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β€ŽMaxwellsOperator.htmlβ€Ž

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<p>$$e^{\tau \partial_a}e^{\epsilon \partial_{b}} \stackrel{?}{=}
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e^{\tau \partial_a+\epsilon \partial_{b}} $$</p>
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<p>This is true when $\tau$ and $\epsilon$ are small, but small compared to what? Compared to the curvature. This is what we are assuming by a <em>linear</em> vector manifold. One way to measure curvature, would be to move along $a$ then $b$, then back along $-a$ <em>then</em> $-b$. Basically reverse your steps in a different order to get back to the start.<br>
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$$\Delta f
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= e^{-\tau \partial_a}e^{-\epsilon \partial_b}e^{\tau \partial_a}e^{\epsilon \partial_b}f -f
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=( e^{-\tau \partial_a}e^{-\epsilon \partial_b}e^{\tau \partial_a}e^{\epsilon \partial_b}-1)f
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= (R\tilde{R} -1)f $$
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Another method is to compare the difference in $f$ at some nearby point, going either way .</br></p>
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<p>$$\Delta f
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= e^{\tau \partial_a}e^{\epsilon \partial_b}f -e^{\epsilon \partial_b}e^{\tau \partial_a}f
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= (R -\tilde R )f
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$$
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Lets see if we can re-work this in terms of conjugation, because conjugation is dank.
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\begin{align*}
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\Delta f &amp;= e^{-\tau \partial_a}e^{-\epsilon \partial_b}e^{\tau \partial_a}e^{\epsilon \partial_b}f -f\\
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&amp;=( e^{-\tau \partial_a}e^{-\epsilon \partial_b}e^{\tau \partial_a}e^{\epsilon \partial_b}-1)f\\
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&amp;= (R\tilde{R} -1)f \\
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\end{align*}</br></p>
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<p>Another method is to compare the difference in $f$ at some nearby point, going either way .</p>
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<p>\begin{align*}
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\Delta f &amp;= e^{\tau \partial_a}e^{\epsilon \partial_b}f -e^{\epsilon \partial_b}e^{\tau \partial_a}f \\
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&amp;= (R -\tilde R )f
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\end{align*}</p>
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<p>Lets see if we can re-work this in terms of conjugation, because conjugation is dank.
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$$ e^{\tau \partial_a}e^{\epsilon \partial_b} fe^{\tilde{\epsilon \partial_b}}e^{\tilde{\tau \partial_a}}
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=f(x+\tau a +\epsilon b -\epsilon b -\tau a ) =f(x) $$
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which is a dumb thing to write when we are in a linear space.</p>
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β€ŽOperatorClass.htmlβ€Ž

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<pre>(3.78 + 5.89e-08 πžβ‚€β‚ + 5.16e-09 πžβ‚€β‚‚ + 3.78e-08 πžβ‚€β‚ƒ + -9.25e-10 πžβ‚β‚‚ + -9.34e-08 πžβ‚β‚ƒ + -6.92e-09 πžβ‚‚β‚ƒ + 2.41e-25 πžβ‚€β‚β‚‚β‚ƒ,
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3.78 + 5.89e-08 πžβ‚€β‚ + 5.16e-09 πžβ‚€β‚‚ + 3.78e-08 πžβ‚€β‚ƒ + -9.25e-10 πžβ‚β‚‚ + -9.34e-08 πžβ‚β‚ƒ + -6.92e-09 πžβ‚‚β‚ƒ + 2.41e-25 πžβ‚€β‚β‚‚β‚ƒ,
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3.78 + 1.5e-07 πžβ‚€β‚ + 5.17e-09 πžβ‚€β‚‚ + 4.1e-08 πžβ‚€β‚ƒ + -9.68e-09 πžβ‚β‚‚ + -1.82e-07 πžβ‚β‚ƒ + -7.02e-09 πžβ‚‚β‚ƒ + 2.12e-24 πžβ‚€β‚β‚‚β‚ƒ)</pre>
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<pre>(5.2 + 2.75e-08 πžβ‚€β‚ + 1.79e-08 πžβ‚€β‚‚ + 4.84e-08 πžβ‚€β‚ƒ + 1.09e-08 πžβ‚β‚‚ + -1.56e-09 πžβ‚β‚ƒ + -6.99e-09 πžβ‚‚β‚ƒ + 1.54e-24 πžβ‚€β‚β‚‚β‚ƒ,
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5.2 + 2.75e-08 πžβ‚€β‚ + 1.79e-08 πžβ‚€β‚‚ + 4.84e-08 πžβ‚€β‚ƒ + 1.09e-08 πžβ‚β‚‚ + -1.56e-09 πžβ‚β‚ƒ + -6.99e-09 πžβ‚‚β‚ƒ + 1.54e-24 πžβ‚€β‚β‚‚β‚ƒ,
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5.2 + 4.93e-08 πžβ‚€β‚ + 4.95e-08 πžβ‚€β‚‚ + 1.05e-07 πžβ‚€β‚ƒ + 2.71e-09 πžβ‚β‚‚ + -2.76e-08 πžβ‚β‚ƒ + 4.55e-08 πžβ‚‚β‚ƒ + 4.62e-24 πžβ‚€β‚β‚‚β‚ƒ)</pre>
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<pre>3.33e+02 + 1.81e+02 πžβ‚€β‚ + 0.00344 πžβ‚€β‚‚ + 6.32 πžβ‚€β‚ƒ + -17.5 πžβ‚β‚‚ + -1.78e+02 πžβ‚β‚ƒ + -0.194 πžβ‚‚β‚ƒ + 3.76e-15 πžβ‚€β‚β‚‚β‚ƒ</pre>
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<pre>1.22e+03 + 43.5 πžβ‚€β‚ + 63.1 πžβ‚€β‚‚ + 1.12e+02 πžβ‚€β‚ƒ + -16.4 πžβ‚β‚‚ + -52.1 πžβ‚β‚ƒ + 1.05e+02 πžβ‚‚β‚ƒ + 6.16e-15 πžβ‚€β‚β‚‚β‚ƒ</pre>
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