Abstract
Power dissipation in a p−n + Si solar cell has been monitored using the electroacoustic technique. Experimental results are described by a vector model which takes into account the different physical locations of the several heat-generating or heat-consuming processes. Analysis of experimental data based on this model allows separation of the different contributions to the power dissipated in the cell and a direct insight into the power loss mechanisms in the device.
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Abbreviations
- D th :
-
thermal diffusion coefficient of the sample
- EA:
-
electroacoustic
- E gap :
-
energy of the gap of the semiconductor
- hv :
-
energy of the incident light
- i dark :
-
cell current density in the dark
- i 0 :
-
saturation current density of the device
- l :
-
sample thickness
- n :
-
quality factor of the device
- P :
-
total power dissipated in the cell in PA experiments
- PA:
-
photoacoustic
- P dark :
-
total power dissipated in the solar cell in the dark in EA experiments
- P fs, inj, P bs, inj :
-
cooling of front and back surface of the cell by injected carriers
- P fs, photo, P bs, photo :
-
heating of front and back surface of the cell by photogenerated carriers
- P inj :
-
power dissipated in the recombination of injected carriers
- P jc :
-
power absorbed in the junction cooling process
- P light :
-
total power dissipated in the illuminated solar cell in EA experiments
- P photo :
-
power dissipated by photogenerated carriers when drifting along the potential slope
- P therm :
-
power dissipated by thermalization of photocarriers in the conduction band
- V :
-
amplitude of the modulated potential applied to the cell
- α, β:
-
phase angles between vector contributions to the total dissipated power in the cell
- ΔE c, ΔE v :
-
energy difference between the quasi-Fermi levels of the n(p) semiconductor and the bottom (top) of the conduction (valence) band
- μth=(2D th/ω)1/2 :
-
thermal diffusion length of the sample
- Φd :
-
phase of EA signal in the dark
- Φ1 :
-
phase of EA signal with light
- ω:
-
frequency of the modulated voltage applied to the cell.
References
A. Fujishima, G.H. Brilmyer, A.J. Bard: Proc. Electrochem. Soc. 77, 172 (1977)
D. Cahen, P.-E. Nordal, S.O. Kanstad: Appl. Phys. Lett. 49, 1351 (1986)
H. Koinuma, K. Hashimoto, K. Fueki: In Conf. Rec. 18th IEEE Photovolt. Spec. Conf. (1985) p. 1683
Y. Mishima, M. Hirose, I. Suemune, M. Yamanishi, Y. Osaka: J. Phys. 42, (Suppl.), C4–447 (1981)
R.E. Wagner, A. Mandelis: Phys. Rev. B 38, 9920 (1988)
J. Rappich, J.K. Dohrmann: In Photoacoustic and Photothermal Phenomena, ed. by P. Hess, J. Pelzl, Springer Ser. Opt. Sci. Vol. 58 (Springer, Berlin, Heidelberg 1988) p. 204
J. Rappich, J.K. Dohrmann: Ber. Bunsenges. Phys. Chem. 92, 1342 (1988)
A. Rosencwaig, A. Gersho: J. Appl. Phys. 47, 64 (1976)
M. Wolf, D. Cahen: Solar Cells 27, 247 (1989)
I.F. Faria, C.C. Ghizoni, L.C.M. Miranda, H. Vargas: J. Appl. Phys. 59, 3294 (1986)
H.L. Riete, L.C.M. Miranda, H. Vargas: Appl. Phys. A 44, 219 (1987)
S.M.N. Mello, C.C. Ghizoni, L.C.M. Miranda, H. Vargas: J. Appl. Phys. 61, 5176 (1987)
M. Wolf: Energy Convers. 11, 63 (1971)
D. Cahen, H. Flaisher, M. Wolf: In Photoacoustic and Photothermal Phenomena, ed. by P. Hess, J. Pelzl, Springer Ser. Opt. Sci. Vol. 58 (Springer, Berlin, Heidelberg 1988) p. 247
W. Thielemann, B. Rheinländer: Solid State Electron. 28, 1111 (1985)
H. Flaisher, M. Wolf, D. Cahen: J. Appl. Phys. 66, 1832 (1989)
B. Büchner, M. Wolf, D. Cahen: Mater. Sci. Eng. A 122, 127 (1989)
D. Cahen, B. Büchner, F. Decker, M. Wolf: IEEE Trans. ED-37, 498 (1990)
H. Flaisher, D. Cahen, M. Wolf: IEEE Trans. ED-34, 457 (1987)
B. Büchner, H. Flaisher, M. Wolf, D. Cahen: Conf. Rec. 20th IEEE Photovolt. Spec. Conf. (1988) p. 1452
B. Büchner, H. Flaisher, M. Wolf, D. Cahen: J. Appl. Phys. 67, 4338 (1990)