Bourbaki

Historical note

(Chapters II and III)

(N.B. Numbers in brackets refer to the bibliography at the end of this Note.)

Linear algebra is both one of the oldest and one of the newest branches of mathematics. On the other hand, at the origins of mathematics are the problems which are solved by a single multiplication or division, that is by calculating a value of a function f(x)=axf(x) = ax, or by solving an equation ax=bax = b: these are typical problems of linear algebra and it is impossible to deal with them, indeed even to pose them correctly, without "thinking linearly".

On the other hand, not only these questions but almost everything concerning equations of the first degree had long been relegated to elementary teaching, when the modern development of the notions of field, ring, topological vector space, etc. came to isolate and emphasize the essential notions of linear algebra (for example duality); then the essentially linear character of almost the whole of modern mathematics was perceived, of which "linearization" is itself one of the distinguishing traits, and linear algebra was given the place it merits. To give its history, from our present point of view, would therefore be a task as difficult as it is important; and we must therefore be content to give a brief summary.

From the above it is seen that linear algebra was no doubt born in response to the needs of practical calculators; thus we see the rule of three† and the rule of false position, more or less clearly stated, playing an important role in all the manuals of practical arithmetic, from the Rhind papyrus of the Egyptians to those used in our primary schools, by way of Āryabhaṭa, the Arabs, Leonard of

† Cf. J. Tropfke, Geschichte der Elementar-Mathematik, 1. Band, 2te Ausgabe, Berlin-Leipzig (W. de Gruyter), 1921, pp. 150–155.

Pisa and the countless "calculation books" of the Middle Ages and the Renaissance; but they never constituted more than a small part, for the use of practical men, of the most advanced scientific theories.

As for mathematicians proper, the nature of their research on linear algebra depends on the general structure of their science. Ancient Greek mathematics, as expounded in the Elements of Euclid, developed two abstract theories of a linear character, on the one hand that of magnitudes ([2], Book V; cf. Historical Note to General Topology, IV) and on the other hand that of integers ([2], Book VII). With the Babylonians we find methods much more akin to our elementary algebra; they know how to solve, and most elegantly ([1], pp. 181–183), systems of equations of the first degree. For a very long time, nevertheless, the progress of linear algebra is mainly confined to that of algebraic calculations and they should be considered from this point of view, foreign to this Note; to reduce a linear system to an equation of the type ax=bax = b, it suffices, in the case of a single unknown, to know the rules (already, in substance, stated by Diophantus) for taking terms from one side to the other and combining similar terms; and, in the case of several unknowns, it suffices to know also how to eliminate them successively until only one is left. Also the Treatises on algebra, until the XVIIIth century, think that all is accomplished as far as the first degree is concerned, when they have expounded these rules; as for a system of as many equations as unknowns (they do not consider others) where the left hand sides are not linearly independent forms, they are content to observe in passing that this indicates a badly posed problem. In the treatises of the XIXth century and even certain more recent works, this point of view is only modified by the progress of notation, which allows writing systems of nn equations in nn unknowns, and by the introduction of determinants which allow formulae of an explicit solution to be given in the "general case"; this progress, the credit for which would have belonged to Leibniz ([7], p. 239) had he developed and published his ideas on this subject, is mainly due to the mathematicians of the XVIIIth and early XIXth centuries.

