Differential geometry in physics

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SUMMARY

Differential geometry provides significant insights into physics, particularly in reformulating classical theories such as Hamiltonian Mechanics and Electromagnetism. Key concepts include the wedge product, Hodge duality, and de Rham cohomology, which enhance mathematical clarity and facilitate the transition to General Relativity (GR) and gauge theories. Recommended readings include "Differential Forms" by Bott and Tu, "General Relativity" by Straumann, and "Gauge Fields, Knots and Gravity" by Baez and Muniain, among others. These resources cover both advanced and foundational topics, bridging pure mathematics and physical applications.

PREREQUISITES
  • Understanding of differential forms and their applications in physics
  • Familiarity with General Relativity and gauge theories
  • Basic knowledge of Hamiltonian mechanics and symplectic geometry
  • Ability to comprehend mathematical texts, particularly in differential geometry
NEXT STEPS
  • Study "Differential Forms" by Bott and Tu for foundational concepts in differential geometry
  • Explore "General Relativity" by Straumann for a mathematical treatment of Einstein-Maxwell Theory
  • Research symplectic geometry and its applications in Hamiltonian mechanics
  • Investigate "Recent Developments in Deformation Quantization" by Waldmann for insights into Quantum Mechanics
USEFUL FOR

This discussion is beneficial for physicists, mathematicians, and students interested in the intersection of differential geometry and theoretical physics, particularly those focusing on advanced topics in General Relativity and gauge theories.

Silviu
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Hello! I started reading some differential geometry applied in physics (wedge product, Hodge duality etc.) and how you can rewrite classical theories (Hamiltonian Mechanics, Electromagnetism) in a much nicer way. Can someone point me towards some reading about how can more information be obtained using these methods than the classical approach (I assume this is not used just to write old stuff in a nicer way, but it also gives new insight) and any reading that I might need in between in order to understand? Thank you!
 
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Silviu said:
I assume this is not used just to write old stuff in a nicer way, but it also gives new insight
Well, it gives you a better mathematical insight, hence you can apply mathematical theorems possibly more directly. For example it becomes much clearer, when and why the scalar and vector potentials exist. (this is connected to the concept of de Rham cohomology. The natural reference for this is: Bott, Tu - Differential Forms)

Also it makes the transition to GR and gauge theories easier. The formulation of ED in terms of differential forms is useful because you can in fact directly generalize it to the Maxwell-part of Einstein-Maxwell-Theory and also it is nice to relate it more directly to gauge theory, where the gauge field ##A## (=vector potential) is naturally written as a 1-form. Furthermore, if you can deal with it, it makes most calculations much shorter.

For a nice mathematical treatment of Einstein-Maxwell-Theory, see
Straumann - General Relativity.

Gauge theory (and also a nice treatment of ED) is incorporated in
Baez, Muniain - Gauge Fields, Knots and Gravity

Further general references:
Nakahara - Geometry, Topology and Physics
Frankel - The Geometry of Physics
Naber - Topology, Geometry and Gauge Fields I and II
Naber - The Geometry of Minkowski Space Time


In all of these you will find more advanced stuff and more basic stuff, as well as physical applications and pure mathematics.

If you are capable of reading and understanding German, I would also recommend
Knauff - Mathematische Physik-Klassische Mechanik

For Hamiltonian mechanics you could also search for books and lecture notes on symplectic geometry, e.g. https://people.math.ethz.ch/~acannas/Papers/lsg.pdf

The symplectic approach to Hamiltonian mechanics is for example used in the Deformation Quantization approach to Quantum Mechanics, where you deform the symplectic structure on phase space in order to represent Quantum Mechanics purely algebraically in terms of classical functions.
See, e.g.
Waldmann - Recent Developments in Deformation Quantization
 
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