Orthogonal group

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v · mathematics, the orthogonal group of degree n over a field F (written as O(n,F)) is the group of n × n orthogonal matrices with entries from F, with the group operation of matrix multiplication. This is a subgroup of the general linear group GL(n,F) given by $\mathrm{O}(n,F) = \{ Q \in \mathrm{GL}(n,F) \mid Q^T Q = Q Q^T = I \}$ where QT is the transpose of Q. The classical orthogonal group over the real numbers is usually just written O(n). More generally the orthogonal group of a non-singular quadratic form over F is the group of linear operators preserving the form – the above group O(n, F) is then the orthogonal group of the sum-of-n-squares quadratic form.[1] The Cartan–Dieudonné theorem describes the structure of the orthogonal group for non-singular form. This article only discusses definite forms – the orthogonal group of the positive definite form (equivalent to sum of n squares) and negative definite forms (equivalent to the negative sum of n squares) are identical – O(n,0) = O(0,n) – though the associated Pin groups differ; for other non-singular forms O(p,q), see indefinite orthogonal group. Every orthogonal matrix has determinant either 1 or −1. The orthogonal n-by-n matrices with determinant 1 form a normal subgroup of O(n,F) known as the special orthogonal group, SO(n,F). (More precisely, SO(n,F) is the kernel of the Dickson invariant, discussed below.) By analogy with GL/SL (general linear group, special linear group), the orthogonal group is sometimes called the general orthogonal group and denoted GO, though this term is also sometimes used for indefinite orthogonal groups O(p,q). The derived subgroup Ω(n,F) of O(n,F) is an often studied object because when F is a finite field Ω(n,F) is often a central extension of a finite simple group. Both O(n,F) and SO(n,F) are algebraic groups, because the condition that a matrix be orthogonal, i.e. have its own transpose as inverse, can be expressed as a set of polynomial equations in the entries of the matrix. Over the real number field Over the field R of real numbers, the orthogonal group O(n,R) and the special orthogonal group SO(n,R) are often simply denoted by O(n) and SO(n) if no confusion is possible. They form real compact Lie groups of dimension n(n − 1)/2. O(n,R) has two connected components, with SO(n,R) being the identity component, i.e., the connected component containing the identity matrix. The real orthogonal and real special orthogonal groups have the following geometric interpretations: O(n,R) is a subgroup of the Euclidean group E(n), the group of isometries of Rn; it contains those that leave the origin fixed – O(n,R) = E(n) ∩ GL(n,R). It is the symmetry group of the sphere (n = 3) or hypersphere and all objects with spherical symmetry, if the origin is chosen at the center. SO(n,R) is a subgroup of E+(n), which consists of direct isometries, i.e., isometries preserving orientation; it contains those that leave the origin fixed – $SO(n,\mathbf{R}) = E^+(n) \cap GL(n,\mathbf{R}) = E(n) \cap GL^+(n,\mathbf{R}).$ It is the rotation group of the sphere and all objects with spherical symmetry, if the origin is chosen at the center. { I, −I } is a normal subgroup and even a characteristic subgroup of O(n,R), and, if n is even, also of SO(n,R). If n is odd, O(n,R) is the direct product of SO(n,R) and { I, −I }. The cyclic group of k-fold rotations Ck is for every positive integer k a normal subgroup of O(2,R) and SO(2,R). Relative to suitable orthogonal bases, the isometries are of the form: $\begin{bmatrix} \begin{matrix}R_1 & & \\ & \ddots & \\ & & R_k\end{matrix} & 0 \\ 0 & \begin{matrix}\pm 1 & & \\ & \ddots & \\ & & \pm 1\end{matrix} \\ \end{bmatrix}$ where the matrices R1,...,Rk are 2-by-2 rotation matrices in orthogonal planes of rotation. As a special case, known as Euler's rotation theorem, any (non-identity) element of SO(3,R) is rotation about a uniquely defined axis. The orthogonal group is generated by reflections (two reflections give a rotation), as in a Coxeter group,[note 1] and elements have length at most n (require at most n reflections to generate; this follows from the above classification, noting that a rotation is generated by 2 reflections, and