schematic diagram of energy conversion efficiency of an n-type variable doped GaN-based anode solar cell based on a vacuum separation type p-n junction under different anode work function conditions is shown, and the energy conversion efficiency is higher as the anode work function is reduced. The n-type variable doped GaN-based anode material provided by the invention is subjected to an ultra-vacuum activation process to obtain the n-type GaN-based receiving layer with low electron affinity, so that the work function of the anode material is reduced, and the energy conversion efficiency of the solar cell is improved.
Examples
A vacuum separation type p-n junction based n-type variable doping GaN-based anode solar cell comprises a GaAs photocathode, a vacuum cavity and an anode, wherein the anode is made of a GaN-based material, and the anode is made of a GaN-based materialThe anode comprises a substrate layer 1, an AlN buffer layer 2 and an n-type variable doping GaN receiving layer 3 from outside to inside in sequence. The substrate layer 1 is a sapphire substrate, the AlN buffer layer 2 grows on the upper surface of the sapphire substrate in an MOCVD mode and has the thickness of 50nm, the n-type variable doping GaN receiving layer 3 grows on the AlN buffer layer 2 in an MOCAD mode and has the thickness of 200nm, the n-type variable doping GaN-based receiving layer 3 comprises 4 layers, the first layer has the thickness of 50nm, the doping concentration is 1 multiplied by 1019cm-3(ii) a The second layer has a thickness of 50nm and a doping concentration of 5 × 1018cm-3(ii) a The thickness of the third layer is 50nm, and the doping concentration is 2.5 multiplied by 1018cm-3(ii) a The thickness of the fourth layer is 50nm, and the doping concentration is 1 multiplied by 1018cm-3。