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MyWikiBiz, Author Your Legacy — Wednesday May 01, 2024
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We are going to consider various ''operators'' on these functions.  Here, an operator <math>\operatorname{F}</math> is a function that takes one function <math>f\!</math> into another function <math>\operatorname{F}f.</math>
 
We are going to consider various ''operators'' on these functions.  Here, an operator <math>\operatorname{F}</math> is a function that takes one function <math>f\!</math> into another function <math>\operatorname{F}f.</math>
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<pre>
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The first couple of operators that we need to consider are logical analogues of those that occur in the classical ''finite difference calculus'', namely:
The first couple of operators that we need to consider are logical analogues
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of those that occur in the classical "finite difference calculus", namely:
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{| align="center" cellpadding="6" width="90%"
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| The ''difference operator'' <math>\Delta,\!</math> written here as <math>\operatorname{D}.</math>
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|-
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| The ''enlargement" operator'' <math>\Epsilon,\!</math> written here as <math>\operatorname{E}.</math>
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|}
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1.  The "difference" operator [capital Delta], written here as D.
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These days, <math>\operatorname{E}</math> is more often called the ''shift operator''.
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2.  The "enlargement" operator [capital Epsilon], written here as E.
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In order to describe the universe in which these operators operate, it is necessary to enlarge the original universe of discourse, passing from the space <math>U = X \times Y</math> to its ''differential extension'', <math>\operatorname{E}U,</math> that has the following description:
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These days, E is more often called the "shift" operator.
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{| align="center" cellpadding="6" width="90%"
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| <math>\operatorname{E}U ~=~ U \times \operatorname{d}U ~=~ X \times Y \times \operatorname{d}X \times \operatorname{d}Y,</math>
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|-
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| with
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|-
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| <math>\operatorname{d}X = \{ \texttt{(} \operatorname{d}x \texttt{)}, \operatorname{d}x \}</math> &nbsp;and&nbsp; <math>\operatorname{d}Y = \{ \texttt{(} \operatorname{d}y \texttt{)}, \operatorname{d}y \}.</math>
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|}
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In order to describe the universe in which these operators operate,
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<pre>
it will be necessary to enlarge our original universe of discourse.
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We mount up from the space U = X x Y to its "differential extension",
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EU = U x dU = X x Y x dX x dY, with dX = {(dx), dx} and dY = {(dy), dy}.
   
The interpretations of these new symbols can be diverse, but the easiest
 
The interpretations of these new symbols can be diverse, but the easiest
 
for now is just to say that dx means "change x" and dy means "change y".
 
for now is just to say that dx means "change x" and dy means "change y".
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