is true more generally for indefinite orthogonal groups, by the Cartan–Dieudonné theorem). A longest element (element needing the most reflections) is reflection through the origin (the map $v \mapsto -v$), though so are other maximal combinations of rotations (and a reflection, in odd dimension). The symmetry group of a circle is O(2,R), also called Dih (S1), where S1 denotes the multiplicative group of complex numbers of absolute value 1. SO(2,R) is isomorphic (as a Lie group) to the circle S1 (circle group). This isomorphism sends the complex number exp(φi) = cos(φ) + i sin(φ) to the orthogonal matrix $\begin{bmatrix}\cos(\phi)&-\sin(\phi)\\ \sin(\phi)&\cos(\phi)\end{bmatrix}.$ The group SO(3,R), understood as the set of rotations of 3-dimensional space, is of major importance in the sciences and engineering. See rotation group and the general formula for a 3 × 3 rotation matrix in terms of the axis and the angle. In terms of algebraic topology, for n > 2 the fundamental group of SO(n,R) is cyclic of order 2, and the spinor group Spin(n) is its universal cover. For n = 2 the fundamental group is infinite cyclic and the universal cover corresponds to the real line (the spinor group Spin(2) is the unique 2-fold cover). Even and odd dimension The structure of the orthogonal group differs in certain respects between even and odd dimensions – for example, − I (reflection through the origin) is orientation-preserving in even dimension, but orientation-reversing in odd dimension. When this distinction wishes to be emphasized, the groups are generally denoted O(2k) and O(2k+1), reserving n for the dimension of the space (n = 2k or n = 2k + 1). The letters p or r are also used, indicating the rank of the corresponding Lie algebra; in odd dimension the corresponding Lie algebra is Br = so2r + 1, while in even dimension the Lie algebra is Dr = so2r. Lie algebra The Lie algebra associated to the Lie groups O(n,R) and SO(n,R) consists of the skew-symmetric real n-by-n matrices, with the Lie bracket given by the commutator. This Lie algebra is often denoted by o(n,R) or by so(n,R), and called the orthogonal Lie algebra or special orthogonal Lie algebra. These Lie algebras are the compact real forms of two of the four families of semisimple Lie algebras: in odd dimension Br = so2r + 1, while in even dimension Dr = so2r. More intrinsically, given a vector space with an inner product, the special orthogonal Lie algebra is given by the bivectors on the space, which are sums of simple bivectors (2-blades) $v \wedge w$. The correspondence is given by the map $v \wedge w \mapsto v^* \otimes w - w^* \otimes v,$ where v * is the covector dual to the vector v; in coordinates these are exactly the elementary skew-symmetric matrices. This characterization is used in interpreting the curl of a vector field (naturally a 2-vector) as an infinitesimal rotation or "curl", hence the name. Generalizing the inner product with a nondegenerate form yields the indefinite orthogonal Lie algebras sop,q. The representation theory of the orthogonal Lie algebras includes both representations corresponding to linear representations of the orthogonal groups, and representations corresponding to projective representations of the orthogonal groups (linear representations of spin groups), the so-called spin representation, which are important in physics. 3D isometries that leave the origin fixed Isometries of R3 that leave the origin fixed, forming the group O(3,R), can be categorized as: SO(3,R): identity rotation about an axis through the origin by an angle not equal to 180° rotation about an axis through the origin by an angle of 180° the same with inversion in the origin (x is mapped to −x), i.e. respectively: inversion in the origin rotation about an axis by an angle not equal to 180°, combined with reflection in the plane through the origin perpendicular to the axis reflection in a plane through the origin. The 4th and 5th in particular, and in a wider sense the 6th also, are called improper rotations. See also the similar overview including translations. Conformal group Main article: Conformal group Being isometries (preserving distances), orthogonal transforms also preserve angles, and are thus conformal maps, though not all conformal linear transforms