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  2. Bivector - Wikipedia

    en.wikipedia.org/wiki/Bivector

    A description of the projective geometry can be constructed in the geometric algebra using basic operations. For example, given two distinct points in RP n−1 represented by vectors a and b the line containing them is given by a ∧ b (or b ∧ a). Two lines intersect in a point if A ∧ B = 0 for their bivectors A and B. This point is given ...

  3. Riemannian manifold - Wikipedia

    en.wikipedia.org/wiki/Riemannian_manifold

    Left- and bi-invariant metrics on Lie groups are an important source of examples of Riemannian manifolds. Berger spheres , constructed as left-invariant metrics on the special unitary group SU(2), are among the simplest examples of the collapsing phenomena, in which a simply-connected Riemannian manifold can have small volume without having ...

  4. Biorthogonal system - Wikipedia

    en.wikipedia.org/wiki/Biorthogonal_system

    An example is the pair of sets of respectively left and right eigenvectors of a matrix, indexed by eigenvalue, if the eigenvalues are distinct. [ 1 ] A biorthogonal system in which E = F {\displaystyle E=F} and v ~ i = u ~ i {\displaystyle {\tilde {v}}_{i}={\tilde {u}}_{i}} is an orthonormal system .

  5. Metric signature - Wikipedia

    en.wikipedia.org/wiki/Metric_signature

    The signature of a metric tensor is defined as the signature of the corresponding quadratic form. [2] It is the number (v, p, r) of positive, negative and zero eigenvalues of any matrix (i.e. in any basis for the underlying vector space) representing the form, counted with their algebraic multiplicities.

  6. Dual basis - Wikipedia

    en.wikipedia.org/wiki/Dual_basis

    In linear algebra, given a vector space with a basis of vectors indexed by an index set (the cardinality of is the dimension of ), the dual set of is a set of vectors in the dual space with the same index set such that and form a biorthogonal system.

  7. Hodge star operator - Wikipedia

    en.wikipedia.org/wiki/Hodge_star_operator

    Generalizing this to an n-dimensional vector space, the Hodge star is a one-to-one mapping of k-vectors to (n – k)-vectors; the dimensions of these spaces are the binomial coefficients = (). The naturalness of the star operator means it can play a role in differential geometry, when applied to the cotangent bundle of a pseudo-Riemannian ...

  8. Bipolar coordinates - Wikipedia

    en.wikipedia.org/wiki/Bipolar_coordinates

    The equations for x and y can be combined to give + = ⁡ (+) [2] [3] or + = ⁡ (). This equation shows that σ and τ are the real and imaginary parts of an analytic function of x+iy (with logarithmic branch points at the foci), which in turn proves (by appeal to the general theory of conformal mapping) (the Cauchy-Riemann equations) that these particular curves of σ and τ intersect at ...

  9. Universal geometric algebra - Wikipedia

    en.wikipedia.org/wiki/Universal_geometric_algebra

    Some r-vectors are scalars (r = 0), vectors (r = 1) and bivectors (r = 2). One may generate a finite-dimensional GA by choosing a unit pseudoscalar (I). The set of all vectors that satisfy = is a vector space. The geometric product of the vectors in this vector space then defines the GA, of which I is a member.

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