What Does One Form Mean in Relativity Theory?

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SUMMARY

The discussion clarifies the concept of "One Forms" in Relativity Theory, defining them as mathematical entities that represent linear functions taking vectors to scalars, specifically categorized as tensors. The local linear behavior of functions on a manifold is expressed using coordinate 1-forms, denoted as dxi, leading to the equation df = ∑(∂f/∂xi)dxi. Participants recommend studying "Applied Differential Geometry" and "Spacetime, Geometry and Cosmology" by William Burke to gain a deeper understanding of the topic, emphasizing the necessity of a foundation in tensor analysis.

PREREQUISITES
  • Tensor analysis
  • Understanding of manifolds
  • Basic knowledge of differential geometry
  • Familiarity with covariant vectors
NEXT STEPS
  • Study the concept of manifolds in detail
  • Learn about covariant tensors and their applications
  • Explore the operator divergence and its relation to One Forms
  • Read "Applied Differential Geometry" and "Spacetime, Geometry and Cosmology" by William Burke
USEFUL FOR

This discussion is beneficial for students and enthusiasts of Relativity Theory, mathematicians interested in differential geometry, and anyone seeking to understand the mathematical foundations of One Forms and their applications in physics.

Jomapil
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Hello, everyone

I began do learn Relativity Theory. I don't understand the term " One Forms " that appear in some books. Can anyone tell me what did it mean? The translation to Portuguese doesn't any sense and the explanation of the books is not very explicative for me.

Thank you very much.
 
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''One forms'' are a mathematical lingo for a linear function that takes a vector and returns a scalar; it's therefore a type of tensor.
 
1-forms are the geometric objects corresponding to the local linear behavior of functions on a manifold.

If a patch of a manifold M is described by the coordinate functions xi : M → R, then for any function f on that patch, its local linear behavior can be given a coordinate representation in terms of the coordinate 1-forms dxi thus: df = ∑(∂f/∂xi)dxi, where the numnbers ∂f/∂xi are called the components of df.

For more details I recommend these books: "Applied Differential Geometry" and "Spacetime, Geometry and Cosmology" by William Burke.
 
A one-form is exactly the same as what other people call "a covariant vector". :) But to understand this you need some basis in tensor analysis.
 
Good evening.

haushofer - I studied tensor calculus 35 years ago and I'm reading and exercising at the same time I'm learning Relativity Theory, so I understand your explanation - EVERY covariant tensor is an One-Form.

ManyNames - I think I understood your explanation - for example the operator divergence [ div(vctor) --> escalar] is an One-Forms.

dx - I'm going soon to read about manifolds - anyway I also understood your help.

Thank you everyone and a good new week.
 
In an inertial frame of reference (IFR), there are two fixed points, A and B, which share an entangled state $$ \frac{1}{\sqrt{2}}(|0>_A|1>_B+|1>_A|0>_B) $$ At point A, a measurement is made. The state then collapses to $$ |a>_A|b>_B, \{a,b\}=\{0,1\} $$ We assume that A has the state ##|a>_A## and B has ##|b>_B## simultaneously, i.e., when their synchronized clocks both read time T However, in other inertial frames, due to the relativity of simultaneity, the moment when B has ##|b>_B##...

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