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Example 1.
Create the jet space J^3(E) for the bundle E = R x R with coordinates (x, u) -> (x).
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Show that the EulerLagrange form for omega1 is 0 so that omega1 is dH exact.
E >
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| (2.1) |
E >
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| (2.2) |
Apply the horizontal homotopy operator to omega1.
E >
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| (2.3) |
Check that the horizontal exterior derivative of eta1 gives omega1.
E >
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| (2.4) |
Example 2.
Show that the integration by parts operator for the type (1, 2) omega2 is 0 so that omega2 is dH exact.
E >
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| (2.5) |
E >
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| (2.6) |
Apply the horizontal homotopy operator to omega2.
E >
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| (2.7) |
Example 3.
Show that the Euler-Lagrange form for omega3 is 0 so that omega3 is dH exact.
E >
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| (2.8) |
E >
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| (2.9) |
E >
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| (2.10) |
Apply the horizontal homotopy operator to omega3. Because omega3 is singular at u[2] = 0 we change the integration limits in the homotopy formula but still perform a radial integration. See HorizontalExteriorDerivative for a detailed discussion.
E >
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| (2.11) |
Check that HorizontalExteriorDerivative of eta3 gives omega3.
E >
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| (2.12) |
Instead of changing the limits of integration we can change the integration path to a sequence of coordinate lines. See HorizontalExteriorDerivative for a detailed discussion.
E >
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| (2.13) |
E >
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| (2.14) |
Example 4.
Create the jet space J^2(E) for the bundle E = R^3 x R^2 with coordinates (x, y, u, v) -> (x, y).
E >
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Define a type(1, 0) form omega4 and check that it is closed.
E2 >
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| (2.15) |
E2 >
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Apply the horizontal homotopy operator to omega4 to define eta4.
E2 >
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| (2.17) |
Check that omega4 = dH(eta4).
E2 >
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| (2.18) |
Define a type(2, 0) form omega5 and check that its Euler-Lagrange form vanishes identically.
E2 >
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| (2.19) |
E2 >
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| (2.20) |
E2 >
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| (2.21) |
E2 >
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| (2.22) |
So omega5 = dH(eta5a) but we can often find a much simpler answer.
E2 >
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| (2.23) |
E2 >
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| (2.24) |
E2 >
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| (2.25) |
E2 >
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