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Hélène Esnault

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Algebraic geometry is a branch of mathematics which uses abstract algebraic techniques, mainly from commutative algebra , to solve geometrical problems . Classically, it studies zeros of multivariate polynomials ; the modern approach generalizes this in a few different aspects.

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114-553: Hélène Esnault (born 17 July 1953) is a French and German mathematician, specializing in algebraic geometry . Born in Paris, Esnault earned her PhD in 1976 from the University of Paris VII . She wrote her dissertation on Singularites rationnelles et groupes algebriques (Rational singularities and algebraic groups) under the direction of Lê Dũng Tráng . She did her habilitation at the University of Bonn in 1985, and pursued her studies at

228-403: A = 0 {\displaystyle x^{2}+y^{2}-a=0} is a circle if a > 0 {\displaystyle a>0} , but has no real points if a < 0 {\displaystyle a<0} . Real algebraic geometry also investigates, more broadly, semi-algebraic sets , which are the solutions of systems of polynomial inequalities. For example, neither branch of

342-456: A Fields medal , made new impacts in mathematics by using topological quantum field theory and string theory to make predictions and provide frameworks for new rigorous mathematics, which has resulted for example in the conjectural mirror symmetry and the Seiberg–Witten invariants . Riemannian geometry studies Riemannian manifolds , smooth manifolds with a Riemannian metric . This is

456-487: A directional derivative of a function from multivariable calculus is extended to the notion of a covariant derivative of a tensor . Many concepts of analysis and differential equations have been generalized to the setting of Riemannian manifolds. A distance-preserving diffeomorphism between Riemannian manifolds is called an isometry . This notion can also be defined locally , i.e. for small neighborhoods of points. Any two regular curves are locally isometric. However,

570-430: A field k . In classical algebraic geometry, this field was always the complex numbers C , but many of the same results are true if we assume only that k is algebraically closed . We consider the affine space of dimension n over k , denoted A ( k ) (or more simply A , when k is clear from the context). When one fixes a coordinate system, one may identify A ( k ) with k . The purpose of not working with k

684-497: A regular point , whose tangent is the line at infinity , while the point at infinity of the cubic curve is a cusp . Also, both curves are rational, as they are parameterized by x , and the Riemann-Roch theorem implies that the cubic curve must have a singularity, which must be at infinity, as all its points in the affine space are regular. Thus many of the properties of algebraic varieties, including birational equivalence and all

798-447: A vector bundle endomorphism (called an almost complex structure ) It follows from this definition that an almost complex manifold is even-dimensional. An almost complex manifold is called complex if N J = 0 {\displaystyle N_{J}=0} , where N J {\displaystyle N_{J}} is a tensor of type (2, 1) related to J {\displaystyle J} , called

912-595: A concept of distance expressed by means of a smooth positive definite symmetric bilinear form defined on the tangent space at each point. Riemannian geometry generalizes Euclidean geometry to spaces that are not necessarily flat, though they still resemble Euclidean space at each point infinitesimally, i.e. in the first order of approximation . Various concepts based on length, such as the arc length of curves, area of plane regions, and volume of solids all possess natural analogues in Riemannian geometry. The notion of

1026-403: A continuous function on a closed subset always extends to the ambient topological space. Just as with the regular functions on affine space, the regular functions on V form a ring, which we denote by k [ V ]. This ring is called the coordinate ring of V . Since regular functions on V come from regular functions on A , there is a relationship between the coordinate rings. Specifically, if

1140-403: A function to be polynomial (or regular) does not depend on the choice of a coordinate system in A . When a coordinate system is chosen, the regular functions on the affine n -space may be identified with the ring of polynomial functions in n variables over k . Therefore, the set of the regular functions on A is a ring, which is denoted k [ A ]. We say that a polynomial vanishes at

1254-409: A fundamental role in algebraic geometry. Nowadays, the projective space P of dimension n is usually defined as the set of the lines passing through a point, considered as the origin, in the affine space of dimension n + 1 , or equivalently to the set of the vector lines in a vector space of dimension n + 1 . When a coordinate system has been chosen in the space of dimension n + 1 , all

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1368-428: A manifold, as even the notion of a topological space had not been encountered, but he did propose that it might be possible to investigate or measure the properties of the metric of spacetime through the analysis of masses within spacetime, linking with the earlier observation of Euler that masses under the effect of no forces would travel along geodesics on surfaces, and predicting Einstein's fundamental observation of

1482-504: A new interpretation of Euler's theorem in terms of the principle curvatures, which is the modern form of the equation. The field of differential geometry became an area of study considered in its own right, distinct from the more broad idea of analytic geometry, in the 1800s, primarily through the foundational work of Carl Friedrich Gauss and Bernhard Riemann , and also in the important contributions of Nikolai Lobachevsky on hyperbolic geometry and non-Euclidean geometry and throughout

1596-461: A nondegenerate 2- form ω , called the symplectic form . A symplectic manifold is an almost symplectic manifold for which the symplectic form ω is closed: d ω = 0 . A diffeomorphism between two symplectic manifolds which preserves the symplectic form is called a symplectomorphism . Non-degenerate skew-symmetric bilinear forms can only exist on even-dimensional vector spaces, so symplectic manifolds necessarily have even dimension. In dimension 2,