But we must first study various currents of ideas which, much more than the study of linear equations, contributed to the development of linear algebra in the sense in which we understand it. Inspired by the study of Appollonius, Fermat [4(a)], having conceived, even before Descartes [5], the principle of analytic geometry, has the idea of classifying plane curves according to their degree (which, having become little by little familiar to all mathematicians, can be considered to have been definitely grasped towards the end of the XVIIth century) and formulates the fundamental principle that an equation of the first degree, in the plane, represents a line and an equation of the second degree a conic: a principle from which he deduces immediately some "very beautiful" consequences relating to geometric loci. At the same time, he enunciates [4(b)] the classification of problems into problems with a single solution, problems which reduce to an equation in two unknowns, an equation in three unknowns, etc.; and he adds: the first consist of determining a point, the second a line or plane locus, the others a surface, etc. ("... such a problem does not seek only a point or a line, but the whole of a surface appropriate to the question; here surfaces as loci have their genesis and similarly for the rest", loc. cit., p. 186; here already is the germ of n-dimensional geometry). This paper, formulating the principle of dimension in algebra and algebraic geometry, indicates a fusion of algebra and geometry in absolute conformity with modern ideas, but which, as has already been seen, took more than two centuries to penetrate into men's minds.

At least these ideas soon result in the expansion of analytic geometry which reaches its fulness in the XVIIIth century with Clairaut, Euler, Cramer, Lagrange and many others. The linear character of the formulae for transformation of coordinates in the plane and in space, which Fermat cannot have failed already to have perceived, is put in relief for example by Euler ([8(a)], Chapters II–III and Appendix to Chapter IV), who here lays the foundation of the classification of plane curves and that of surfaces according to their degree (invariant precisely because of the linearity of these formulae); he it is also (loc. cit., Chapter XVIII) who introduces the word "affinity" to describe the relation between curves which can be derived one from the other by a transformation x′=ax,y′=byx' = ax, y' = by (but without perceiving anything geometrically invariant in this definition which remains bound to a particular choice of axes). A little later we see Lagrange [9(a)] devoting a whole memoir, which long remained justly famous, to typically linear and multilinear problems of analytic geometry in three dimensions. Around about this time, in relation to the linear problem constituted by the search for a plane curve passing through given points, the notion of determinant takes shape, first in a somewhat empirical way, with Cramer [10] and Bezout [11]; this notion is then developed by several authors and its essential properties are definitively established by Cauchy [13] and Jacobi [16(a)].

On the other hand, whilst mathematicians had a slight tendency to despise equations of the first degree, the solution of differential equations was considered a capital problem; it was natural that, among these equations, linear equations, with constant coefficients or otherwise, should early be distinguished and their study contributed to emphasize linearity and related properties. This is certainly seen in the work of Lagrange [9(b)] and Euler [8(b)], at least as far as homogeneous equations are concerned; for these authors see no point in saying that the general solution of the non-homogeneous equation is the sum of a particular solution and the general solution of the corresponding homogeneous equation and they make no use of this principle (known however to d'Alembert); we note here also that, when they state that the general solution of the homogeneous linear equation of order nn is a linear combination of nn particular solutions, they do not add that these must be linearly independent and make no effort to make the latter notion explicit; it seems that only the teaching of Cauchy at the École Polytechnique throws some light ([14], pp. 573–574) on these points as on many others. But already Lagrange (loc. cit.) introduces also (purely by calculation, it is true, and without giving it a name) the adjoint equation L∗(y)=0L^*(y) = 0 of a linear differential equation L(y)=0L(y) = 0, an example typical of duality by virtue of the relation

∫zL(y) dx=∫L∗(z)y dx, \int z L(y)\, dx = \int L^*(z) y\, dx,

valid for yy and zz zero at the extremities of the interval of integration; more precisely, and 30 years before Gauss defined explicitly the transpose of a linear substitution in 3 variables, we see here the first example without doubt of a "functional operator" L∗L^* the transpose or "adjoint" of an operator LL given by means of a bilinear function (here the integral ∫yz dx\int yz\, dx).

