Talk:Symmetry

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Revision as of 12:18, 25 October 2006 by Douglaseagleson (talk | contribs)
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This is real hard stuff to get good. And the transfrom as symmetric appears to exact good design. A certain alteration as the relation appears to always be, though. Any transform is a certain transformed relation! This is the form of symmetric.

Take transform itself to. And so the correct transform for abstract symmetry become a certain absolute. All, a, as the, s. A set of a element where each, a, as, s, is a function unrelated/independent to a's cause to exist.

And the mathmatical form of transfrom then allows this definition o. And so the set o, as transform of, a, appears the group as symmetry itself.

A logicial inverted symmetry appears the cause, to set a. And so the finite appearance of the Hamiltonian t, a. This property of the Hamiltonian caused enormous effect in mathematics and to identify the reason as its finite a, is the meaning of t.

this form is allowed.


 A= |h|

A set of all a as A then functionally relates any. Making the eigenstate a differential.

And so I challenge the author. I use this way different logical symemtry to alter the Hamiltonian to the form Hamilton himself was searching for.

Please consider the implication. --Douglaseagleson 08:18, 25 October 2006 (EDT)