
A solar cell (also known as a photovoltaic cell or PV cell) is defined as an electrical device that converts light energy into electrical energy through the photovoltaic effect. A solar cell is basically a p-n junction diode. Solar cells are a form of photoelectric cell, defined as a device whose electrical characteristics –. . A solar cell functions similarly to a junction diode, but its construction differs slightly from typical p-n junction diodes. A very thin layer of p-type. . When light photons reach the p-n junctionthrough the thin p-type layer, they supply enough energy to create multiple electron-hole pairs,. [pdf]

By the 1960s solar power was the standard for powering space-bound satellites. In the early 1970s, solar cell technology became cheaper and more available ($20/watt). Between 1970 and 1990, solar power became more commercially operated. Railroad crossings, oil rigs, space stations, microwave towers, aircraft, etc. Now, houses and businesses all over the world use solar cells to power electrical devices with a wide variety of uses. Solar power is the dominant technol. [pdf]
Photovoltaic (PV) cells are popularly considered a feasible device for solar energy conversion. However, the temperature on the surface of a working solar cells can be high, which significantly decreases the power conversion efficiency and seriously reduces the cell life.
A photovoltaic (PV) plant allows for the transformation of solar radiation into the electrical energy, and this conversion takes place through a so-called semiconductor devices termed as PV cells. Nowadays the most used semiconductor material is silicon, which can be monocrystalline, polycrystalline, or amorphous.
However, the temperature on the surface of a working solar cells can be high, which significantly decreases the power conversion efficiency and seriously reduces the cell life. Therefore, developing novel technologies to solve thermal issues for photovoltaic power systems is necessary.
Thermophotovoltaics is the photovoltaic approach most directly associated with thermal conversion (Fig. 7a). Emission from the heated receiver is confined to a narrow bandwidth, through filtering for example, and directed to a cell.
Solar energy conversion describes technologies devoted to the transformation of solar energy to other (useful) forms of energy, including electricity, fuel, and heat.
Solar energy conversion has the potential to be a very cost-effective technology. It is cheaper as compared to non-conventional energy sources. The use of solar energy help to increase employment and development of the transportation & agriculture sector.

In , the radiative efficiency limit (also known as the detailed balance limit, Shockley–Queisser limit, Shockley Queisser Efficiency Limit or SQ Limit) is the maximum theoretical using a single to collect power from the cell where the only loss mechanism is radiative recombination in the solar cell. It was first calculated by and This required amount of energy to excite an electron is defined as band gap. Band gap is an intrinsic property of semiconductors and eventually has a direct influence on the photovoltaic cell voltage. [pdf]
The band gap represents the minimum energy required to excite an electron in a semiconductor to a higher energy state. Only photons with energy greater than or equal to a material's band gap can be absorbed. A solar cell delivers power, the product of current and voltage.
At the same time, if the band gap of the PV material is too small compared to the incident photon energy, a significant amount of energy will be converted to heat, which is not a good thing for PV cell itself. No matter how much higher the photon energy is compared to the band gap, only one electron can be freed by one photon.
No matter how much higher the photon energy is compared to the band gap, only one electron can be freed by one photon. This is the reason for the limited efficiency of the photovoltaic cells. The data in Figure 4.2 show how the maximum efficiency of a solar cell depends on the band gap.
The ideal photovoltaic material has a band gap in the range 1–1.8 eV. Once what to look for has been estab-lished (a suitable band gap in this case), the next step is to determine where to look for it. Starting from a blank canvas of the periodic table goes beyond the limitations of present human and computational processing power.
If one were to choose a single parameter to perform a first screen to determine a material’s promise in photovoltaics, it would be its band gap. The band gap represents the minimum energy required to excite an electron in a semiconductor to a higher energy state.
Only photons with energy greater than or equal to a material’s band gap can be absorbed. A solar cell delivers power, the product of cur-rent and voltage. Larger band gaps produce higher maximum achievable voltages, but at the cost of reduced sunlight absorption and therefore reduced current.
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