access icon free Enhancing the efficiency of the intermediate band solar cells by introducing: carrier losses, alloying and strain

A detailed balance model is used to determine the efficiency of intermediate band solar cell including carrier losses from the intermediate band. The effect of the energy gap of the host semiconductor is examined as a function of the intermediate band position in the energy gap and the host semiconductor energy gap. Generally the optimal intermediate band level decreases within the energy gap to mitigate the carrier losses, and carrier losses are less detrimental to small energy gap materials. We therefore focus on the role of carrier losses in wide bandgap semiconductor intermediate band solar cell systems, such as the GaN semiconductor with an Mn impurity band. Experimentally Mn acceptor level in the GaN energy gap is 1.8 eV above the valence band, which is 199 meV off the ideal intermediate band and reduces the efficiency to 21.36%. We demonstrate how carrier losses can be introduced into the system to shift the optimum IB position. Introducing carrier losses shifts the optimal intermediate band position to 1.8 eV above the valence band and increases the efficiency to 23.41%. We compare this to the effect of alloying GaN and introducing biaxial strain to shift the effective position of the Mn impurity band on the efficiency.

Inspec keywords: manganese; valence bands; blackbody radiation; gallium compounds; solar cells; III-V semiconductors; impurities; energy gap

Other keywords: efficiency 21.36 percent; impurity; wide band gap semiconductor IBSC systems; alloying; electron volt energy 1.8 eV; biaxial strain; efficiency 23.41 percent; GaN; carrier losses; blackbody radiation function; Mn; electron volt energy 199 meV; energy gap; intermediate band solar cells; valence band

Subjects: Electronic structure of crystalline semiconductor compounds and insulators; Surface states, surface band structure, surface electron density of states; Solar cells and arrays; Impurity and defect levels in II-VI and III-V semiconductors; Heat radiation; Photoelectric conversion; solar cells and arrays

References

    1. 1)
      • 8. Vurgaftman, I., Meyer, J.R., Ram-Mohan, L.R.: ‘Band parameters for III–V compound semiconductors and their alloys’, J. Appl. Phys., 2001, 89, (11), pp. 58155875.
    2. 2)
      • 5. Graf, T., Gjukic, M., Brandt, M.S., et al: ‘The Mn(3+/2+) acceptor level in group III nitrides’, Appl. Phys. Lett., 2002, 81, (27), pp. 51595161.
    3. 3)
      • 9. Adams, A.R.: ‘Strained-layer quantum-well lasers’, IEEE J. Sel. Top. Quantum Electron., 2011, 17, (5), pp. 13641373.
    4. 4)
      • 1. Luque, A., Marti, A.: ‘Increasing the efficiency of ideal solar cells by photon induced transitions at intermediate levels’, Phys. Rev. Lett., 1997, 78, (26), pp. 50145017.
    5. 5)
      • 4. Okada, Y., Yoshida, K., Shoji, Y., et al: ‘Recent progress on quantum dot intermediate band solar cells’, IEICE Electron. Express, 2013, 10, (17), p. 20132007.
    6. 6)
      • 2. Wang, Q.-Y., Rorison, J.: ‘Modelling of quantum dot intermediate band solar cells: effect of intermediate band linewidth broadening’, IET Optoelectron., 2014, 8, (2), pp. 8187.
    7. 7)
      • 3. Shockley, W., Queisser, H.J.: ‘Detailed balance limit of efficiency of p-n junction solar cells’, J. Appl. Phys., 1961, 32, (3), pp. 510519.
    8. 8)
      • 7. Pikus, G.E., Bir, G.L.: ‘Effect of deformation on the hole energy spectrum of germanium and silicon’, Sov. Physics-Solid State, 1960, 1, (11), pp. 15021517.
    9. 9)
      • 6. Martí, A., Tablero, C., Antolín, E., et al: ‘Potential of Mn doped In1−xGaxN for implementing intermediate band solar cells’, Sol. Energy Mater. Sol. Cells, 2009, 93, (5), pp. 641644.
http://iet.metastore.ingenta.com/content/journals/10.1049/iet-opt.2016.0056
Loading

Related content

content/journals/10.1049/iet-opt.2016.0056
pub_keyword,iet_inspecKeyword,pub_concept
6
6
Loading