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・ Paippad Puthenkavu Bhagavathi Temple
・ Paipra
・ Paipra Radhakrishnan
・ PAIR
・ Pair
・ Pair (parliamentary convention)
・ PAIR (puncture-aspiration-injection-reaspiration)
・ Pair a Dice Found
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・ Pair by association
・ Pair Dadeni
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・ Pair Of Dice Paradise
・ Pair of Kings
Pair of pants (mathematics)
・ Pair of spaces
・ Pair potential
・ Pair production
・ Pair programming
・ Pair skating
・ Pair testing
・ Pair trawling
・ Pair-conversion
・ Pair-et-Grandrupt
・ Pair-instability supernova
・ Pair-rule gene
・ Paira
・ Pairagachha
・ Pairan


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Pair of pants (mathematics) : ウィキペディア英語版
Pair of pants (mathematics)

In mathematics, a pair of pants is a simple two-dimensional surface resembling a pair of pants: topologically, it is a sphere with three holes in it. Pairs of pants admit hyperbolic metrics, and their isometry class is determined by the lengths of the boundary curves (the cuff lengths), or dually the distances between the boundaries (the seam lengths).
In hyperbolic geometry all three holes are considered equivalent – no distinction is made between "legs" and "waist". In cobordism theory the holes are not equivalent – a pair of pants is a cobordism between one circle (the "waist") and two circles (the "legs").
== Hyperbolic geometry ==
In hyperbolic geometry, pairs of pants are sewn together, leg to leg, or leg to waist (there is no distinction between the legs and the waist), to create Riemann surfaces of arbitrary genus; conversely, Riemann surfaces can be cut into pairs of pants by cutting along closed geodesics. Because the "legs" can be twisted before being sewn together, there is a large amount of freedom in how the pants can be assembled. This ambiguity gives the Fenchel–Nielsen coordinates for the moduli space of the Riemann surface, which has complex dimension 3(''g'' − 1) = 3''g'' − 3 for ''g'' > 1.
Formally, a pair of pants consists of two hexagonal fundamental polygons stitched together at every other side. Topologically, a pair of pants is the two-sphere ''S''2 with three open disks removed, or equivalently the disk with two open disks removed. This is a deformation retract of the thrice-punctured sphere (a sphere with three points removed), though these are not homeomorphic – the thrice-punctured sphere is not compact, and has no boundary components. Geometrically, a thrice-punctured sphere corresponds to pants where the cuff length is zero – where instead of a boundary circle, one has a cusp – compare ideal triangle.
A pair of pants, as a (subset of a) thrice-punctured sphere, admits a hyperbolic structure, unlike the unpunctured or once or twice punctured spheres (sphere, plane, annulus), which admit positive curvature, zero curvature, and zero curvature, respectively – compare Little Picard theorem.
It is homotopy equivalent to the wedge sum of two circles, and thus has fundamental group isomorphic to the free group on two generators (one generator for each circle).
A pair of pants is analogous to a fattened up hyperbolic triangle, and is frequently so drawn schematically, with the seams as the sides and cuffs at vertices. Compare SSS and AAA congruence of hyperbolic triangles to pairs of pants being determined by seam length or cuff lengths.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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