1710-429: A point if evaluating it at that point gives zero. Let S be a set of polynomials in k [ A ]. The vanishing set of S (or vanishing locus or zero set ) is the set V ( S ) of all points in A where every polynomial in S vanishes. Symbolically, A subset of A which is V ( S ), for some S , is called an algebraic set . The V stands for variety (a specific type of algebraic set to be defined below). Given

1824-414: A regular function on V is the restriction of two functions f and g in k [ A ], then f  −  g is a polynomial function which is null on V and thus belongs to I ( V ). Thus k [ V ] may be identified with k [ A ]/ I ( V ). Using regular functions from an affine variety to A , we can define regular maps from one affine variety to another. First we will define a regular map from

1938-400: A regular map g from V to V ′ and a regular function f of k [ V ′], then f ∘ g ∈ k [ V ] . The map f → f ∘ g is a ring homomorphism from k [ V ′] to k [ V ]. Conversely, every ring homomorphism from k [ V ′] to k [ V ] defines a regular map from V to V ′. This defines an equivalence of categories between the category of algebraic sets and the opposite category of

2052-436: A root of the polynomial x + 1 , projective space is obtained by adding in appropriate points "at infinity", points where parallel lines may meet. To see how this might come about, consider the variety V ( y − x ) . If we draw it, we get a parabola . As x goes to positive infinity, the slope of the line from the origin to the point ( x ,  x ) also goes to positive infinity. As x goes to negative infinity,

2166-477: A subset U of A , can one recover the set of polynomials which generate it? If U is any subset of A , define I ( U ) to be the set of all polynomials whose vanishing set contains U . The I stands for ideal : if two polynomials f and g both vanish on U , then f + g vanishes on U , and if h is any polynomial, then hf vanishes on U , so I ( U ) is always an ideal of the polynomial ring k [ A ]. Two natural questions to ask are: The answer to

2280-515: A symplectic manifold is just a surface endowed with an area form and a symplectomorphism is an area-preserving diffeomorphism. The phase space of a mechanical system is a symplectic manifold and they made an implicit appearance already in the work of Joseph Louis Lagrange on analytical mechanics and later in Carl Gustav Jacobi 's and William Rowan Hamilton 's formulations of classical mechanics . By contrast with Riemannian geometry, where

2394-521: A theorem expressing the curvature of a space curve on a surface in terms of the principal curvatures, known as Euler's theorem . Later in the 1700s, the new French school led by Gaspard Monge began to make contributions to differential geometry. Monge made important contributions to the theory of plane curves, surfaces, and studied surfaces of revolution and envelopes of plane curves and space curves. Several students of Monge made contributions to this same theory, and for example Charles Dupin provided

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2508-419: A variety into affine space: Let V be a variety contained in A . Choose m regular functions on V , and call them f 1 , ..., f m . We define a regular map f from V to A by letting f = ( f 1 , ..., f m ) . In other words, each f i determines one coordinate of the range of f . If V ′ is a variety contained in A , we say that f is a regular map from V to V ′ if

2622-470: A well-known standard definition of metric and parallelism. In Riemannian geometry , the Levi-Civita connection serves a similar purpose. More generally, differential geometers consider spaces with a vector bundle and an arbitrary affine connection which is not defined in terms of a metric. In physics, the manifold may be spacetime and the bundles and connections are related to various physical fields. From

2736-423: A year later Tullio Levi-Civita and Gregorio Ricci-Curbastro produced their textbook systematically developing the theory of absolute differential calculus and tensor calculus . It was in this language that differential geometry was used by Einstein in the development of general relativity and pseudo-Riemannian geometry . The subject of modern differential geometry emerged from the early 1900s in response to

2850-459: Is a mathematical discipline that studies the geometry of smooth shapes and smooth spaces, otherwise known as smooth manifolds . It uses the techniques of differential calculus , integral calculus , linear algebra and multilinear algebra . The field has its origins in the study of spherical geometry as far back as antiquity . It also relates to astronomy , the geodesy of the Earth , and later

2964-401: Is a function F : T M → [ 0 , ∞ ) {\displaystyle F:\mathrm {T} M\to [0,\infty )} such that: Symplectic geometry is the study of symplectic manifolds . An almost symplectic manifold is a differentiable manifold equipped with a smoothly varying non-degenerate skew-symmetric bilinear form on each tangent space, i.e.,

3078-475: Is a price to pay in technical complexity: the intrinsic definitions of curvature and connections become much less visually intuitive. These two points of view can be reconciled, i.e. the extrinsic geometry can be considered as a structure additional to the intrinsic one. (See the Nash embedding theorem .) In the formalism of geometric calculus both extrinsic and intrinsic geometry of a manifold can be characterized by

3192-417: Is a rational curve, as it has the parametric equation which may also be viewed as a rational map from the line to the circle. The problem of resolution of singularities is to know if every algebraic variety is birationally equivalent to a variety whose projective completion is nonsingular (see also smooth completion ). It was solved in the affirmative in characteristic 0 by Heisuke Hironaka in 1964 and

