In linear algebra, a one-form on a vector space is the same as a linear functional on the space. The usage of one-form in this context usually distinguishes the one-forms from higher-degree multilinear functionals on the space. For details, see linear functional.
In differential geometry, a one-form on a differentiable manifold is a smooth section of the cotangent bundle. Equivalently, a one-form on a manifold M is a smooth mapping of the total space of the tangent bundle of M to R whose restriction to each fibre is a linear functional on the tangent space. Symbolically,
where αx is linear.
Often one-forms are described locally, particularly in local coordinates. In a local coordinate system, a one-form is a linear combination of the differentials of the coordinates:
where the fi are smooth functions. Note the use of upper numerical indices, not to be confused with powers. From this perspective, a one-form has a covariant transformation law on passing from one coordinate system to another. Thus a one-form is an order 1 covariant tensor field.
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Many real-world concepts can be described as one-forms:
Let be open (e.g., an interval ), and consider a differentiable function , with derivative f'. The differential df of f, at a point , is defined as a certain linear map of the variable dx. Specifically, . (The meaning of the symbol dx is thus revealed: it is simply an argument, or independent variable, of the function df.) Hence the map sends each point x to a linear functional df(x,dx). This is the simplest example of a differential (one-)form.
In terms of the de Rham complex, one has an assignment from zero-forms (scalar functions) to one-forms i.e., .