absorption coefficients of semiconductor thin...

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PHYS 4580, PHYS 6/7280 The University of Toledo Profs. R. Ellingson and M. Heben Absorption coefficients of semiconductor thin films October 8, 2013

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  • PHYS 4580, PHYS 6/7280 The University of Toledo

    Profs. R. Ellingson and M. Heben

    Absorption coefficients of semiconductor thin films

    October 8, 2013

  • Typical Si PV Cell Structure

    Real Space Schematic

    Energy Band Diagram

    Total Device Thickness:

    a few hundred microns

    Optical absorption

  • Typical Thin Film (CIGS) Cell Structure

    Total Device Thickness:

    a few microns

  • Total Incident (λ) = A(λ) + T(λ)+ R(λ)

    Conservation of Energy for each wavelength

    Why must some PV layers be so thick?

    (want to maximize absorption)

  • Mechanisms of Optical Absorption

    • Energy is absorbed by a “system”,

    potential energy of system is

    increased.

    • For a system in which we are

    concerned with gravitational potential

    energy, consider the energy required

    to put put a book on a shelf.

    • For semiconductors, optical

    absorption occurs any time a

    “carrier” can be excited to a higher

    “state”.

    • Typically, the carriers we are

    concerned with are electrons, and

    the excitation is across the band gap.

  • Absorption coefficient

    α (λ) - the absorption coefficient

    ni (λ) - density of carriers in an initial state

    nf (λ) - density of unoccupied states

    Pif(λ) - probability that transition will take place

    In addition to “band gap excitation”, another important

    absorption process is “free carrier absorption”, which is

    typically seen in metals and TCOs.

    (a connection between the optical and electronic

    properties of materials)

  • Types of Semiconductor Band Gaps

    Valence Band Valence Band

    Conduction

    Band Conduction

    Band

    Energ

    y

    Momentum Momentum

    Energ

    y

    Indirect Band Gap Direct Band Gap

    • A direct transition requires just a photon of sufficient energy

    • An indirect transition require both a photon and a phonon

    “two body event” is lower probability.

    • Energy and Momentum must be conserved.

    Direct

    transition Indirect

    transition

  • Density of States in 3D Crystal • “States” – allowed solutions to the Shrodinger Equation

    • Analogy to waves on a string, but in 3 dimensions

    http://hyperphysics.phy-astr.gsu.edu/hbase/waves/string.html

    Density of States

    Units of: # per energy-volume

    Energy

    DO

    S

  • DOS

    Energy

    hv Eg

    nf

    ni

  • Absorption Coefficients for some Semiconductors

  • 95% Absorption Depth (CdTe)

  • Beer-Lambert Law

    Itotal (λ) I (λ)

    X

  • Detecto

    r

    R

    T

    Calculation of the absorption coefficient, α(λ), for a thin film

    A + R + T = 1

    total

    t

    I

    IT

    Itotal

    dt eII

    0 RII total 10

    dtotalt eRII 1

    Since It = (T)(Itotal) (T)(Itotal) = (1-R)(Itotal)e-α(λ)d

    R

    Td

    R

    Te d

    1ln

    1

    d

    R

    T

    1

    ln

  • Reproduced From “Optical Processes in Semiconductors”, Pankove