In mathematics, the Riemann sphere, named after Bernhard Riemann, ^{[1]} is a model of the extended complex plane (also called the closed complex plane): the complex plane plus one point at infinity. This extended plane represents the extended complex numbers, that is, the complex numbers plus a value for infinity. With the Riemann model, the point is near to very large numbers, just as the point is near to very small numbers.
The extended complex numbers are useful in complex analysis because they allow for division by zero in some circumstances, in a way that makes expressions such as wellbehaved. For example, any rational function on the complex plane can be extended to a holomorphic function on the Riemann sphere, with the poles of the rational function mapping to infinity. More generally, any meromorphic function can be thought of as a holomorphic function whose codomain is the Riemann sphere.
In geometry, the Riemann sphere is the prototypical example of a Riemann surface, and is one of the simplest complex manifolds. In projective geometry, the sphere is an example of a complex projective space and can be thought of as the complex projective line , the projective space of all complex lines in . As with any compact Riemann surface, the sphere may also be viewed as a projective algebraic curve, making it a fundamental example in algebraic geometry. It also finds utility in other disciplines that depend on analysis and geometry, such as the Bloch sphere of quantum mechanics and in other branches of physics.
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Transcription
Extended complex numbers
The extended complex numbers consist of the complex numbers together with . The set of extended complex numbers may be written as , and is often denoted by adding some decoration to the letter , such as
The notation has also seen use, but as this notation is also used for the punctured plane , it can lead to ambiguity.^{[2]}
Geometrically, the set of extended complex numbers is referred to as the Riemann sphere (or extended complex plane).
Arithmetic operations
Addition of complex numbers may be extended by defining, for ,
for any complex number , and multiplication may be defined by
for all nonzero complex numbers , with . Note that and are left undefined. Unlike the complex numbers, the extended complex numbers do not form a field, since does not have an additive nor multiplicative inverse. Nonetheless, it is customary to define division on by
for all nonzero complex numbers with and . The quotients and are left undefined.
Rational functions
Any rational function (in other words, is the ratio of polynomial functions and of with complex coefficients, such that and have no common factor) can be extended to a continuous function on the Riemann sphere. Specifically, if is a complex number such that the denominator is zero but the numerator is nonzero, then can be defined as . Moreover, can be defined as the limit of as , which may be finite or infinite.
The set of complex rational functions—whose mathematical symbol is —form all possible holomorphic functions from the Riemann sphere to itself, when it is viewed as a Riemann surface, except for the constant function taking the value everywhere. The functions of form an algebraic field, known as the field of rational functions on the sphere.
For example, given the function
we may define , since the denominator is zero at , and since as . Using these definitions, becomes a continuous function from the Riemann sphere to itself.
As a complex manifold
As a onedimensional complex manifold, the Riemann sphere can be described by two charts, both with domain equal to the complex number plane . Let be a complex number in one copy of , and let be a complex number in another copy of . Identify each nonzero complex number of the first with the nonzero complex number of the second . Then the map
is called the transition map between the two copies of —the socalled charts—glueing them together. Since the transition maps are holomorphic, they define a complex manifold, called the Riemann sphere. As a complex manifold of 1 complex dimension (i.e. 2 real dimensions), this is also called a Riemann surface.
Intuitively, the transition maps indicate how to glue two planes together to form the Riemann sphere. The planes are glued in an "insideout" manner, so that they overlap almost everywhere, with each plane contributing just one point (its origin) missing from the other plane. In other words, (almost) every point in the Riemann sphere has both a value and a value, and the two values are related by . The point where should then have value ""; in this sense, the origin of the chart plays the role of in the chart. Symmetrically, the origin of the chart plays the role of in the chart.
Topologically, the resulting space is the onepoint compactification of a plane into the sphere. However, the Riemann sphere is not merely a topological sphere. It is a sphere with a welldefined complex structure, so that around every point on the sphere there is a neighborhood that can be biholomorphically identified with .