3306-631: Is a system of generators of a polynomial ideal whose computation allows the deduction of many properties of the affine algebraic variety defined by the ideal. Given an ideal I defining an algebraic set V : Gröbner basis computations do not allow one to compute directly the primary decomposition of I nor the prime ideals defining the irreducible components of V , but most algorithms for this involve Gröbner basis computation. The algorithms which are not based on Gröbner bases use regular chains but may need Gröbner bases in some exceptional situations. Differential geometry Differential geometry

3420-445: Is a useful notion, which, similarly to the affine case, is defined as the set of the quotients of two homogeneous elements of the same degree in the homogeneous coordinate ring. Real algebraic geometry is the study of real algebraic varieties. The fact that the field of the real numbers is an ordered field cannot be ignored in such a study. For example, the curve of equation x 2 + y 2 −

3534-409: Is an affine variety, its coordinate ring is an integral domain and has thus a field of fractions which is denoted k ( V ) and called the field of the rational functions on V or, shortly, the function field of V . Its elements are the restrictions to V of the rational functions over the affine space containing V . The domain of a rational function f is not V but the complement of

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3648-416: Is called irreducible if it cannot be written as the union of two smaller algebraic sets. Any algebraic set is a finite union of irreducible algebraic sets and this decomposition is unique. Thus its elements are called the irreducible components of the algebraic set. An irreducible algebraic set is also called a variety . It turns out that an algebraic set is a variety if and only if it may be defined as

3762-412: Is given by all the smooth complex projective varieties . CR geometry is the study of the intrinsic geometry of boundaries of domains in complex manifolds . Conformal geometry is the study of the set of angle-preserving (conformal) transformations on a space. Differential topology is the study of global geometric invariants without a metric or symplectic form. Differential topology starts from

3876-473: Is intimately linked to the development of geometry more generally, of the notion of space and shape, and of topology , especially the study of manifolds . In this section we focus primarily on the history of the application of infinitesimal methods to geometry, and later to the ideas of tangent spaces , and eventually the development of the modern formalism of the subject in terms of tensors and tensor fields . The study of differential geometry, or at least

3990-657: Is one which defines some notion of size, distance, shape, volume, or other rigidifying structure. For example, in Riemannian geometry distances and angles are specified, in symplectic geometry volumes may be computed, in conformal geometry only angles are specified, and in gauge theory certain fields are given over the space. Differential geometry is closely related to, and is sometimes taken to include, differential topology , which concerns itself with properties of differentiable manifolds that do not rely on any additional geometric structure (see that article for more discussion on

4104-398: Is simply exponential in the number of the variables. A body of mathematical theory complementary to symbolic methods called numerical algebraic geometry has been developed over the last several decades. The main computational method is homotopy continuation . This supports, for example, a model of floating point computation for solving problems of algebraic geometry. A Gröbner basis

4218-423: Is sufficient only for developing analysis on the manifold, while doing geometry requires, in addition, some way to relate the tangent spaces at different points, i.e. a notion of parallel transport . An important example is provided by affine connections . For a surface in R , tangent planes at different points can be identified using a natural path-wise parallelism induced by the ambient Euclidean space, which has

4332-417: Is the Levi-Civita connection of g {\displaystyle g} . In this case, ( J , g ) {\displaystyle (J,g)} is called a Kähler structure , and a Kähler manifold is a manifold endowed with a Kähler structure. In particular, a Kähler manifold is both a complex and a symplectic manifold . A large class of Kähler manifolds (the class of Hodge manifolds )

4446-452: Is the Riemannian symmetric spaces , whose curvature is not necessarily constant. These are the closest analogues to the "ordinary" plane and space considered in Euclidean and non-Euclidean geometry . Pseudo-Riemannian geometry generalizes Riemannian geometry to the case in which the metric tensor need not be positive-definite . A special case of this is a Lorentzian manifold , which is

4560-490: Is the radical of the ideal generated by S . In more abstract language, there is a Galois connection , giving rise to two closure operators ; they can be identified, and naturally play a basic role in the theory; the example is elaborated at Galois connection. For various reasons we may not always want to work with the entire ideal corresponding to an algebraic set U . Hilbert's basis theorem implies that ideals in k [ A ] are always finitely generated. An algebraic set

4674-597: Is the following part of Hilbert's sixteenth problem : Decide which respective positions are possible for the ovals of a nonsingular plane curve of degree 8. One may date the origin of computational algebraic geometry to meeting EUROSAM'79 (International Symposium on Symbolic and Algebraic Manipulation) held at Marseille , France, in June 1979. At this meeting, Since then, most results in this area are related to one or several of these items either by using or improving one of these algorithms, or by finding algorithms whose complexity

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4788-461: Is the restriction to V of a regular function on A . For an algebraic set defined on the field of the complex numbers, the regular functions are smooth and even analytic . It may seem unnaturally restrictive to require that a regular function always extend to the ambient space, but it is very similar to the situation in a normal topological space , where the Tietze extension theorem guarantees that