At the same time and again with Lagrange [9(c)], linear substitutions, in 2 and 3 variables at first, were in the process of conquering arithmetic. Clearly the set of values of a function F(x,y)F(x, y), when xx and yy are given all integral values, does not change when a linear substitution with integral coefficients, of determinant 1, is performed on xx and yy; on this fundamental observation Lagrange founds the theory of representations of numbers by forms and that of the reduction of forms; and Gauss, by a step whose boldness it has become difficult for us to appreciate, isolates the notion of equivalence and that of class of forms (cf. Historical Note to I); on this subject, he recognizes the necessity of certain elementary principles relating to linear substitutions and introduces in particular the notion of transpose or adjoint ([12(a)], p. 304). From this moment onwards, the arithmetic study and the algebraic study of quadratic forms, in 2, 3 and later nn variables, that of bilinear forms which are closely related to them and more recently the generalization of these notions to an infinity of variables were, right up to the present, to constitute one of the most fertile sources of progress for linear algebra (cf. Historical Note to IX).

But a perhaps still more decisive progress was the creation by Gauss, in the same Disquisitiones (cf. Historical Note to I), of the theory of finite commutative groups, which occur there in four different ways, in the additive group of integers modulo mm (for mm an integer), in the multiplicative group of integers prime to mm modulo mm, in the group of classes of binary quadratic forms and finally in the multiplicative group of mm-th roots of unity; and, as we have already noted, it is clearly as commutative groups, or rather as modules over Z\mathbf{Z}, that Gauss treats all these groups and studies their structure, their relations of isomorphism, etc. In the module of "complex integers" a+bia + bi, he is later seen studying an infinite module over Z\mathbf{Z}, whose isomorphism he no doubt perceived with the module of periods (discovered by him in the complex domain) of elliptic functions; in any case this idea already appears neatly in Jacobi's work, for example in his famous proof of the impossibility of a function with 3 periods and his views on the problem of inversion of Abelian integrals [16(b)], to result soon in the theorems of Kronecker (cf. Historical Note to General Topology, VII).

Here, another current joins those whose course and occasional meanders we have sought to trace, which had long remained underground. As will later be expounded in more detail (Historical Note to IX), "pure" geometry in the sense understood in the last century, that is essentially projective geometry of the plane and space without using coordinates, had been created in the XVIIth century by Desargues [6], whose ideas, appreciated in their true value by a Fermat and put into practice by a Pascal, had then been buried in oblivion, eclipsed by the brilliant progress of analytic geometry; it was revived towards the end of the XVIIIth century, with Monge, then Poncelet and his rivals Brianchon and Chasles, sometimes completely and voluntarily separated from analytic methods, sometimes (especially in Germany) closely intermixed with them. Now projective transformations, from whatever point of view they are considered (synthetic or analytic), are of course just linear substitutions on the projective or "barycentric" coordinates; the theory of conics (in the XVIIth century) and later that of quadrics, with whose projective properties this school is principally concerned for a long time, are just that of quadratic forms, whose close connection with linear algebra we have already pointed out earlier. To these notions is added that of polarity: also created by Desargues, the theory of poles and polars becomes, in the hands of Monge and his successors and soon under the name of the principle of duality, a powerful tool for transforming geometric theorems; if it cannot be affirmed that its relation with adjoint differential equations was perceived during that period (they are indicated by Pincherle at the end of the century), then at least Chasles did not fail [17] to perceive its relation with the notion of reciprocal spherical triangles, introduced into spherical trigonometry by Viète ([3], p. 428) and Snellius as early as the XVIth century. But duality in projective geometry is only an aspect of duality of vector spaces, taking account of the modifications imposed when passing from the affine space to the projective space (which is a quotient space of it, under the relation "scalar multiplication").

The XIXth century, more than any period in our history, was rich in mathematicians of the first order; and it is difficult in a few pages, even restricting ourselves to the most salient features, to describe all that is produced in their hands by the coming together of these movements of ideas. Between the purely synthetic methods on the one hand, a species of Procrustean bed where their orthodox protagonists put themselves to torture, and the analytic methods related to a system of coordinates arbitrarily imposed on the space, the need is soon felt for a geometric calculus, dreamed of but not created by Leibniz and imperfectly sketched by Carnot: first appears addition of vectors, implicit in Gauss's work in his geometric representation of imaginary numbers and the applications he makes of this to elementary geometry (cf. Historical Note to General Topology, VIII), developed by Bellavitis under the name of "method of equipollences" and taking its definitive form with Grassmann, Möbius and Hamilton; at the same time, under the name of "barycentric calculus", Möbius gives a version of it suitable for the needs of projective geometry [18].

