- Fundamental domain
In

geometry , the**fundamental domain**of asymmetry group of an object or pattern is a part of the pattern, as small as possible, which, based on thesymmetry , determines the whole object or pattern. The set of orbits of the symmetry group define a partitioning of space. Each partition consists of points which, based on the symmetry, have equal properties, e.g., for a color pattern on the plane, have the same color. A fundamental domain is a set of representatives of these orbits. This is not unique, but typically a convenient connected part of space is chosen.**Hints at general definition**Given an action of a group "G" on a

topological space "X" byhomeomorphism s, a**fundamental domain**(also called**fundamental region**) for this action is a set "D" of representatives for the orbits. It is usually required to be a reasonbly nice set topologically, in one of several precisely defined ways. One typical condition is that "D" is "almost" an open set, in the sense that "D" is thesymmetric difference of an open set in "G" with a set ofmeasure zero , for a certain (quasi)invariant measure on "X". A fundamental domain always contains afree regular set "U", anopen set moved around by "G" intodisjoint copies, and nearly as good as "D" in representing the orbits. Frequently "D" is required to be a complete set of coset representatives with some repetitions, but the repeated part has measure zero. This is a typical situation inergodic theory . If a fundamental domain is used to calculate anintegral on "X"/"G", sets of measure zero do not matter.For example, when "X" is

Euclidean space **R**^{"n"}of dimension "n", and "G" is the lattice**Z**^{"n"}acting on it by translations, the quotient "X"/"G" is the "n"-dimensionaltorus . A fundamental domain "D" here can be taken to be[0,1) ^{"n"}, which differs from the open set (0,1)^{"n"}by a set of measure zero, or the closed unit cube[0,1] ^{"n"}, whose boundary consists of the points whose orbit has more than one representative in "D".**Examples**Examples in the three-dimensional Euclidean space

**R**^{3}.

*for "n"-fold rotation: an orbit is either a set of "n" points around the axis, or a single point on the axis; the fundamental domain is a sector

*for reflection in a plane: an orbit is either a set of 2 points, one on each side of the plane, or a single point in the plane; the fundamental domain is a half-space bounded by that plane

*for inversion in a point: an orbit is a set of 2 points, one on each side of the center, except for one orbit, consisting of the center only; the fundamental domain is a half-space bounded by any plane through the center

*for 180° rotation about a line: an orbit is either a set of 2 points opposite to each other with respect to the axis, or a single point on the axis; the fundamental domain is a half-space bounded by any plane through the line

*for discretetranslational symmetry in one direction: the orbits are translates of a 1D lattice in the direction of the translation vector; the fundamental domain is an infinite slab

*for discrete translational symmetry in two directions: the orbits are translates of a 2D lattice in the plane through the translation vectors; the fundamental domain is an infinite bar withparallelogram matic cross section

*for discrete translational symmetry in three directions: the orbits are translates of the lattice; the fundamental domain is aprimitive cell which is e.g. aparallelepiped , or aWigner-Seitz cell , also called Voronoi cell/diagram.In the case of translational symmetry combined with other symmetries, the fundamental domain is part of the primitive cell. For example, for

wallpaper group s the fundamental domain is a factor 1, 2, 3, 4, 6, 8, or 12 smaller than the primitive cell.**Fundamental domain for the modular group**The existence and description of a fundamental domain is in general something requiring painstaking work to establish. The diagram to the right shows part of the construction of the fundamental domain for the action of the

modular group Γ on theupper half-plane "H".This famous diagram appears in all classical books on

elliptic modular function s. (It was probably well known toC. F. Gauss , who dealt with fundamental domains in the guise of thereduction theory of quadratic forms .) Here, each triangular region (bounded by the blue lines) is afree regular set of the action of Γ on "H". The boundaries (the blue lines) are not a part of the free regular sets. To construct a fundamental domain of "H"/Γ, one must also consider how to assign points on the boundary, being careful not to double-count such points. Thus, the free regular set in this example is:$U\; =\; left\{\; z\; in\; H:\; left|\; z\; ight|\; >\; 1,,\; left|\; ,mbox\{Re\}(z)\; ,\; ight|\; <\; frac\{1\}\{2\}\; ight\}.$

The fundamental domain is built by adding the boundary on the left plus half the arc on the bottom:

:$D=Ucupleft\{\; z\; in\; H:\; left|\; z\; ight|\; geq\; 1,,\; mbox\{Re\}(z)=frac\{-1\}\{2\}\; ight\}\; cup\; left\{\; z\; in\; H:\; left|\; z\; ight|\; =\; 1,,\; frac\{-1\}\{2\}\{re\}(z)0\; ight\}.\; math>$

The choice of which points of the boundary to include as a part of the fundamental domain is arbitrary, and varies from author to author.

The core difficulty of defining the fundamental domain lies not so much with the definition of the set "per se", but rather with how to treat integrals over the fundamental domain, when integrating functions with poles and zeros on the boundary of the domain.

**ee also***

Free regular set

*Fundamental polygon

*Brillouin zone

*Fundamental pair of periods

*Petersson inner product

*Cusp neighborhood **External links***

*Wikimedia Foundation.
2010.*

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