Delta Functions and Convolutions

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    Some additional math concepts

    Complex numbers

    The complex number a + ib should be viewed simply as the point in the xy-

    plane having Cartesian coordinates (a, b), or equivalently as the vector

    connecting the origin to that point.

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    Eulers formula:

    Important relations:

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    1It follows that 1 if n is integer

    Then: if n is integer

    1 1

    0

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    Let us recall the scalar product, of two vectors, one of the direct lattice, one of the

    reciprocal lattice:

    X

    X = integer number

    1

    Then:

    This property will be extremely useful in the future

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    The Dirac delta function

    The Dirac delta function is defi

    ned by theproperties:

    0 for 0

    for 0and

    1

    Area under the box=1

    x=0

    a

    1/a

    The delta function as a limit of box function

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    The delta function as a limit of a gaussian function

    1 2

    x

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    The Dirac delta function in 2D...

    x=0

    x=x0x=0

    0 for for

    The Dirac delta function in 3D...

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    Lattice functions

    where and is an integer

    Delta functions can be used to represent lattice functions. For example, in a

    one-dimensional space, a lattice with period a may be represented by:

    vanishes everywhere except at the lattice points where it becomes infinite

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    Lattice functions

    ,,

    ,,

    By the same fashion, a three-dimensional lattice defined by the basis vectorsa, b and c may be represented by:

    vanishes everywhere except at the lattice points where it becomes infinite

    Where

    ,, and u, v, w are integers

    ,,

    ,,

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    Convolutions

    A convolution between two functions and is denoted by and is defined by:

    A convolution is in essence an integral that expresses the amount of

    overlap of one function as it is shifted over another function. It

    therefore "blends" one function with another.

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    One example of convolution

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    Another example of convolution

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    Other examples of convolution

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    Convolutions with delta functions

    1. Flip :

    0

    0

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    Convolutions with delta functions

    2. Translate by :

    0

    0

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    Convolutions with delta functions

    3. Move from left toright ( runs from to +)

    0

    0

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    Convolutions with delta functions

    3. Move from left toright ( runs from to +)

    0

    0

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    Convolutions with delta functions

    3. Move from left toright ( runs from to +)

    0

    0

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    Convolutions with delta functions

    0

    0

    4. At some point starts overlapping with

    Because is infinetly narrow at , and the area under is equal to 1, in theonly point of overlap, the area under is equal to

    starts appearing

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    Convolutions with delta functions

    0

    0

    The area under is always equal to

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    Convolutions with delta functions

    0

    0

    The area under is always equal to

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    Convolutions with delta functions

    0

    0

    The area under is always equal to

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    Convolutions with delta functions

    0

    0

    The area under is always equal to

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    Convolutions with delta functions

    0

    0

    We are clearly flipping horizontally as advances and thefunction is filtered through

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    Convolutions with delta functions

    0

    0

    We are clearly flipping horizontally as advances and thefunction is filtered through

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    Convolutions with delta functions

    0

    0

    We are clearly flipping horizontally as advances and thefunction is filtered through

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    Convolutions with delta functions

    0

    0

    We are clearly flipping horizontally as advances and thefunction is filtered through

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    Convolutions with delta functions

    0

    0

    We are clearly flipping horizontally as advances and thefunction is filtered through

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    Summarizing:

    The convolution of with has the effect of translating from theorigin to

    0

    0

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    Convolutions

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    We come now to an important conclusion:

    A crystal can be described mathematically as the convolution of a function which describes the content of the unit cell (for example the electronic density

    distribution) with the lattice function

    ,,

    ,,