At the same period, and by the same men, the step, so natural (once engaged on this path), already announced by Fermat, is taken from the plane and "ordinary" space to nn-dimensional space; indeed an inevitable step, since the algebraic phenomena which can in two or three variables be interpreted geometrically are still valid for an arbitrary number of variables; thus to impose, in using geometric language, the limitation to 2 or 3 dimensions, would be for the modern mathematician just as tiresome a yoke as that which always prevented the Greeks from extending the notion of number to ratios of incommensurable magnitudes. Hence the language and ideas relating to nn-dimensional space appear almost simultaneously on all sides, obscurely in the work of Gauss, clearly in the work of the mathematicians of the following generation; and their greater or less assurance in using them was perhaps less due to their mathematical inclinations than to their philosophical or even purely practical outlook. In any case, Cayley and Grassmann, around 1846, handle these concepts with the greatest of ease (and this, says Cayley quite contrary to Grassmann ([22(a)], p. 321), "without recourse to any metaphysical notion"); Cayley is never far away from the analytic interpretation and coordinates, whereas in Grassmann's work from the start, addition of vectors in nn-dimensional space and the geometric aspect take the upper hand, to result in the developments of which we shall speak in a moment.

Meantime the impulse given by Gauss was pushing mathematicians, in two different ways, towards this study of algebras or "hypercomplex systems". On the one hand, it was inevitable to try to extend the domain of real numbers otherwise than by introducing the "imaginary unit" i=−1i = \sqrt{-1} and perhaps thus open up vaster domains just as fertile as that of the complex numbers. Gauss himself was convinced ([12(b)], p. 178) of the impossibility of such an extension, as long as one wants to preserve the principal properties of complex numbers, that is, in modern language, those which make it into a commutative field; and, either under his influence or independently, his contemporaries seem to have shared this conviction, which was only justified much later by Weierstrass [23] in a precise theorem. But, once multiplication of complex numbers is interpreted by rotations in the plane, then, if it is proposed to extend this idea to three dimensional space, (since the rotations in space form a non-Abelian group) non-commutative multiplications have to be envisaged; this is one of Hamilton's† guiding ideas in his discovery of quaternions [20], the first example of a non-commutative field. The singular nature of this example (the only one, as Frobenius was later to show, which can be constructed over the

† Cf. the interesting preface of his Lectures on quaternions [20] where he retraces the whole history of his discovery.

field of real numbers) somewhat restricts its import, in spite of or perhaps even because of the formation of a school of fanatical "quaternionists": a strange phenomenon, which was later reproduced around the work of Grassmann, and then by the vulgarizers who draw from Hamilton and Grassmann what is called "vector calculus". The abandoning a little later of associativity, by Graves and Cayley who construct the "Cayley numbers", opens up no very interesting path. But after Sylvester had introduced matrices and (without giving it a name) had clearly defined their rank [21], again it was Cayley [22(b)] who created the calculus of matrices, not without observing (an essential fact often lost sight of later) that a matrix is only an abridged notation for a linear substitution, just as Gauss denoted the form aX2+2bXY+cY2aX^2 + 2bXY + cY^2 by (a,b,c)(a, b, c). This is just one aspect, the most interesting for us of course, of the abundant production by Sylvester and Cayley on determinants and everything connected with them, a production full of ingenious identities and impressive calculations.