are orthogonal. In classical terms this is the difference between congruence and similarity, as exemplified by SSS (Side-Side-Side) congruence of triangles and AAA (Angle-Angle-Angle) similarity of triangles. The group of conformal linear maps of Rn is denoted CO(n) for the conformal orthogonal group, and consists of the product of the orthogonal group with the group of dilations. If n is odd, these two subgroups do not intersect, and they are a direct product: $\operatorname{CO}(2k+1) = \operatorname{O}(2k+1) \times \mathbf{R}$, while if n is even, these subgroups intersect in $\pm 1$, so this is not a direct product, but it is a direct product with the subgroup of dilation by a positive scalar: $\operatorname{CO}(2k) = \operatorname{O}(2k) \times \mathbf{R}^+$. Similarly one can define CSO(n); note that this is always :$\operatorname{CSO}(n) := \operatorname{CO}(n) \cap \operatorname{GL}_+(n) = \operatorname{SO}(n) \times \mathbf{R}^+$. Over the complex number field Over the field C of complex numbers, O(n,C) and SO(n,C) are complex Lie groups of dimension n(n − 1)/2 over C (which means the dimension over R is twice that). O(n,C) has two connected components, and SO(n,C) is the connected component containing the identity matrix. For n ≥ 2 these groups are noncompact. Just as in the real case SO(n,C) is not simply connected. For n > 2 the fundamental group of SO(n,C) is cyclic of order 2 whereas the fundamental group of SO(2,C) is infinite cyclic. The complex Lie algebra associated to O(n,C) and SO(n,C) consists of the skew-symmetric complex n-by-n matrices, with the Lie bracket given by the commutator. Topology Low dimensional The low dimensional (real) orthogonal groups are familiar spaces: $\begin{align} \mbox{O}(1) &= \left\{\pm 1\right\} = S^0\\ \mbox{SO}(1) &= \left\{1\right\} = *\\ \mbox{SO}(2) &= S^1\\ \mbox{SO}(3) &= \mathbf{RP}^3. \end{align}$ The group SO(4) is double covered by $\mbox{SU}(2)\times \mbox{SU}(2)=S^3\times S^3$. There are numerous charts on SO(3), due to the importance of 3-dimensional rotations in engineering applications. Here Sn denotes the n-dimensional sphere, RPn the n-dimensional real projective space, and SU(n) the special unitary group of degree n. Homotopy groups The homotopy groups of the orthogonal group are related to homotopy groups of spheres, and thus are in general hard to compute. However, one can compute the homotopy groups of the stable orthogonal group (aka the infinite orthogonal group), defined as the direct limit of the sequence of inclusions $\mbox{O}(0) \subset \mbox{O}(1)\subset \mbox{O}(2)\subset\cdots\subset O = \bigcup_{k=0}^\infty \mbox{O}(k)$ (as the inclusions are all closed inclusions, hence cofibrations, this can also be interpreted as a union). Sn is a homogeneous space for O(n + 1), and one has the following fiber bundle: $\mbox{O}(n) \to \mbox{O}(n+1) \to S^n,$ which can be understood as "The orthogonal group O(n + 1) acts transitively on the unit sphere Sn, and the stabilizer of a point (thought of as a unit vector) is the orthogonal group of the perpendicular complement, which is an orthogonal group one dimension lower". The map $\mbox{O}(n) \to \mbox{O}(n+1)$ is the natural inclusion. Thus the inclusion $\mbox{O}(n) \to \mbox{O}(n+1)$ is (n − 1)-connected, so the homotopy groups stabilize, and πk(O) = πk(O(n)) for n > k + 1: thus the homotopy groups of the stable space equal the lower homotopy groups of the unstable spaces. Via Bott periodicity, $\Omega^8 O \simeq O$, thus the homotopy groups of O are 8-fold periodic, meaning πk + 8O = πkO, and one needs only to compute the lower 8 homotopy groups to compute them all. $\begin{align} \pi_0 O &= \mathbf Z/2\\ \pi_1 O &= \mathbf Z/2\\ \pi_2 O &= 0\\ \pi_3 O &= \mathbf Z\\ \pi_4 O &= 0\\ \pi_5 O &= 0\\ \pi_6 O &= 0\\ \pi_7 O &= \mathbf Z\\ \end{align}$ Relation to KO-theory Via the clutching construction, homotopy groups of the stable space O are identified with stable vector bundles on spheres (up to isomorphism), with a dimension shift of 1: πkO = πk + 1BO. Setting $KO = BO \times \mathbf Z = \Omega^{-1} O \times \mathbf Z$ (to make π0 fit into the periodicity), one obtains: $\begin{align} \pi_0 KO &= \mathbf Z\\ \pi_1 KO &= \mathbf Z/2\\ \pi_2 KO &= \mathbf Z/2\\ \pi_3 KO &= 0\\ \pi_4 KO &= \mathbf Z\\ \pi_5 KO &= 0\\ \pi_6 KO &= 0\\ \pi_7 KO &= 0.