4902-467: Is the study of connections on vector bundles and principal bundles, and arises out of problems in mathematical physics and physical gauge theories which underpin the standard model of particle physics . Gauge theory is concerned with the study of differential equations for connections on bundles, and the resulting geometric moduli spaces of solutions to these equations as well as the invariants that may be derived from them. These equations often arise as

5016-477: Is the tangent space at the unit endowed with the Lie bracket between left-invariant vector fields . Beside the structure theory there is also the wide field of representation theory . Geometric analysis is a mathematical discipline where tools from differential equations, especially elliptic partial differential equations are used to establish new results in differential geometry and differential topology. Gauge theory

5130-404: Is to emphasize that one "forgets" the vector space structure that k carries. A function f  : A → A is said to be polynomial (or regular ) if it can be written as a polynomial, that is, if there is a polynomial p in k [ x 1 ,..., x n ] such that f ( M ) = p ( t 1 ,..., t n ) for every point M with coordinates ( t 1 ,..., t n ) in A . The property of

5244-412: Is yet unsolved in finite characteristic. Just as the formulas for the roots of second, third, and fourth degree polynomials suggest extending real numbers to the more algebraically complete setting of the complex numbers, many properties of algebraic varieties suggest extending affine space to a more geometrically complete projective space. Whereas the complex numbers are obtained by adding the number i ,

5358-521: The Bernoulli brothers , Jacob and Johann made important early contributions to the use of infinitesimals to study geometry. In lectures by Johann Bernoulli at the time, later collated by L'Hopital into the first textbook on differential calculus , the tangents to plane curves of various types are computed using the condition d y = 0 {\displaystyle dy=0} , and similarly points of inflection are calculated. At this same time

5472-529: The Euler–Lagrange equations and the first theory of the calculus of variations , which underpins in modern differential geometry many techniques in symplectic geometry and geometric analysis . This theory was used by Lagrange , a co-developer of the calculus of variations, to derive the first differential equation describing a minimal surface in terms of the Euler–Lagrange equation. In 1760 Euler proved

5586-462: The Euler–Lagrange equations describing the equations of motion of certain physical systems in quantum field theory , and so their study is of considerable interest in physics. The apparatus of vector bundles , principal bundles , and connections on bundles plays an extraordinarily important role in modern differential geometry. A smooth manifold always carries a natural vector bundle, the tangent bundle . Loosely speaking, this structure by itself

5700-909: The Gottfried Wilhelm Leibniz Prize . In 2014 she was elected to the Academia Europaea and is a member of the Academy of Sciences Leopoldina , the Berlin-Brandenburg Academy of Sciences and Humanities and the Europäische Akademie Nordrhein-Westfalen  [ de ] . In 2019, she won the Cantor medal . Algebraic geometry The fundamental objects of study in algebraic geometry are algebraic varieties , which are geometric manifestations of solutions of systems of polynomial equations . Examples of

5814-545: The Mercator projection as a way of mapping the Earth. Mercator had an understanding of the advantages and pitfalls of his map design, and in particular was aware of the conformal nature of his projection, as well as the difference between praga , the lines of shortest distance on the Earth, and the directio , the straight line paths on his map. Mercator noted that the praga were oblique curvatur in this projection. This fact reflects

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5928-541: The Nijenhuis tensor (or sometimes the torsion ). An almost complex manifold is complex if and only if it admits a holomorphic coordinate atlas . An almost Hermitian structure is given by an almost complex structure J , along with a Riemannian metric g , satisfying the compatibility condition An almost Hermitian structure defines naturally a differential two-form The following two conditions are equivalent: where ∇ {\displaystyle \nabla }

6042-501: The Poincaré conjecture . During this same period primarily due to the influence of Michael Atiyah , new links between theoretical physics and differential geometry were formed. Techniques from the study of the Yang–Mills equations and gauge theory were used by mathematicians to develop new invariants of smooth manifolds. Physicists such as Edward Witten , the only physicist to be awarded

6156-565: The Theorema Egregium of Carl Friedrich Gauss showed that for surfaces, the existence of a local isometry imposes that the Gaussian curvatures at the corresponding points must be the same. In higher dimensions, the Riemann curvature tensor is an important pointwise invariant associated with a Riemannian manifold that measures how close it is to being flat. An important class of Riemannian manifolds

6270-781: The University of Duisburg-Essen . Afterwards, she was a Heisenberg scholar of the Deutsche Forschungsgemeinschaft (DFG) at the Max Planck Institute for Mathematics in Bonn. She became the first Einstein Professor at Freie Universität Berlin in 2012, as head of the algebra and number theory research group, after working previously at the University of Duisburg-Essen, the Max-Planck-Institut für Mathematik in Bonn, and at

6384-621: The curvature provides a local invariant of Riemannian manifolds, Darboux's theorem states that all symplectic manifolds are locally isomorphic. The only invariants of a symplectic manifold are global in nature and topological aspects play a prominent role in symplectic geometry. The first result in symplectic topology is probably the Poincaré–Birkhoff theorem , conjectured by Henri Poincaré and then proved by G.D. Birkhoff in 1912. It claims that if an area preserving map of an annulus twists each boundary component in opposite directions, then

