les 1 struct operat solar cell

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    F.SpertinoF.Spertino

    STRUCTURE ANDOPERATION

    F. Spertino

    .

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    BACKGROUND ON SEMICONDUCTORS

    The solar or photovoltaic (PV) cell is

    the basic element of the PV systems, Si

    sunlight into electricity occurs inside.

    The conversion efficienc is achieved

    by exploiting the properties ofsemiconductors. In Silicon (Si) the

    4 valence electrons, available for

    chemical bonding with surroundingatoms.

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    BACKGROUND ON SEMICONDUCTORS

    To understand the conversion process, it is advisable toremember some h sical remarks: the ener bandstructure of the atom and the generation of electron-

    hole couples. The energy band is the set of energy levels owned by

    the electron. It is composed of:

    - valence band, that is composed of electron set involvedin chemical bonding;

    - con uc on an , a s compose o e ec rons w anenergy level (higher than the previous) to permit their

    - band gap (energy gap), which represents the energy

    band to the conduction band.

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    BACKGROUND ON SEMICONDUCTORS

    Insulators

    Conduction band

    ConductorsSemiconductors

    EcConduction band

    Ec

    E

    Ec

    Eg

    Valence bandEv

    gValence band

    Valence band

    Ev

    Crystalline Silicon (c-Si) 1,12

    -

    nergy gap e o ma or sem con uc ors

    ,

    Germanium (Ge) 0,67

    Gallium Arsenide (GaAs) 1,42

    Indium Phosphide (InP) 1,34

    Copper Indium Diselenide (CuInSe) 1,05

    Cadmium Telluride (CdTe) 1,45

    Cadmium Sulfide (CdS) 2,4

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    BACKGROUND ON SEMICONDUCTORS

    In order to obtain the diodeSihole

    have to realize the P-N junction in a

    semiconductor, putting together two B SiSicrystals: one is "doped" withtrivalent atoms (boron) and the

    r w vatoms (phosphorus).Si electron

    -atoms and holes in the lattice, while

    the N-t e cr stal has free electrons P Sifrom the bond.

    Holes and electrons move freely in

    the lattice due to diffusion.

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    THE PHOTOVOLTAIC EFFECT

    At the interface, electrons of the N-type crystal spread to theP-type crystal (vice versa for holes), forming a space charge

    region ("+" on N-type and "-" on the P-type), in which there.

    When the electric field generated counter-balances the, .

    The radiation, with sufficient energy (Eph= hf = hc/> Eg),

    In the presence of the junction electric field, electrons are

    attracted to the N area ositivel char ed and holes to theP area (negatively charged).

    This charge motion is the source of the photovoltaic current.

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    THE PHOTOVOLTAIC EFFECT

    In a single-junction cell, the doped N layer is placed abovethe P layer in a thickness ranging from 200 to 300 m.

    Junction

    field1V/m

    The radiation is able to reach the junction (depletion region)because the N layer is very thin (1m).

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    THE PHOTOVOLTAIC EFFECT

    In the solar spectrum, onlyp o ons w su c en

    energy are able to generate- .

    Photons (visible and above

    surplus of energy that is lostin the creation of electron/hole pairs: itimplies a limit in the

    .

    Limits conversion for Silicon

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    THE PHOTOVOLTAIC EFFECT

    Additional disadvantages are:

    not all incident photons penetrate into the, r r rvanished by the frontal electrode;

    some electron-hole pairs recombinetheirselves before they can be separatedby the electric field inside the junction;

    the frontal electrode of the cell has anamount of resistance.

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    THE PHOTOVOLTAIC EFFECT

    N layer There are also other types of junction...

    Electric

    N layer

    insic

    Electric

    field intr

    fieldEg2

    g

    P-N junction

    Eg

    P-I-N junction

    Eg1

    Hetero- unction

    Note the different erformance of the field in the unction

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    THE PHOTOVOLTAIC EFFECT

    Look at energy bands of a P-N junction with forward or

    IforrevNote that the

    direction of current

    - + the flow of positiveorwar as

    (+ on the P layer)

    -

    Reverse bias

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    thus the diffusion current in the diode is growing

    considerably

    The reverse bias increases the potential barrier: asmall reverse saturation current runs

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    THE STRUCTURE OF THE SOLAR CELL

    The material of widespread PV cells is

    single- and multi- (orpo y- crysta ine si icon.

    Each cell is obtained by aw r thickness and 10 20 cm

    On the frontal side (often

    "textured" a la er ofantireflective coating isapplied.

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    THE STRUCTURE OF THE SOLAR CELL

    -from the sawing of a round cylinder

    in ot wafer .

    Poly-crystalline cells are derived fromthe fusion and solidification of Silicon

    in a quartz crucible (square ingot). On the back side (P-type) it is applied

    a contact as arge as t e sur ace othe cell.

    r - ycontact is formed by thin Ag

    .