\\ \end{align}$ Computation and Interpretation of homotopy groups Low-dimensional groups The first few homotopy groups can be calculated by using the concrete descriptions of low-dimensional groups. $\pi_0(O) = \pi_0(\mbox{O}(1)) = \mathbf Z/2$ from orientation-preserving/reversing (this class survives to O(2) and hence stably) $\mbox{SO}(3) = \mathbf{RP}^3 = S^3/(\mathbf Z/2)$ yields $\pi_1(O) = \pi_1(\mbox{SO}(3)) = \mathbf Z/2$, which is spin π2(O) = π2(SO(3)) = 0, which surjects onto π2(SO(4)); this latter thus vanishes. Lie groups From general facts about Lie groups, π2G always vanishes, and π3G is free (free abelian). Vector bundles From the vector bundle point of view, π0(KO) is vector bundles over S0, which is two points. Thus over each point, the bundle is trivial, and the non-triviality of the bundle is the difference between the dimensions of the vector spaces over the two points, so $\pi_0(KO) = \mathbf Z$ is dimension. Loop spaces Using concrete descriptions of the loop spaces in Bott periodicity, one can interpret higher homotopy of O as lower homotopy of simple to analyze spaces. Using π0, O and O/U have two components, $KO = BO \times \mathbf Z$ and $KSp = BSp \times \mathbf Z$ have $\mathbf Z$ components, and the rest are connected. Interpretation of homotopy groups In a nutshell:[2] $\pi_0(KO) = \mathbf Z$ is dimension $\pi_1(KO) = \mathbf Z/2$ is orientation $\pi_2(KO) = \mathbf Z/2$ is spin $\pi_4(KO) = \mathbf Z$ is topological quantum field theory. Let $F = \mathbf R, \mathbf C, \mathbf H, \mathbf O$, and let LF be the tautological line bundle over the projective line $\mathbf{FP}^1$, and [LF] its class in K-theory. Noting that $\mathbf{RP}^1 = S^1, \mathbf{CP}^1 = S^2, \mathbf{HP}^1 = S^3, \mathbf{OP}^1 = S^7$, these yield vector bundles over the corresponding spheres, and π1(KO) is generated by $[L_{\mathbf R}]$ π2(KO) is generated by $[L_{\mathbf C}]$ π4(KO) is generated by $[L_{\mathbf H}]$ π8(KO) is generated by $[L_{\mathbf O}].$ From the point of view of symplectic geometry, $\pi_0(KO) \cong \pi_8(KO) = \mathbf Z$ can be interpreted as the Maslov index, thinking of it as the fundamental group of the stable Lagrangian Grassmannian π1(U / O), as $U/O \simeq \Omega^7(KO),$ so π1(U / O) = π1 + 7(KO). Over finite fields Orthogonal groups can also be defined over finite fields $\mathbf{F}_q$, where q is a power of a prime p. When defined over such fields, they come in two types in even dimension: O + (2n,q) and O − (2n,q); and one type in odd dimension: O(2n + 1,q). If V is the vector space on which the orthogonal group G acts, it can be written as a direct orthogonal sum as follows: $V = L_1 \oplus L_2 \oplus \cdots \oplus L_m \oplus W,$ where Li are hyperbolic lines and W contains no singular vectors. If W = 0, then G is of plus type. If W = < w > then G has odd dimension. If W has dimension 2, G is of minus type. In the special case where n = 1, $O^\epsilon(2, q)$ is a dihedral group of order $2(q - \epsilon)$. We have the following formulas for the order of these groups, O(n,q) = { A in GL(n,q) : A·At=I }, when the characteristic is greater than two $|O(2n+1,q)|=2q^n\prod_{i=0}^{n-1}(q^{2n}-q^{2i}).$ If −1 is a square in $\mathbf{F}_q$ $|O(2n,q)|=2(q^n-1)\prod_{i=1}^{n-1}(q^{2n}-q^{2i}).$ If −1 is a nonsquare in $\mathbf{F}_q$ $|O(2n,q)|=2(q^n+(-1)^{n+1})\prod_{i=1}^{n-1}(q^{2n}-q^{2i}).$ The Dickson invariant For orthogonal groups, the Dickson invariant is a homomorphism from the orthogonal group to Z/2Z, and is 0 or 1 depending on whether an element is the product of an even or odd number of reflections. More concretely, the Dickson invariant can be defined as $D(f)=\operatorname{rank} (I-f) \mod 2$ where I is the identity (Taylor 1992, Theorem 11.43). Over fields that are not of characteristic 2 it is equivalent to the determinant: the determinant is −1 to the power of the Dickson invariant. Over fields of characteristic 2, the determinant is always 1, so the Dickson invariant gives no extra information. The special orthogonal group is the kernel of the Dickson invariant and usually has index 2 in O(n,F).