Ricci calculus

In <a href="/facts/Mathematics/pxTouaz4">mathematics</a>, Ricci calculus constitutes the rules of index notation and manipulation for <a href="/facts/Tensors/pNjFo5tV">tensors</a> and <a href="/facts/Tensor_fields/cAC6F6rF">tensor fields</a> on a <a href="/facts/Differentiable_manifold/aSnbXKcV">differentiable manifold</a>, with or without a <a href="/facts/Metric_tensor/tbqek1gJ">metric tensor</a> or <a href="/facts/Connection_(mathematics)/KURsCmIu">connection</a>. It is also the modern name for what used to be called the absolute differential calculus (the foundation of tensor calculus), tensor calculus or tensor analysis developed by <a href="/facts/Gregorio_Ricci-Curbastro/HjBVjmPB">Gregorio Ricci-Curbastro</a> in 1887–1896, and subsequently popularized in a paper written with his pupil <a href="/facts/Tullio_Levi-Civita/LmxVG3GP">Tullio Levi-Civita</a> in 1900. <a href="/facts/Jan_Arnoldus_Schouten/0tWqLRmq">Jan Arnoldus Schouten</a> developed the modern notation and formalism for this mathematical framework, and made contributions to the theory, during its applications to <a href="/facts/General_relativity/jVsoIg8X">general relativity</a> and <a href="/facts/Differential_geometry/c04XmyLu">differential geometry</a> in the early twentieth century. The basis of modern tensor analysis was developed by <a href="/facts/Bernhard_Riemann/oV2fL0k8">Bernhard Riemann</a> in a paper from 1861.
A component of a tensor is a <a href="/facts/Real_number/R02gw5Pb">real number</a> that is used as a coefficient of a basis element for the tensor space. The tensor is the sum of its components multiplied by their corresponding basis elements. Tensors and tensor fields can be expressed in terms of their components, and operations on tensors and tensor fields can be expressed in terms of operations on their components. The description of tensor fields and operations on them in terms of their components is the focus of the Ricci calculus. This notation allows an efficient expression of such tensor fields and operations. While much of the notation may be applied with any tensors, operations relating to a <a href="/facts/Differential_structure/nHHTJud2">differential structure</a> are only applicable to tensor fields. Where needed, the notation extends to components of non-tensors, particularly <a href="/facts/Multidimensional_array/gHJJ3XPw">multidimensional arrays</a>.
A tensor may be expressed as a linear sum of the <a href="/facts/Tensor_product/7K3pR1ap">tensor product</a> of <a href="/facts/Vector_(mathematics_and_physics)/U8mM7A5F">vector</a> and <a href="/facts/Covector/oGh7Asrz">covector</a> basis elements. The resulting tensor components are labelled by indices of the basis. Each index has one possible value per <a href="/facts/Dimension/0ktmUyac">dimension</a> of the underlying <a href="/facts/Vector_space/M1pxMLx2">vector space</a>. The number of indices equals the degree (or order) of the tensor.
For compactness and convenience, the Ricci calculus incorporates <a href="/facts/Einstein_notation/UXwS43wU">Einstein notation</a>, which implies summation over indices repeated within a term and <a href="/facts/Universal_quantification/agNmvJKN">universal quantification</a> over free indices. Expressions in the notation of the Ricci calculus may generally be interpreted as a set of simultaneous equations relating the components as functions over a manifold, usually more specifically as functions of the coordinates on the manifold. This allows intuitive manipulation of expressions with familiarity of only a limited set of rules.

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Ricci calculus