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The method of coadjoint orbits suggests that irreducible unitary representations of a Lie group $G$ are something like quantum mechanical systems. In fact finding all irreducible unitary representation of nilpotent lie groups correspounds to geometric quantization of coadjoint orbits. In fact quantiz ation problem comes down to a finite set of coadjoint orbits for each reductive group: the nilpotent orbits. The method was carried over to geometric quantization where you want to deform the pointwise multiplication of functions with the Poisson bracket to a noncommutative product with the Poisson bracket as a first order approximation. Ultimately this lead to star product quantization.

In symplectic geometry: quantization commutes with reduction :

states that the space of global sections of a line bundle satisfying the quantization condition on the symplectic quotient of a compact symplectic manifold is the space of invariant sections of the line bundle.

In topology, Geometric quantization is related to K-theory: About the conjecture quantisation co mmutes with reduction for noncompact simple groups the only finite dimensional unitary representations are direct sums of the trivial one which by Landsman's idea we can replace the representation ring of a group by the K-theory of its $C^∗$-algebra, and the $K$-index by the analytic assembly map.

The method of coadjoint orbits suggests that irreducible unitary representations of a Lie group $G$ are something like quantum mechanical systems. In fact finding all irreducible unitary representation of nilpotent lie groups correspounds to geometric quantization of coadjoint orbits. In fact quantiz ation problem comes down to a finite set of coadjoint orbits for each reductive group: the nilpotent orbits.

In symplectic geometry: quantization commutes with reduction :

states that the space of global sections of a line bundle satisfying the quantization condition on the symplectic quotient of a compact symplectic manifold is the space of invariant sections of the line bundle.

In topology, Geometric quantization is related to K-theory: About the conjecture quantisation co mmutes with reduction for noncompact simple groups the only finite dimensional unitary representations are direct sums of the trivial one which by Landsman's idea we can replace the representation ring of a group by the K-theory of its $C^∗$-algebra, and the $K$-index by the analytic assembly map.

The method of coadjoint orbits suggests that irreducible unitary representations of a Lie group $G$ are something like quantum mechanical systems. In fact finding all irreducible unitary representation of nilpotent lie groups correspounds to geometric quantization of coadjoint orbits. In fact quantiz ation problem comes down to a finite set of coadjoint orbits for each reductive group: the nilpotent orbits. The method was carried over to geometric quantization where you want to deform the pointwise multiplication of functions with the Poisson bracket to a noncommutative product with the Poisson bracket as a first order approximation. Ultimately this lead to star product quantization.

In symplectic geometry: quantization commutes with reduction :

states that the space of global sections of a line bundle satisfying the quantization condition on the symplectic quotient of a compact symplectic manifold is the space of invariant sections of the line bundle.

In topology, Geometric quantization is related to K-theory: About the conjecture quantisation co mmutes with reduction for noncompact simple groups the only finite dimensional unitary representations are direct sums of the trivial one which by Landsman's idea we can replace the representation ring of a group by the K-theory of its $C^∗$-algebra, and the $K$-index by the analytic assembly map.

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The method of coadjoint orbits suggests that irreducible unitary r epresentationsrepresentations of a Lie group $G$ are something like quantum mechanical systems. In fact finding all irreducible unitary representation of nilpotent lie groups correspounds to geometric quantization of coadjoint orbits. In fact quantiz ation problem comes down to a finite set of coadjoint orbits for each reductive group: the nilpotent orbits.

In symplectic geometry: quantization commutes with reduction :

states that the space of global sections of a line bundle satisfying the quantization condition on the symplectic quotient of a compact symplectic manifold is the space of invariant sections of the line bundle.

In topology, Geometric quantization is related to K-theory: About the conjecture quantisation co mmutes with reduction for noncompact simple groups the only finite dimensional unitary representations are direct sums of the trivial one which by Landsman's idea we can replace the representation ring of a group by the K-theory of its $C^∗$-algebra, and the $K$-index by the analytic assembly map.

The method of coadjoint orbits suggests that irreducible unitary r epresentations of a Lie group $G$ are something like quantum mechanical systems. In fact finding all irreducible unitary representation of nilpotent lie groups correspounds to geometric quantization of coadjoint orbits. In fact quantiz ation problem comes down to a finite set of coadjoint orbits for each reductive group: the nilpotent orbits.

In symplectic geometry: quantization commutes with reduction :

states that the space of global sections of a line bundle satisfying the quantization condition on the symplectic quotient of a compact symplectic manifold is the space of invariant sections of the line bundle.

The method of coadjoint orbits suggests that irreducible unitary representations of a Lie group $G$ are something like quantum mechanical systems. In fact finding all irreducible unitary representation of nilpotent lie groups correspounds to geometric quantization of coadjoint orbits. In fact quantiz ation problem comes down to a finite set of coadjoint orbits for each reductive group: the nilpotent orbits.

In symplectic geometry: quantization commutes with reduction :

states that the space of global sections of a line bundle satisfying the quantization condition on the symplectic quotient of a compact symplectic manifold is the space of invariant sections of the line bundle.

In topology, Geometric quantization is related to K-theory: About the conjecture quantisation co mmutes with reduction for noncompact simple groups the only finite dimensional unitary representations are direct sums of the trivial one which by Landsman's idea we can replace the representation ring of a group by the K-theory of its $C^∗$-algebra, and the $K$-index by the analytic assembly map.

added 281 characters in body
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user21574
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The method of coadjoint orbits suggests that irreducible unitary r epresentations of a Lie group $G$ are something like quantum mechanical systems. In fact finding all irreducible unitary representation of nilpotent lie groups correspounds to geometric quantization of coadjoint orbits. In fact quantiz ation problem comes down to a finite set of coadjoint orbits for each reductive group: the nilpotent orbits.

In symplectic geometry: quantization commutes with reduction :

states that the space of global sections of a line bundle satisfying the quantization condition on the symplectic quotient of a compact symplectic manifold is the space of invariant sections of the line bundle.

The method of coadjoint orbits suggests that irreducible unitary r epresentations of a Lie group $G$ are something like quantum mechanical systems. In fact finding all irreducible unitary representation of nilpotent lie groups correspounds to geometric quantization of coadjoint orbits. In fact quantiz ation problem comes down to a finite set of coadjoint orbits for each reductive group: the nilpotent orbits.

The method of coadjoint orbits suggests that irreducible unitary r epresentations of a Lie group $G$ are something like quantum mechanical systems. In fact finding all irreducible unitary representation of nilpotent lie groups correspounds to geometric quantization of coadjoint orbits. In fact quantiz ation problem comes down to a finite set of coadjoint orbits for each reductive group: the nilpotent orbits.

In symplectic geometry: quantization commutes with reduction :

states that the space of global sections of a line bundle satisfying the quantization condition on the symplectic quotient of a compact symplectic manifold is the space of invariant sections of the line bundle.

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user21574
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