[3] When the characteristic of F is not 2, the Dickson Invariant is 0 whenever the determinant is 1. Thus when the characteristic is not 2, SO(n,F) is commonly defined to be the elements of O(n,F) with determinant 1. Each element in O(n,F) has determinant −1 or 1. Thus in characteristic 2, the determinant is always 1. The Dickson invariant can also be defined for Clifford groups and Pin groups in a similar way (in all dimensions). Orthogonal groups of characteristic 2 Over fields of characteristic 2 orthogonal groups often behave differently. This section lists some of the differences. Traditionally these groups are known as the hypoabelian groups but this term is no longer used for these groups. Any orthogonal group over any field is generated by reflections, except for a unique example where the vector space is 4 dimensional over the field with 2 elements and the Witt index is 2.[4] Note that a reflection in characteristic two has a slightly different definition. In characteristic two, the reflection orthogonal to a vector u takes a vector v to v+B(v,u)/Q(u)·u where B is the bilinear form and Q is the quadratic form associated to the orthogonal geometry. Compare this to the Householder reflection of odd characteristic or characteristic zero, which takes v to v − 2·B(v,u)/Q(u)·u. The center of the orthogonal group usually has order 1 in characteristic 2, rather than 2, since I = − I. In odd dimensions 2n+1 in characteristic 2, orthogonal groups over perfect fields are the same as symplectic groups in dimension 2n. In fact the symmetric form is alternating in characteristic 2, and as the dimension is odd it must have a kernel of dimension 1, and the quotient by this kernel is a symplectic space of dimension 2n, acted upon by the orthogonal group. In even dimensions in characteristic 2 the orthogonal group is a subgroup of the symplectic group, because the symmetric bilinear form of the quadratic form is also an alternating form. The spinor norm The spinor norm is a homomorphism from an orthogonal group over a field F to F*/F*2, the multiplicative group of the field F up to square elements, that takes reflection in a vector of norm n to the image of n in F*/F*2. For the usual orthogonal group over the reals it is trivial, but it is often non-trivial over other fields, or for the orthogonal group of a quadratic form over the reals that is not positive definite. Galois cohomology and orthogonal groups In the theory of Galois cohomology of algebraic groups, some further points of view are introduced. They have explanatory value, in particular in relation with the theory of quadratic forms; but were for the most part post hoc, as far as the discovery of the phenomena is concerned. The first point is that quadratic forms over a field can be identified as a Galois H1, or twisted forms (torsors) of an orthogonal group. As an algebraic group, an orthogonal group is in general neither connected nor simply-connected; the latter point brings in the spin phenomena, while the former is related to the discriminant. The 'spin' name of the spinor norm can be explained by a connection to the spin group (more accurately a pin group). This may now be explained quickly by Galois cohomology (which however postdates the introduction of the term by more direct use of Clifford algebras). The spin covering of the orthogonal group provides a short exact sequence of algebraic groups. $1 \rightarrow \mu_2 \rightarrow \mathrm{Pin}_V \rightarrow O_V \rightarrow 1$ Here μ2 is the algebraic group of square roots of 1; over a field of characteristic not 2 it is roughly the same as a two-element group with trivial Galois action. The connecting homomorphism from H0(OV), which is simply the group OV(F) of F-valued points, to H1(μ2) is essentially the spinor norm, because H1(μ2) is isomorphic to the multiplicative group of the field modulo squares. There is also the connecting homomorphism from H1 of the orthogonal group, to the H2 of the kernel of the spin covering. The cohomology is non-abelian, so that this is as far as we can go, at least with the conventional definitions. Related groups The orthogonal groups and special orthogonal groups have a number of important subgroups, supergroups, quotient groups, and covering groups. These are listed below. The inclusions $O(n) \subset U(n) \subset Sp(n)=USp(2n)$ and $USp(n) \subset U(n) \subset O(2n)$ are part of a sequence of 