6498-447: The equivalence principle a full 60 years before it appeared in the scientific literature. In the wake of Riemann's new description, the focus of techniques used to study differential geometry shifted from the ad hoc and extrinsic methods of the study of curves and surfaces to a more systematic approach in terms of tensor calculus and Klein's Erlangen program, and progress increased in the field. The notion of groups of transformations

6612-416: The hyperbola of equation x y − 1 = 0 {\displaystyle xy-1=0} is a real algebraic variety. However, the branch in the first quadrant is a semi-algebraic set defined by x y − 1 = 0 {\displaystyle xy-1=0} and x > 0 {\displaystyle x>0} . One open problem in real algebraic geometry

6726-401: The orthogonality between the osculating circles of a plane curve and the tangent directions is realised, and the first analytical formula for the radius of an osculating circle, essentially the first analytical formula for the notion of curvature , is written down. In the wake of the development of analytic geometry and plane curves, Alexis Clairaut began the study of space curves at just

6840-478: The topology of the curve and the relationship between curves defined by different equations. Algebraic geometry occupies a central place in modern mathematics and has multiple conceptual connections with such diverse fields as complex analysis , topology and number theory . As a study of systems of polynomial equations in several variables, the subject of algebraic geometry begins with finding specific solutions via equation solving , and then proceeds to understand

6954-432: The two-dimensional sphere of radius 1 in three-dimensional Euclidean space R could be defined as the set of all points ( x , y , z ) {\displaystyle (x,y,z)} with A "slanted" circle in R can be defined as the set of all points ( x , y , z ) {\displaystyle (x,y,z)} which satisfy the two polynomial equations First we start with

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7068-399: The 1600s. Around this time there were only minimal overt applications of the theory of infinitesimals to the study of geometry, a precursor to the modern calculus-based study of the subject. In Euclid 's Elements the notion of tangency of a line to a circle is discussed, and Archimedes applied the method of exhaustion to compute the areas of smooth shapes such as the circle , and

7182-531: The 1860s, and Felix Klein coined the term non-Euclidean geometry in 1871, and through the Erlangen program put Euclidean and non-Euclidean geometries on the same footing. Implicitly, the spherical geometry of the Earth that had been studied since antiquity was a non-Euclidean geometry, an elliptic geometry . The development of intrinsic differential geometry in the language of Gauss was spurred on by his student, Bernhard Riemann in his Habilitationsschrift , On

7296-463: The Darboux theorem holds: all contact structures on an odd-dimensional manifold are locally isomorphic and can be brought to a certain local normal form by a suitable choice of the coordinate system. Complex differential geometry is the study of complex manifolds . An almost complex manifold is a real manifold M {\displaystyle M} , endowed with a tensor of type (1, 1), i.e.

7410-586: The University of Paris VII. In 2007 Esnault was editor-in-chief and founder of the journal Algebra & Number Theory . From 1998 to 2010 she co-edited Mathematische Annalen ; she has also served as editor of Acta Mathematica Vietnamica, Astérisque , Duke Mathematical Journal , and Mathematical Research Letters. In 2001 she won the Prix Paul Doistau-Émile Blutet of the Académie des Sciences de Paris. In 2003, Esnault and Eckart Viehweg received

7524-448: The age of 16. In his book Clairaut introduced the notion of tangent and subtangent directions to space curves in relation to the directions which lie along a surface on which the space curve lies. Thus Clairaut demonstrated an implicit understanding of the tangent space of a surface and studied this idea using calculus for the first time. Importantly Clairaut introduced the terminology of curvature and double curvature , essentially

7638-403: The beginning and through the middle of the 19th century, differential geometry was studied from the extrinsic point of view: curves and surfaces were considered as lying in a Euclidean space of higher dimension (for example a surface in an ambient space of three dimensions). The simplest results are those in the differential geometry of curves and differential geometry of surfaces. Starting with

7752-414: The development of quantum field theory and the standard model of particle physics . Outside of physics, differential geometry finds applications in chemistry , economics , engineering , control theory , computer graphics and computer vision , and recently in machine learning . The history and development of differential geometry as a subject begins at least as far back as classical antiquity . It

7866-476: The development of the modern theory, including Jean-Louis Koszul who introduced connections on vector bundles , Shiing-Shen Chern who introduced characteristic classes to the subject and began the study of complex manifolds , Sir William Vallance Douglas Hodge and Georges de Rham who expanded understanding of differential forms , Charles Ehresmann who introduced the theory of fibre bundles and Ehresmann connections , and others. Of particular importance

7980-443: The distinction between the two subjects). Differential geometry is also related to the geometric aspects of the theory of differential equations , otherwise known as geometric analysis . Differential geometry finds applications throughout mathematics and the natural sciences . Most prominently the language of differential geometry was used by Albert Einstein in his theory of general relativity , and subsequently by physicists in

8094-400: The exact opposite of the parabola. So the behavior "at infinity" of V ( y  −  x ) is different from the behavior "at infinity" of V ( y  −  x ). The consideration of the projective completion of the two curves, which is their prolongation "at infinity" in the projective plane , allows us to quantify this difference: the point at infinity of the parabola is