Also (amongst other things) Grassmann discovers an algebra over the reals, the exterior algebra which still bears his name. His work, earlier even than that of Hamilton [19(a)], created in an almost complete moral solitude, remained for a long time little known, no doubt because of its originality, because also of the philosophical mists, in which it begins by enveloping itself and which for example at first deterred Möbius. Moved by preoccupations analogous to those of Hamilton but of greater import (and which, as he soon sees, are the same as those of Leibniz), Grassmann constructs a vast algebraico-geometric edifice, resting on a geometric or "intrinsic" conception (already more or less axiomatized) of nn-dimensional vector space; among the more elementary results at which he arrives, we quote for example the definition of linear independence of vectors, that of dimension and the fundamental relation

dim⁡V+dim⁡W=dim⁡(V+W)+dim⁡(V∩W) \dim V + \dim W = \dim(V + W) + \dim(V \cap W)

(loc. cit., p. 209; cf. [19(b)], p. 21). But it is especially exterior multiplication, then inner multiplication, of multivectors which provide him with the tools with which he easily treats first the problems of linear algebra proper and then those relating to the Euclidean structure, that is orthogonality of vectors (where he finds the equivalent of duality, which he does not possess).

The other path opened up by Gauss in the study of hypercomplex systems is that starting from the complex integers a+bia + bi; after these follow quite naturally algebras or more general hypercomplex systems, over the ring Z\mathbf{Z} of integers and over the field Q\mathbf{Q} of rationals, and first of all those already envisaged by Gauss which are generated by roots of unity, then algebraic number fields and modules of algebraic integers: the former are the principal topic in the work of Kummer, the study of the latter was undertaken by Dirichlet, Hermite, Kronecker and Dedekind. Here, in contrast to what happens with algebras over the reals, it is not necessary to abandon any of the characteristic properties of commutative fields and attention was confined to the latter throughout the XIXth century. But linear properties and for example the search for the basis for the integers of the field (indispensable for a general definition of the discriminant) play an essential role at many points; and with Dedekind at any rate the methods are destined to become typically "hypercomplex"; Dedekind himself moreover, without setting himself the problem of algebras in general, is conscious of this character of his works and of what relates them for example to the results of Weierstrass on hypercomplex systems over the reals ([24], in particular vol. 2, p. 1). At the same time the determination of the structure of the multiplicative group of units in an algebraic number field, effected by Dirichlet in some famous notes [15] and almost at the same time by Hermite, was vitally important in clarifying ideas on modules over Z\mathbf{Z}, their generating systems and, their bases (when such exist). Then the notion of ideal, defined by Dedekind in algebraic number fields (as a module over the ring of integers of the field), whilst Kronecker introduces in polynomial rings (under the name of "systems of modules") an equivalent notion, gives the first examples of modules over more general rings than Z\mathbf{Z}; and in the work of the same authors, and then Hilbert, in particular cases the notion of group with operators is slowly isolated, and the possibility of constructing always from such a group a module over a suitably defined ring.

At the same time, the arithmetico-algebraic study of quadratic bilinear forms and their "reduction" (or, what amounts to the same, of matrices and their "invariants") leads to the discovery of the general principles on the solution of systems of linear equations, principles which due to the lack of the notion of rank, had escaped Jacobi.\footnote{Concerning the classification of systems of nn equations in nn unknowns when the determinant is zero, he says ([16(a)], p. 370): "paullo prolixum videtur negotium" (it could not be elucidated briefly).} The problem of the solution in integers of systems of linear equations with integral coefficients is attacked and solved, first in a special case by Hermite and then in all its generality by H. J. Smith [25]; the results of the latter are found again, only in 1878, by Frobenius, in the framework of a vast programme of research instituted by Kronecker and in which Weierstrass also participates; incidentally during the course of these works, Kronecker gives definitive form to the theorems on linear systems with real (or complex) coefficients, which are also elucidated, in an obscure manual, with the minute care characteristic of him, by the famous author of Alice in Wonderland; as for Kronecker, he disdains to publish these results and leaves them to his colleagues and disciples; the word "rank" itself is only introduced by Frobenius. Also in the course of their teaching at the University of Berlin Kronecker [26] and Weierstrass introduce the "axiomatic" definition of determinants (as an alternating multilinear function of nn vectors in nn-dimensional space, normed so that it takes the value 1 at the unit matrix), a definition equivalent to that derived from Grassmann’s calculus and to that adopted in this Treatise; again during his courses Kronecker, without feeling the need to give it a name and in a still non-intrinsic form, introduces the tensor product of spaces and the “Kronecker” product of matrices (the linear substitution induced on a tensor product by given linear substitutions applied to the factors).

