Uniform Thin Film Deposition

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    Thermal Vapor Deposition

    How to obtain a thin film of uniform thickness

    over a substrate of considerable size

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    Thermal Vapor Deposition

    A basic technique for thin film deposition over a

    substrate.

    Source material is heated in high vaccum.

    The evaporated atoms get impinged over the substratesurface.

    The evaporation rate is given by:

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    Film Thickness and Uniformity

    Uniform film thickness is essential in case of

    microelectronics - integrated circuits, optical

    coatings.

    Accuracy of about 1% is required.

    Understanding deposition geometry is important.

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    Deposition Geometry

    Characteristics of the source and orientation &

    placement of the substrate.

    Consider evaporation from a point source.

    Total evaporated mass:

    Mass deposition (substrate):

    Deposition depends on:

    geometric orientation ().

    source-substrate distance.

    dAc = dAscos

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    Deposition Geometry

    Similarly for a surface source, we have the following

    expression:

    Deposition rate depends upon:

    Source-substrate distance

    Emission angle and orientation ( and )

    and are equal if both surfaces are parallel

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    Uniform Thickness

    Difficulties arise while dealing with substrates having a

    large surface area or curved surface

    Consider evaporation from a point source to a planar

    substrate.

    The film thickness d =

    Thickest deposit (d0) occurs at l = 0.

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    Similarly, for the surface source:

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    We can utilize the film thickness distribution to design

    source-substrate geometries for coating.

    Example 1 : Coating of 150cm wide substrate using two

    point sources. Tolerance: 10%

    Parameters: Distance of sources from the centre line (D) and the

    distance between source and substrate (hv)

    A superposition of the solution for individual sources can provide

    the graphical variation of thickness as a function of D and h Range for d/d0 is between 0.9 and 1.1

    D/hv = 0.6 is optimum, maximum allowed value of r/hv = 0.87

    Since r = 150/2 = 75cm, hv = 75/0.87 = 86.2 cm

    Further, distance between the sources (2D) = 2x0.6x86.2 =

    103.4 cm

    Other solutions obviously exist, but we are seeking minimum

    value of hv , to minimise waste of evaporant.

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    Example 2 : Composite optical coating where a 1%

    film thickness variation is required in each layer.

    Diameter of substrate = 2r = 25 cm.

    Substrate is rotated to even out source distribution anomalies.

    Necessary fixturing requires that the sources be offset from the

    axis of rotation by a distance R = 20 cm

    How high (hv) should the rotating substrate be placed from the

    source for optimum deposition? Film thckness variation is a complicated function of 3-D

    geometry.

    The graph suggests hv/R = 1.33 in conjunction with r/R = 0.6 is

    suitable. (deviation between -0.6% to +0.5%)

    required distance is hv = 1.33 x 20 = 26.6 cm

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    Another way to acheive thickness uniformity is to haveboth the surface source and substrate on the surface ofa sphere as shown:

    We Have:

    Mass deposited is constant.

    There are limitations.

    Other methods:

    Varying the location of source

    Use of shutters

    Controlled by a computer

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    References:

    Milton Ohring, Materials Science of Thin Films, 2ndedition, Academic Press, (1992).