8208-400: The finitely generated reduced k -algebras. This equivalence is one of the starting points of scheme theory . In contrast to the preceding sections, this section concerns only varieties and not algebraic sets. On the other hand, the definitions extend naturally to projective varieties (next section), as an affine variety and its projective completion have the same field of functions. If V

8322-470: The first question is provided by introducing the Zariski topology , a topology on A whose closed sets are the algebraic sets, and which directly reflects the algebraic structure of k [ A ]. Then U = V ( I ( U )) if and only if U is an algebraic set or equivalently a Zariski-closed set. The answer to the second question is given by Hilbert's Nullstellensatz . In one of its forms, it says that I ( V ( S ))

8436-496: The first set of intrinsic coordinate systems on a surface, beginning the theory of intrinsic geometry upon which modern geometric ideas are based. Around this time Euler's study of mechanics in the Mechanica lead to the realization that a mass traveling along a surface not under the effect of any force would traverse a geodesic path, an early precursor to the important foundational ideas of Einstein's general relativity , and also to

8550-406: The foundational contributions of many mathematicians, including importantly the work of Henri Poincaré on the foundations of topology . At the start of the 1900s there was a major movement within mathematics to formalise the foundational aspects of the subject to avoid crises of rigour and accuracy, known as Hilbert's program . As part of this broader movement, the notion of a topological space

8664-398: The homogeneous (reduced) ideal defining the variety. Every projective algebraic set may be uniquely decomposed into a finite union of projective varieties. The only regular functions which may be defined properly on a projective variety are the constant functions. Thus this notion is not used in projective situations. On the other hand, the field of the rational functions or function field

8778-417: The hypotheses which lie at the foundation of geometry . In this work Riemann introduced the notion of a Riemannian metric and the Riemannian curvature tensor for the first time, and began the systematic study of differential geometry in higher dimensions. This intrinsic point of view in terms of the Riemannian metric, denoted by d s 2 {\displaystyle ds^{2}} by Riemann,

8892-501: The intrinsic properties of the totality of solutions of a system of equations. This understanding requires both conceptual theory and computational technique. In the 20th century, algebraic geometry split into several subareas. Much of the development of the mainstream of algebraic geometry in the 20th century occurred within an abstract algebraic framework, with increasing emphasis being placed on "intrinsic" properties of algebraic varieties not dependent on any particular way of embedding

9006-507: The inventor of intrinsic differential geometry. In his fundamental paper Gauss introduced the Gauss map , Gaussian curvature , first and second fundamental forms , proved the Theorema Egregium showing the intrinsic nature of the Gaussian curvature, and studied geodesics, computing the area of a geodesic triangle in various non-Euclidean geometries on surfaces. At this time Gauss was already of

9120-610: The lack of a metric-preserving map of the Earth's surface onto a flat plane, a consequence of the later Theorema Egregium of Gauss . The first systematic or rigorous treatment of geometry using the theory of infinitesimals and notions from calculus began around the 1600s when calculus was first developed by Gottfried Leibniz and Isaac Newton . At this time, the recent work of René Descartes introducing analytic coordinates to geometry allowed geometric shapes of increasing complexity to be described rigorously. In particular around this time Pierre de Fermat , Newton, and Leibniz began

9234-479: The language and the tools of classical algebraic geometry, mainly concerned with complex points, and of algebraic number theory. Wiles' proof of the longstanding conjecture called Fermat's Last Theorem is an example of the power of this approach. In classical algebraic geometry, the main objects of interest are the vanishing sets of collections of polynomials , meaning the set of all points that simultaneously satisfy one or more polynomial equations . For instance,

9348-405: The level sets of a differentiable function on M (the technical term is "completely nonintegrable tangent hyperplane distribution"). Near each point p , a hyperplane distribution is determined by a nowhere vanishing 1-form α {\displaystyle \alpha } , which is unique up to multiplication by a nowhere vanishing function: A local 1-form on M is a contact form if

9462-399: The map has at least two fixed points. Contact geometry deals with certain manifolds of odd dimension. It is close to symplectic geometry and like the latter, it originated in questions of classical mechanics. A contact structure on a (2 n + 1) -dimensional manifold M is given by a smooth hyperplane field H in the tangent bundle that is as far as possible from being associated with

9576-411: The mathematical basis of Einstein's general relativity theory of gravity . Finsler geometry has Finsler manifolds as the main object of study. This is a differential manifold with a Finsler metric , that is, a Banach norm defined on each tangent space. Riemannian manifolds are special cases of the more general Finsler manifolds. A Finsler structure on a manifold M {\displaystyle M}

9690-516: The most studied classes of algebraic varieties are lines , circles , parabolas , ellipses , hyperbolas , cubic curves like elliptic curves , and quartic curves like lemniscates and Cassini ovals . These are plane algebraic curves . A point of the plane lies on an algebraic curve if its coordinates satisfy a given polynomial equation . Basic questions involve the study of points of special interest like singular points , inflection points and points at infinity . More advanced questions involve

