What Defines a One-Form in Multivariable Calculus and Differential Geometry?

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In summary, the answer to "is it necessary that the components \omega_\mu be components of a type (0,1) tensor? " is "No".
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pellman
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A one-form is something of the form

[tex]\omega=\omega_\mu dx^\mu[/tex]

But is it necessary that the components [tex]\omega_\mu[/tex] be components of a type (0,1) tensor?

For instance, the connection one-form is defined to be

[tex]{\omega^{\alpha}}_\beta = {\Gamma^\alpha}_{\gamma\beta} \hat{\theta}^\gamma[/tex]

where [tex]\hat{\theta}^\gamma[/tex] is a basis of the dual tangent space, though not necessarily a coordinate basis. Here the components [tex]{\Gamma^\alpha}_{\gamma\beta} [/tex]--the connection coefficients, i.e., Christoffel symbols-- not only are not those of a type (0,1) tensor, they are not even those of a tensor.

So is this legitimately a one-form?
 
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I think with any vector bundle E over your manifold M, it's fair to call any (bundle) mapping TM-->E a "one-form". (i.e. a function that takes tangent vectors and maps them to E-vectors)

For the usual one-forms, E is just the trivial line bundle MxR-->M -- that is, the one in which scalar fields live. Each (usual) one-form takes a tangent vector field on M and maps it to a scalar field on M. T*M is the bundle in which all such one-forms live.
 
  • #3
Thank you, Hurkyl. I'm getting there, I really am. But I am in chap 7 of Nakahara's Geometry, Topology, and Physics and fibre bundles and such are in chap 9. I think you are saying that the answer to "is it necessary that the components [tex]\omega_\mu[/tex] be components of a type (0,1) tensor? " is "No". Is that right?

Each (usual) one-form takes a tangent vector field on M and maps it to a scalar field on M. T*M is the bundle in which all such one-forms live

Then again, maybe this means "Yes, it is necessary"? The elements of T*M are identical with the (0,1) tensors, aren't they?
 
  • #4
pellman said:
(...)
For instance, the connection one-form is defined to be

[tex]{\omega^{\alpha}}_\beta = {\Gamma^\alpha}_{\gamma\beta} \hat{\theta}^\gamma[/tex]
(...)

I heared "connection one-form" but i see 2 components "two indices" ! [tex]{{\omega^{\alpha}}_\beta}'s[/tex] are not one-forms and are not expressed in the natural basis (dx) they are the components of a 1-1 tensor and a form has never been a 1-1 tensor ! I think :biggrin:
 
  • #5
I think maybe it is just sloppy use of the term "one-form". Though I think it is standard. The wikipedia entry just calls it "connection form" instead of "connection one form" But it is linear in the one-form basis elements [tex]\hat{\theta}^\alpha[/tex]. It is not a k-form where k>1.

On the other hand, maybe any linear combination of the [tex]\hat{\theta}^\alpha[/tex] is a one form, even though the coefficients are the not components of a (0,1) tensor. I'm not able to glean how strict the definition of a one-form is from the sources I have checked.
 

FAQ: What Defines a One-Form in Multivariable Calculus and Differential Geometry?

What is the definition of a one-form?

A one-form is a mathematical object that associates a real number to each point in a vector space. It can be thought of as a function that takes in a vector and returns a scalar value.

How is a one-form different from a vector?

A vector is a mathematical object that has both magnitude and direction, and can be represented by an arrow. A one-form, on the other hand, is a function that takes in a vector and returns a scalar value. In other words, a one-form operates on vectors, while a vector is an element of the vector space itself.

What are some examples of one-forms?

Some common examples of one-forms include work, pressure, and heat flux. These are all quantities that take in a vector (such as force, area, or heat flow) and return a scalar value.

What is the geometric interpretation of a one-form?

The geometric interpretation of a one-form is a set of tangent planes to a surface. Each point on the surface represents a different tangent plane, and the one-form assigns a scalar value to that plane. This allows for the calculation of quantities such as work and flux through the surface.

How is a one-form represented mathematically?

In coordinate form, a one-form is represented by a linear combination of basis one-forms, which are typically denoted by the symbols dx, dy, and dz. These basis one-forms are associated with the coordinate axes, and the coefficients represent the values assigned to each tangent plane. In index notation, a one-form is represented by a covector, which is a column vector with the same number of components as the basis one-forms.

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