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creation of charge carriers (e-h pairs) within the PV device, and
(c) separation of (e-h) pairs before their recombination — in
order to (d) pass through an external circuit to create useful
power.Toachievethesefourfunctionssimultaneously,anelectronic
device containing a suitable interface with a built-in electric field
is necessary. Such an interface can be an MS Schottky contact, a
p-n homo-junction, a p-n hetero-junction, an n-n hetero-junction,
or a p-p hetero-junction. MS and p-n junctions can be further
modified to form MIS and p-i-n junctions respectively to enhance
theirperformance.Toproduceane cientPVsolarcell,twoormore
interfaces mentioned above can be combined to form one solar cell
structure. The graded bandgap multi-layer solar cell structures are
thewayforwardtoimprovingsolarenergyconversioninthefuture.
References
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Rinehart and Winston.
4. J. N. Lalena and D. A. Clearly (2005) Principles of Inorganic Materials
Design , JohnWiley & Sons.
5. C.Kittel(2005) Introduction to Solid State Physics, 8thedn,JohnWiley&
Sons.
6. J. S. Blakemore (1974) Solid State Physics , 2nd edn, W. B. Saunders
Company.
7. N. W. Ashcroft and N. D. Mermin (1976) Solid State Physics , Cengage
Learning.
8. C. N. R. Rao and J. Gopalakrishnan (1997) New Directions in Solid State
Chemistry , 2nd edn, Cambridge University Press.
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3rd edn, Taylor &Francis Group.
10. S. M. Sze and K. K. Ng (2007) Physics of Semiconductor Devices , John
Wiley & Sons.
11. J. Singh (2001) Semiconductor Devices: Basic Principles , John Wiley &
Sons.
 
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