Difference between revisions of "Lagrangian manifold"
(Importing text file) |
(latex details) |
||
(One intermediate revision by one other user not shown) | |||
Line 1: | Line 1: | ||
− | + | <!-- | |
+ | l0572701.png | ||
+ | $#A+1 = 19 n = 0 | ||
+ | $#C+1 = 19 : ~/encyclopedia/old_files/data/L057/L.0507270 Lagrangian manifold | ||
+ | Automatically converted into TeX, above some diagnostics. | ||
+ | Please remove this comment and the {{TEX|auto}} line below, | ||
+ | if TeX found to be correct. | ||
+ | --> | ||
− | + | {{TEX|auto}} | |
+ | {{TEX|done}} | ||
− | is | + | An $ n $- |
+ | dimensional differentiable submanifold $ L ^ {n} $ | ||
+ | of a $ 2n $- | ||
+ | dimensional [[Symplectic manifold|symplectic manifold]] $ M ^ {2n} $ | ||
+ | such that the exterior form $ \omega $ | ||
+ | specifying the symplectic structure on $ M ^ {2n} $ | ||
+ | vanishes identically on $ L ^ {n} $( | ||
+ | that is, for any point $ x \in L ^ {n} $ | ||
+ | and any vectors $ X $ | ||
+ | and $ Y $ | ||
+ | which are tangent to $ L ^ {n} $ | ||
+ | at this point one has $ \omega ( X , Y ) = 0 $). | ||
+ | In the most important case, when $ M ^ {2n} = \mathbf R ^ {2n} $ | ||
+ | with coordinates ( $ p _ {1} \dots p _ {n} , q _ {1} \dots q _ {n} $) | ||
+ | and $ \omega = \sum_{i=1} ^ {n} dp _ {i} \wedge dq _ {i} $, | ||
+ | the condition that the submanifold $ L ^ {n} $ | ||
+ | given by the parametric equations | ||
− | + | $$ | |
+ | p _ {i} = p _ {i} ( u _ {1} \dots u _ {n} ) ,\ q _ {i} = q _ {i} ( u _ {1} \dots u _ {n} ) | ||
+ | $$ | ||
− | + | is Lagrangian, has the form | |
− | |||
− | |||
− | |||
+ | $$ | ||
+ | [ u _ {i} , u _ {j} ] = 0 ,\ i , j = 1 \dots n , | ||
+ | $$ | ||
+ | where $ [ u _ {i} , u _ {j} ] $ | ||
+ | is the [[Lagrange bracket]]. | ||
====Comments==== | ====Comments==== | ||
Line 18: | Line 46: | ||
====References==== | ====References==== | ||
− | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> P. Libermann, C.-M. Marle, "Symplectic geometry and analytical mechanics" , Reidel (1987) (Translated from French)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> I. Vaismann, "Symplectic geometry and secondary characteristic classes" , Birkhäuser (1987)</TD></TR></table> | + | <table> |
+ | <TR><TD valign="top">[1]</TD> <TD valign="top"> V.P. Maslov, "Théorie des perturbations et méthodes asymptotiques" , Dunod (1972) (Translated from Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> V.P. Maslov, "Introduction to the method of phase integrals (the WKB method)" , Moscow (1965) (In Russian) (Appendix to the Russian translation of: J. Heading, The WKB method in the multi-dimensional case)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> V.I. Arnol'd, "Mathematical methods of classical mechanics" , Springer (1978) (Translated from Russian)</TD></TR><TR><TD valign="top">[4]</TD> <TD valign="top"> V.P. Maslov, M.V. Fedoryuk, "Quasi-classical approximation for the equations of quantum mechanics" , Reidel (1981) (Translated from Russian)</TD></TR><TR><TD valign="top">[5]</TD> <TD valign="top"> A.S. Mishchenko, B.Yu. Sternin, V.E. Shatalov, "Lagrangian manifolds and the method of the canonical operator" , Moscow (1978) (In Russian)</TD></TR><TR><TD valign="top">[6]</TD> <TD valign="top"> V.I. [V.I. Arnol'd] Arnold, A.B. [A.B. Givent'al] Giventhal, "Symplectic geometry" , ''Dynamical Systems'' , '''IV''' , Springer (1988) (Translated from Russian)</TD></TR> | ||
+ | <TR><TD valign="top">[a1]</TD> <TD valign="top"> P. Libermann, C.-M. Marle, "Symplectic geometry and analytical mechanics" , Reidel (1987) (Translated from French)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> I. Vaismann, "Symplectic geometry and secondary characteristic classes" , Birkhäuser (1987)</TD></TR> | ||
+ | </table> |
Latest revision as of 18:57, 9 January 2024
An $ n $-
dimensional differentiable submanifold $ L ^ {n} $
of a $ 2n $-
dimensional symplectic manifold $ M ^ {2n} $
such that the exterior form $ \omega $
specifying the symplectic structure on $ M ^ {2n} $
vanishes identically on $ L ^ {n} $(
that is, for any point $ x \in L ^ {n} $
and any vectors $ X $
and $ Y $
which are tangent to $ L ^ {n} $
at this point one has $ \omega ( X , Y ) = 0 $).
In the most important case, when $ M ^ {2n} = \mathbf R ^ {2n} $
with coordinates ( $ p _ {1} \dots p _ {n} , q _ {1} \dots q _ {n} $)
and $ \omega = \sum_{i=1} ^ {n} dp _ {i} \wedge dq _ {i} $,
the condition that the submanifold $ L ^ {n} $
given by the parametric equations
$$ p _ {i} = p _ {i} ( u _ {1} \dots u _ {n} ) ,\ q _ {i} = q _ {i} ( u _ {1} \dots u _ {n} ) $$
is Lagrangian, has the form
$$ [ u _ {i} , u _ {j} ] = 0 ,\ i , j = 1 \dots n , $$
where $ [ u _ {i} , u _ {j} ] $ is the Lagrange bracket.
Comments
Also often called Lagrangian submanifold.
References
[1] | V.P. Maslov, "Théorie des perturbations et méthodes asymptotiques" , Dunod (1972) (Translated from Russian) |
[2] | V.P. Maslov, "Introduction to the method of phase integrals (the WKB method)" , Moscow (1965) (In Russian) (Appendix to the Russian translation of: J. Heading, The WKB method in the multi-dimensional case) |
[3] | V.I. Arnol'd, "Mathematical methods of classical mechanics" , Springer (1978) (Translated from Russian) |
[4] | V.P. Maslov, M.V. Fedoryuk, "Quasi-classical approximation for the equations of quantum mechanics" , Reidel (1981) (Translated from Russian) |
[5] | A.S. Mishchenko, B.Yu. Sternin, V.E. Shatalov, "Lagrangian manifolds and the method of the canonical operator" , Moscow (1978) (In Russian) |
[6] | V.I. [V.I. Arnol'd] Arnold, A.B. [A.B. Givent'al] Giventhal, "Symplectic geometry" , Dynamical Systems , IV , Springer (1988) (Translated from Russian) |
[a1] | P. Libermann, C.-M. Marle, "Symplectic geometry and analytical mechanics" , Reidel (1987) (Translated from French) |
[a2] | I. Vaismann, "Symplectic geometry and secondary characteristic classes" , Birkhäuser (1987) |
Lagrangian manifold. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Lagrangian_manifold&oldid=16390