A What is the point of geometric quantization?

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Geometric quantization is explored for its applications in quantum-classical hybrid systems and symplectic geometry, though its practical utility outside mathematical theory is questioned. The discussion highlights its relevance to understanding quantization, integrable quantum systems, and constructing irreducible unitary representations of groups. However, concerns are raised about whether geometric quantization can reproduce quantum mechanics for particles constrained to surfaces in three-dimensional space. References to group representation and geometric quantization are shared, emphasizing the need for clarity between understanding and reproducing quantum mechanics. Overall, the conversation reflects a desire for deeper insights into the practical implications of geometric quantization.
andresB
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I studied the basics of geometric quantization for a recent work in quantum-classical hybrid systems1. It was an easy application of the method of gometric quantization (prequantization + polarization in ##\mathbb{R}^{3}##).
The whole topic seems interesting since I want to learn more of symplectic geometry, but (outside the aforementioned half-quantization to get a quantum-classical theory) I fail to see the point of the whole endeavor. For example, particles constrained to move on a surface are treated with the formalism of the geometric potential of Jensen, Koppe, and Da Costa2 , and not from a quantization of the related classical situation.

What actual result from geometric quantization is important and useful outside the mathematical dicipline of geometric quantization itself?[1]https://arxiv.org/abs/2107.03623
[2]https://arxiv.org/abs/1602.00528
 
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andresB said:
What actual result from geometric quantization is important and useful outside the mathematical dicipline of geometric quantization itself?
It is important for the understanding of quantization in general, for integrable quantum systems and for the construction of irreducible unitary representations of groups.
 
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A. Neumaier said:
It is important for the understanding of quantization in general, for integrable quantum systems and for the construction of irreducible unitary representations of groups.

Well, the first part does not sound convincing. Does geometric quantization reproduces the quantum mechanic of a partice constrained to move on a surface embbeded in ##\mathbb{R}^{3}##?
Does it produce testable results that can't be obtained just by using the usual tools of QM?The unitary representation of groups does sound interesting. My work was about the Galilei Group in classical and "half"-quantized systems. Any good reference on group representation and geometric quantization?
 
andresB said:
Does geometric quantization reproduces the quantum mechanic of a partice constrained to move on a surface
Understanding and reproducing details are very different issues.
andresB said:
Any good reference on group representation and geometric quantization?
https://link.springer.com/chapter/10.1007/978-3-662-06791-8_2
https://arxiv.org/pdf/math-ph/0208008.pdf
https://www.math.columbia.edu/~woit/QM/qmbook.pdf
https://arxiv.org/pdf/1801.02307.pdf
https://link-springer-com.uaccess.univie.ac.at/content/pdf/10.1007/BF02097053.pdf
https://s3.cern.ch/inspire-prod-files-6/6869199e89f197300faf2f93e55dc112
 
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Woodhouse is the standard reference on Geometric Quantization and quite well written.
 
For the quantum state ##|l,m\rangle= |2,0\rangle## the z-component of angular momentum is zero and ##|L^2|=6 \hbar^2##. According to uncertainty it is impossible to determine the values of ##L_x, L_y, L_z## simultaneously. However, we know that ##L_x## and ## L_y##, like ##L_z##, get the values ##(-2,-1,0,1,2) \hbar##. In other words, for the state ##|2,0\rangle## we have ##\vec{L}=(L_x, L_y,0)## with ##L_x## and ## L_y## one of the values ##(-2,-1,0,1,2) \hbar##. But none of these...

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