On the other hand, the uniformization theorem, a central result in the classification of Riemann surfaces, states that every simplyconnected Riemann surface is biholomorphic to the complex plane, the hyperbolic plane, or the Riemann sphere. Of these, the Riemann sphere is the only one that is a closed surface (a compact surface without boundary). Hence the twodimensional sphere admits a unique complex structure turning it into a onedimensional complex manifold.
As the complex projective line
The Riemann sphere can also be defined as the complex projective line. The points of the complex projective line can be defined as equivalence classes of nonnull vectors in the complex vector space : two nonnull vectors and are equivalent iff for some nonzero coefficient .
In this case, the equivalence class is written using projective coordinates. Given any point in the complex projective line, one of and must be nonzero, say . Then by the notion of equivalence, , which is in a chart for the Riemann sphere manifold.^{[3]}
This treatment of the Riemann sphere connects most readily to projective geometry. For example, any line (or smooth conic) in the complex projective plane is biholomorphic to the complex projective line. It is also convenient for studying the sphere's automorphisms, later in this article.
As a sphere
The Riemann sphere can be visualized as the unit sphere in the threedimensional real space . To this end, consider the stereographic projection from the unit sphere minus the point onto the plane which we identify with the complex plane by . In Cartesian coordinates and spherical coordinates on the sphere (with the zenith and the azimuth), the projection is
Similarly, stereographic projection from onto the plane identified with another copy of the complex plane by is written
The inverses of these two stereographic projections are maps from the complex plane to the sphere. The first inverse covers the sphere except the point , and the second covers the sphere except the point . The two complex planes, that are the domains of these maps, are identified differently with the plane , because an orientationreversal is necessary to maintain consistent orientation on the sphere.
The transition maps between coordinates and coordinates are obtained by composing one projection with the inverse of the other. They turn out to be and , as described above. Thus the unit sphere is diffeomorphic to the Riemann sphere.
Under this diffeomorphism, the unit circle in the chart, the unit circle in the chart, and the equator of the unit sphere are all identified. The unit disk is identified with the southern hemisphere , while the unit disk is identified with the northern hemisphere .
Metric
A Riemann surface does not come equipped with any particular Riemannian metric. The Riemann surface's conformal structure does, however, determine a class of metrics: all those whose subordinate conformal structure is the given one. In more detail: The complex structure of the Riemann surface does uniquely determine a metric up to conformal equivalence. (Two metrics are said to be conformally equivalent if they differ by multiplication by a positive smooth function.) Conversely, any metric on an oriented surface uniquely determines a complex structure, which depends on the metric only up to conformal equivalence. Complex structures on an oriented surface are therefore in onetoone correspondence with conformal classes of metrics on that surface.
Within a given conformal class, one can use conformal symmetry to find a representative metric with convenient properties. In particular, there is always a complete metric with constant curvature in any given conformal class.
In the case of the Riemann sphere, the Gauss–Bonnet theorem implies that a constantcurvature metric must have positive curvature . It follows that the metric must be isometric to the sphere of radius in via stereographic projection. In the chart on the Riemann sphere, the metric with is given by
In real coordinates , the formula is
Up to a constant factor, this metric agrees with the standard Fubini–Study metric on complex projective space (of which the Riemann sphere is an example).
Up to scaling, this is the only metric on the sphere whose group of orientationpreserving isometries is 3dimensional (and none is more than 3dimensional); that group is called . In this sense, this is by far the most symmetric metric on the sphere. (The group of all isometries, known as , is also 3dimensional, but unlike is not a connected space.)
Conversely, let denote the sphere (as an abstract smooth or topological manifold). By the uniformization theorem there exists a unique complex structure on up to conformal equivalence. It follows that any metric on is conformally equivalent to the round metric. All such metrics determine the same conformal geometry. The round metric is therefore not intrinsic to the Riemann sphere, since "roundness" is not an invariant of conformal geometry. The Riemann sphere is only a conformal manifold, not a Riemannian manifold. However, if one needs to do Riemannian geometry on the Riemann sphere, the round metric is a natural choice (with any fixed radius, though radius is the simplest and most common choice). That is because only a round metric on the Riemann sphere has its isometry group be a 3dimensional group. (Namely, the group known as , a continuous ("Lie") group that is topologically the 3dimensional projective space .)