8 inclusions used in a geometric proof of the Bott periodicity theorem, and the corresponding quotient spaces are symmetric spaces of independent interest – for example, U(n) / O(n) is the Lagrangian Grassmannian. Lie subgroups In physics, particularly in the areas of Kaluza–Klein compactification, it is important to find out the subgroups of the orthogonal group. The main ones are: $O(n) \supset O(n-1)$ – preserves an axis $O(2n) \supset U(n) \supset SU(n)$ – U(n) are those that preserve a compatible complex structure or a compatible symplectic structure – see 2-out-of-3 property; SU(n) also preserves a complex orientation. $O(2n) \supset USp(n)$ $O(7) \supset G_2$ Lie supergroups The orthogonal group O(n) is also an important subgroup of various Lie groups: $U(n) \supset SU(n) \supset O(n)$ $USp(2n) \supset O(n)$ $G_2 \supset O(3)$ $F_4 \supset O(9)$ $E_6 \supset O(10)$ $E_7 \supset O(12)$ $E_8 \supset O(16)$ Discrete subgroups As the orthogonal group is compact, discrete subgroups are equivalent to finite subgroups.[note 2] These subgroups are known as point group and can be realized as the symmetry groups of polytopes. A very important class of examples are the finite Coxeter groups, which include the symmetry groups of regular polytopes. Dimension 3 is particularly studied – see point groups in three dimensions, polyhedral groups, and list of spherical symmetry groups. In 2 dimensions, the finite groups are either cyclic or dihedral – see point groups in two dimensions. Other finite subgroups include: Permutation matrices (the Coxeter group An) Signed permutation matrices (the Coxeter group Bn); also equals the intersection of the orthogonal group with the integer matrices.[note 3] Covering and quotient groups The orthogonal group is neither simply connected nor centerless, and thus has both a covering group and a quotient group, respectively: Two covering Pin groups, Pin+(n) → O(n) and Pin−(n) → O(n), The quotient projective orthogonal group, O(n) → PO(n). These are all 2-to-1 covers. For the special orthogonal group, the corresponding groups are: Spin group, Spin(n) → SO(n), Projective special orthogonal group, SO(n) → PSO(n). Spin is a 2-to-1 cover, while in even dimension, PSO(2k) is a 2-to-1 cover, and in odd dimension PSO(2k+1) is a 1-to-1 cover, i.e., isomorphic to SO(2k+1). These groups, Spin(n), SO(n), and PSO(n) are Lie group forms of the compact special orthogonal Lie algebra, $\mathfrak{so}_n(\mathbf{R})$ – Spin is the simply connected form, while PSO is the centerless form, and SO is in general neither.[note 4] In dimension 3 and above these are the covers and quotients, while dimension 2 and below are somewhat degenerate; see specific articles for details. Applications to string theory The group O(10) is of special importance in superstring theory because it is the symmetry group of 10 dimensional space-time. Principal homogeneous space: Stiefel manifold Main article: Stiefel manifold The principal homogeneous space for the orthogonal group O(n) is the Stiefel manifold $V_n(\mathbf{R}^n)$ of orthonormal bases (orthonormal n-frames). In other words, the space of orthonormal bases is like the orthogonal group, but without a choice of base point: given an orthogonal space, there is no natural choice of orthonormal basis, but once one is given one, there is a one-to-one correspondence between bases and the orthogonal group. Concretely, a linear map is determined by where it sends a basis: just as an invertible map can take any basis to any other basis, an orthogonal map can take any orthogonal basis to any other orthogonal basis. The other Stiefel manifolds $V_k(\mathbf{R}^n)$ for k < n of incomplete orthonormal bases (orthonormal k-frames) are still homogeneous spaces for the orthogonal group, but not principal homogeneous spaces: any k-frame can be taken to any other k-frame by an orthogonal map, but this map is not uniquely determined. See also Specific transforms Coordinate rotations and reflections Reflection through the origin Specific groups rotation group, SO(3,R) SO(8) Related groups indefinite orthogonal group unitary group symplectic group Lists of groups list of finite simple groups list of simple Lie groups Notes ^ The analogy is stronger: Weyl groups, a class of (representations