The general first order ODE invariant under X
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X rewritten in the gauge xi=0
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If the ODE is given, its right hand side is used to replace the highest derivative (in this example the ODE is of first order).
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So, the above is just the original symmetry X rewritten in the gauge xi=0. Let's test this result.
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The general form in which X above can be rewritten is as follows:
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| (8) |
where _F2(x, y) is an arbitrary function of its arguments, introduced by Xgauge. This result can be tested as well.
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