Automorphisms
The study of any mathematical object is aided by an understanding of its group of automorphisms, meaning the maps from the object to itself that preserve the essential structure of the object. In the case of the Riemann sphere, an automorphism is an invertible conformal map (i.e. biholomorphic map) from the Riemann sphere to itself. It turns out that the only such maps are the Möbius transformations. These are functions of the form
where , , , and are complex numbers such that . Examples of Möbius transformations include dilations, rotations, translations, and complex inversion. In fact, any Möbius transformation can be written as a composition of these.
The Möbius transformations are homographies on the complex projective line. In projective coordinates, the transformation f can be written
Thus the Möbius transformations can be described as twobytwo complex matrices with nonzero determinant. Since they act on projective coordinates, two matrices yield the same Möbius transformation if and only if they differ by a nonzero factor. The group of Möbius transformations is the projective linear group .
If one endows the Riemann sphere with the Fubini–Study metric, then not all Möbius transformations are isometries; for example, the dilations and translations are not. The isometries form a proper subgroup of , namely . This subgroup is isomorphic to the rotation group , which is the group of symmetries of the unit sphere in (which, when restricted to the sphere, become the isometries of the sphere).
Applications
In complex analysis, a meromorphic function on the complex plane (or on any Riemann surface, for that matter) is a ratio of two holomorphic functions and . As a map to the complex numbers, it is undefined wherever is zero. However, it induces a holomorphic map to the complex projective line that is welldefined even where . This construction is helpful in the study of holomorphic and meromorphic functions. For example, on a compact Riemann surface there are no nonconstant holomorphic maps to the complex numbers, but holomorphic maps to the complex projective line are abundant.
The Riemann sphere has many uses in physics. In quantum mechanics, points on the complex projective line are natural values for photon polarization states, spin states of massive particles of spin , and 2state particles in general (see also Quantum bit and Bloch sphere). The Riemann sphere has been suggested as a relativistic model for the celestial sphere.^{[4]} In string theory, the worldsheets of strings are Riemann surfaces, and the Riemann sphere, being the simplest Riemann surface, plays a significant role. It is also important in twistor theory.
See also
 Conformal geometry
 Crossratio
 Dessin d'enfant
 Directed infinity
 Hopf bundle
 Möbius plane
 Parallel (operator) § Properties
 Projectively extended real line
 Smith chart
 Wheel theory
Notes
 ^ Riemann 1857.
 ^ "C^*". Archived from the original on October 8, 2021. Retrieved December 12, 2021.
 ^ Goldman 1999, p. 1.
 ^ Penrose 2007, pp. 428–430.
References
 Brown, James & Churchill, Ruel (1989). Complex Variables and Applications. New York: McGrawHill. ISBN 0070109052.
 Goldman, William Mark (1999). Complex Hyperbolic Geometry. Oxford : New York: Oxford University Press. ISBN 019853793X.
 Griffiths, Phillip & Harris, Joseph (1978). Principles of Algebraic Geometry. John Wiley & Sons. ISBN 0471327921.
 Penrose, Roger (2007). The Road to Reality. London: National Geographic Books. ISBN 9780679776314.
 Riemann, Bernhard (1857). "Theorie der Abel'schen Functionen" [Theory of Abelian functions]. Journal für die reine und angewandte Mathematik (in German). 54: 115–155.
 Rudin, Walter (1987). Real and Complex Analysis. New York: McGraw–Hill. ISBN 0071002766.
External links
 "Riemann sphere", Encyclopedia of Mathematics, EMS Press, 2001 [1994]
 Moebius Transformations Revealed, by Douglas N. Arnold and Jonathan Rogness (a video by two University of Minnesota professors explaining and illustrating Möbius transformations using stereographic projection from a sphere)