of) Coxeter groups, can be considered as simple algebraic groups over the field with one element, and there are a number of analogies between algebraic groups and vector spaces on the one hand, and Weyl groups and sets on the other. ^ Infinite subsets of a compact space have an accumulation point and are not discrete. ^ $O(n) \cap GL(n,\mathbf{Z})$ equals the signed permutation matrices because an integer vector of norm 1 must have a single non-zero entry, which must be ±1 (if it has two non-zero entries or a larger entry, the norm will be larger than 1), and in an orthogonal matrix these entries must be in different coordinates, which is exactly the signed permutation matrices. ^ In odd dimension, SO(2k+1) $\cong$ PSO(2k+1) is centerless (but not simply connected), while in even dimension SO(2k) is neither centerless nor simply connected. References ^ Away from 2, it is equivalent to use bilinear forms or quadratic forms, but at 2 these differ – notably in characteristic 2, but also when generalizing to rings where 2 is not invertible, most significantly the integers, where the notions of even and odd quadratic forms arise. ^ John Baez "This Week's Finds in Mathematical Physics" week 105 ^ (Taylor 1992, page 160) ^ (Grove 2002, Theorem 6.6 and 14.16) Grove, Larry C. (2002), Classical groups and geometric algebra, Graduate Studies in Mathematics, 39, Providence, R.I.: American Mathematical Society, ISBN 978-0-8218-2019-3, MR1859189  Taylor, Donald E. (1992), The Geometry of the Classical Groups, 9, Berlin: Heldermann Verlag, ISBN 3-88538-009-9, MR1189139  External links John Baez "This Week's Finds in Mathematical Physics" week 105 John Baez on Octonions (Italian) n-dimensional Special Orthogonal Group parametrization Wikimedia Foundation. 2010. Игры ⚽ Поможем написать реферат Laurence Tomson Pete Fountain Look at other dictionaries: orthogonal group — ortogonalioji grupė statusas T sritis fizika atitikmenys: angl. orthogonal group vok. orthogonale Gruppe, f rus. ортогональная группа, f pranc. groupe orthogonal, m …   Fizikos terminų žodynas Indefinite orthogonal group — In mathematics, the indefinite orthogonal group, O( p , q ) is the Lie group of all linear transformations of a n = p + q dimensional real vector space which leave invariant a nondegenerate, symmetric bilinear form of signature ( p , q ). The… …   Wikipedia Orthogonal matrix — In linear algebra, an orthogonal matrix (less commonly called orthonormal matrix[1]), is a square matrix with real entries whose columns and rows are orthogonal unit vectors (i.e., orthonormal vectors). Equivalently, a matrix Q is orthogonal if… …   Wikipedia Group of Lie type — In mathematics, a group of Lie type G(k) is a (not necessarily finite) group of rational points of a reductive linear algebraic group G with values in the field k. Finite groups of Lie type form the bulk of nonabelian finite simple groups.… …   Wikipedia Group (mathematics) — This article covers basic notions. For advanced topics, see Group theory. The possible manipulations of this Rubik s Cube form a group. In mathematics, a group is an algebraic structure consisting of a set together with an operation that combines …   Wikipedia Group action — This article is about the mathematical concept. For the sociology term, see group action (sociology). Given an equilateral triangle, the counterclockwise rotation by 120° around the center of the triangle acts on the set of vertices of the… …   Wikipedia Group extension — In mathematics, a group extension is a general means of describing a group in terms of a particular normal subgroup and quotient group. If Q and N are two groups, then G is an extension of Q by N if there is a short exact sequence:1 ightarrow N… …   Wikipedia General linear group — Group theory Group theory …   Wikipedia Lorentz group — Group theory Group theory …   Wikipedia Orthogonal frequency-division multiplexing — Passband modulation v · d · e Analog modulation AM · …   Wikipedia 18+ © Academic, 2000-2024 Contact us: Technical Support, Advertising Dictionaries export, created on PHP, Joomla, Drupal, WordPress, MODx. Mark and share Search through all dictionaries Translate… Search Internet Share the article and excerpts Direct link … Do a right-click on the link above and select “Copy Link”