9804-413: The natural operations such as Lie derivative of natural vector bundles and de Rham differential of forms . Beside Lie algebroids , also Courant algebroids start playing a more important role. A Lie group is a group in the category of smooth manifolds. Beside the algebraic properties this enjoys also differential geometric properties. The most obvious construction is that of a Lie algebra which

9918-621: The notation g {\displaystyle g} for a Riemannian metric, and Γ {\displaystyle \Gamma } for the Christoffel symbols, both coming from G in Gravitation . Élie Cartan helped reformulate the foundations of the differential geometry of smooth manifolds in terms of exterior calculus and the theory of moving frames , leading in the world of physics to Einstein–Cartan theory . Following this early development, many mathematicians contributed to

10032-434: The notion of principal curvatures later studied by Gauss and others. Around this same time, Leonhard Euler , originally a student of Johann Bernoulli, provided many significant contributions not just to the development of geometry, but to mathematics more broadly. In regards to differential geometry, Euler studied the notion of a geodesic on a surface deriving the first analytical geodesic equation , and later introduced

10146-404: The notion of point: In classical algebraic geometry, a point of an affine variety may be identified, through Hilbert's Nullstellensatz , with a maximal ideal of the coordinate ring , while the points of the corresponding affine scheme are all prime ideals of this ring. This means that a point of such a scheme may be either a usual point or a subvariety. This approach also enables a unification of

10260-476: The opinion that the standard paradigm of Euclidean geometry should be discarded, and was in possession of private manuscripts on non-Euclidean geometry which informed his study of geodesic triangles. Around this same time János Bolyai and Lobachevsky independently discovered hyperbolic geometry and thus demonstrated the existence of consistent geometries outside Euclid's paradigm. Concrete models of hyperbolic geometry were produced by Eugenio Beltrami later in

10374-427: The origin if and only if it is homogeneous . In this case, one says that the polynomial vanishes at the corresponding point of P . This allows us to define a projective algebraic set in P as the set V ( f 1 , ..., f k ) , where a finite set of homogeneous polynomials { f 1 , ..., f k } vanishes. Like for affine algebraic sets, there is a bijection between the projective algebraic sets and

10488-508: The other in the regions where both are defined. Equivalently, they are birationally equivalent if their function fields are isomorphic. An affine variety is a rational variety if it is birationally equivalent to an affine space. This means that the variety admits a rational parameterization , that is a parametrization with rational functions . For example, the circle of equation x 2 + y 2 − 1 = 0 {\displaystyle x^{2}+y^{2}-1=0}

10602-405: The points of a line have the same set of coordinates, up to the multiplication by an element of k . This defines the homogeneous coordinates of a point of P as a sequence of n + 1 elements of the base field k , defined up to the multiplication by a nonzero element of k (the same for the whole sequence). A polynomial in n + 1 variables vanishes at all points of a line passing through

10716-602: The proof of the Atiyah–Singer index theorem . The development of complex geometry was spurred on by parallel results in algebraic geometry , and results in the geometry and global analysis of complex manifolds were proven by Shing-Tung Yau and others. In the latter half of the 20th century new analytic techniques were developed in regards to curvature flows such as the Ricci flow , which culminated in Grigori Perelman 's proof of

10830-424: The purposes of mapping the shape of the Earth. Implicitly throughout this time principles that form the foundation of differential geometry and calculus were used in geodesy , although in a much simplified form. Namely, as far back as Euclid 's Elements it was understood that a straight line could be defined by its property of providing the shortest distance between two points, and applying this same principle to

10944-402: The range of f is contained in V ′. The definition of the regular maps apply also to algebraic sets. The regular maps are also called morphisms , as they make the collection of all affine algebraic sets into a category , where the objects are the affine algebraic sets and the morphisms are the regular maps. The affine varieties is a subcategory of the category of the algebraic sets. Given

11058-400: The reduced homogeneous ideals which define them. The projective varieties are the projective algebraic sets whose defining ideal is prime. In other words, a projective variety is a projective algebraic set, whose homogeneous coordinate ring is an integral domain , the projective coordinates ring being defined as the quotient of the graded ring or the polynomials in n + 1 variables by

11172-417: The restriction of its exterior derivative to H is a non-degenerate two-form and thus induces a symplectic structure on H p at each point. If the distribution H can be defined by a global one-form α {\displaystyle \alpha } then this form is contact if and only if the top-dimensional form is a volume form on M , i.e. does not vanish anywhere. A contact analogue of

11286-479: The same period the development of projective geometry . Dubbed the single most important work in the history of differential geometry, in 1827 Gauss produced the Disquisitiones generales circa superficies curvas detailing the general theory of curved surfaces. In this work and his subsequent papers and unpublished notes on the theory of surfaces, Gauss has been dubbed the inventor of non-Euclidean geometry and

11400-400: The slope of the same line goes to negative infinity. Compare this to the variety V ( y  −  x ). This is a cubic curve . As x goes to positive infinity, the slope of the line from the origin to the point ( x ,  x ) goes to positive infinity just as before. But unlike before, as x goes to negative infinity, the slope of the same line goes to positive infinity as well;

11514-494: The study of hyperbolic geometry by Lobachevsky . The simplest examples of smooth spaces are the plane and space curves and surfaces in the three-dimensional Euclidean space , and the study of these shapes formed the basis for development of modern differential geometry during the 18th and 19th centuries. Since the late 19th century, differential geometry has grown into a field concerned more generally with geometric structures on differentiable manifolds . A geometric structure

11628-435: The study of plane curves and the investigation of concepts such as points of inflection and circles of osculation , which aid in the measurement of curvature . Indeed, already in his first paper on the foundations of calculus, Leibniz notes that the infinitesimal condition d 2 y = 0 {\displaystyle d^{2}y=0} indicates the existence of an inflection point. Shortly after this time

11742-416: The study of the geometry of smooth shapes, can be traced back at least to classical antiquity . In particular, much was known about the geometry of the Earth , a spherical geometry , in the time of the ancient Greek mathematicians. Famously, Eratosthenes calculated the circumference of the Earth around 200 BC, and around 150 AD Ptolemy in his Geography introduced the stereographic projection for

11856-429: The subvariety (a hypersurface) where the denominator of f vanishes. As with regular maps, one may define a rational map from a variety V to a variety V '. As with the regular maps, the rational maps from V to V ' may be identified to the field homomorphisms from k ( V ') to k ( V ). Two affine varieties are birationally equivalent if there are two rational functions between them which are inverse one to

11970-442: The surface of the Earth leads to the conclusion that great circles , which are only locally similar to straight lines in a flat plane, provide the shortest path between two points on the Earth's surface. Indeed, the measurements of distance along such geodesic paths by Eratosthenes and others can be considered a rudimentary measure of arclength of curves, a concept which did not see a rigorous definition in terms of calculus until

12084-440: The topological properties, depend on the behavior "at infinity" and so it is natural to study the varieties in projective space. Furthermore, the introduction of projective techniques made many theorems in algebraic geometry simpler and sharper: For example, Bézout's theorem on the number of intersection points between two varieties can be stated in its sharpest form only in projective space. For these reasons, projective space plays

12198-538: The vanishing set of a prime ideal of the polynomial ring . Some authors do not make a clear distinction between algebraic sets and varieties and use irreducible variety to make the distinction when needed. Just as continuous functions are the natural maps on topological spaces and smooth functions are the natural maps on differentiable manifolds , there is a natural class of functions on an algebraic set, called regular functions or polynomial functions . A regular function on an algebraic set V contained in A

12312-412: The variety in an ambient coordinate space; this parallels developments in topology, differential and complex geometry . One key achievement of this abstract algebraic geometry is Grothendieck 's scheme theory which allows one to use sheaf theory to study algebraic varieties in a way which is very similar to its use in the study of differential and analytic manifolds . This is obtained by extending

12426-458: The volumes of smooth three-dimensional solids such as the sphere, cones, and cylinders. There was little development in the theory of differential geometry between antiquity and the beginning of the Renaissance . Before the development of calculus by Newton and Leibniz , the most significant development in the understanding of differential geometry came from Gerardus Mercator 's development of

12540-482: The work of Riemann , the intrinsic point of view was developed, in which one cannot speak of moving "outside" the geometric object because it is considered to be given in a free-standing way. The fundamental result here is Gauss's theorema egregium , to the effect that Gaussian curvature is an intrinsic invariant. The intrinsic point of view is more flexible. For example, it is useful in relativity where space-time cannot naturally be taken as extrinsic. However, there

12654-692: Was Hermann Weyl who made important contributions to the foundations of general relativity, introduced the Weyl tensor providing insight into conformal geometry , and first defined the notion of a gauge leading to the development of gauge theory in physics and mathematics . In the middle and late 20th century differential geometry as a subject expanded in scope and developed links to other areas of mathematics and physics. The development of gauge theory and Yang–Mills theory in physics brought bundles and connections into focus, leading to developments in gauge theory . Many analytical results were investigated including

12768-611: Was developed by Sophus Lie and Jean Gaston Darboux , leading to important results in the theory of Lie groups and symplectic geometry . The notion of differential calculus on curved spaces was studied by Elwin Christoffel , who introduced the Christoffel symbols which describe the covariant derivative in 1868, and by others including Eugenio Beltrami who studied many analytic questions on manifolds. In 1899 Luigi Bianchi produced his Lectures on differential geometry which studied differential geometry from Riemann's perspective, and

12882-461: Was distilled in by Felix Hausdorff in 1914, and by 1942 there were many different notions of manifold of a combinatorial and differential-geometric nature. Interest in the subject was also focused by the emergence of Einstein's theory of general relativity and the importance of the Einstein Field equations. Einstein's theory popularised the tensor calculus of Ricci and Levi-Civita and introduced

12996-416: Was the development of an idea of Gauss's about the linear element d s {\displaystyle ds} of a surface. At this time Riemann began to introduce the systematic use of linear algebra and multilinear algebra into the subject, making great use of the theory of quadratic forms in his investigation of metrics and curvature. At this time Riemann did not yet develop the modern notion of

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