This research cannot be separated from the theory of invariants created by Cayley, Hermite and Sylvester (the “invariant trinity” of which Hermite later speaks in his letters) and which, from a modern point of view, is above all a theory of representations of the linear group. Here there comes to light, as the algebraic equivalent of duality in projective geometry, the distinction between series of cogredient and contragredient variables, that is vectors in a space and vectors in the dual space; and, after attention has been turned first to forms of low degree and then of arbitrary degree, in 2 and 3 variables, almost without delay bilinear, then multilinear forms are examined in several series of “cogredient” or “contragredient” variables, which is equivalent to the introduction of tensors; the latter becomes explicit and is popularized when, under the inspiration of the theory of invariants, Ricci and Levi-Civitá, in 1900, introduce into differential geometry “tensor calculus” [28], which later came into great vogue following its use by the “relativist” physicists. Again the progressive intermingling of the theory of invariants, differential geometry and the theory of partial differential equations (especially the so-called problem of Pfaff and its generalizations) slowly leads geometers to consider alternating bilinear forms of differentials, in particular the “bilinear covariant” of a form of degree 1 (introduced in 1870 by Lipschitz and then studied by Frobenius), to result in the creation by E. Cartan [29] and Poincaré [30] of the calculus of exterior differential forms. Poincaré introduces the latter, in order to form his integral invariants, as the expressions which appear in multiple integrals, whilst Cartan, guided no doubt by his research on algebras, introduces them in a more formal way, but without failing to observe that the algebraic part of their calculus is identical with Grassmann’s exterior multiplication (whence the name which he adopts), thus definitively restoring the work of the latter to its rightful place. The translation, into the notation of tensor calculus, of exterior differential forms, moreover shows immediately their connection with skew-symmetric tensors, which, once a purely algebraic point of view is adopted, shows that they are for alternating multilinear forms what covariant tensors are for arbitrary multilinear forms; this aspect is further clarified with the modern theory of representations of the linear group; and thus, for example, the substantial identity between the definition of determinants given by Weierstrass and Kronecker and that resulting from Grassmann’s calculus is recognized.

We thus arrive at the modern period, where the axiomatic method and the notion of structure (at first vaguely perceived, and defined only recently) allow us to separate concepts which until then had been inextricably mixed, to formulate what was vague or left to intuition and to prove with proper generality theorems which were known only in special cases. Peano, one of the creators of the axiomatic method and also one of the first mathematicians fully to appreciate the work of Grassmann, gives as early as 1888 ([27], Chapter IX) the axiomatic definition of vector spaces (finite-dimensional or otherwise) over the field of real numbers and, in a completely modern notation, of linear mappings of one such space into another; a little later, Pincherle seeks to develop applications of linear algebra, thus conceived, to the theory of functions, in a direction it is true which has not been very fruitful; at least his point of view allows him to recognize “Lagrange’s adjoint” as a special case of the transposition of linear mappings: which appears soon, still more clearly, and for partial differential equations as well as for differential equations, in the course of the memorable works of Hilbert and his school on Hilbert space, and its applications to analysis. It is on that occasion that Toeplitz [31], also introducing (but by means of coordinates) the most general vector space over the reals, makes the fundamental observation that the theory of determinants is not needed to prove the principal theorems of linear algebra, which allows these to be extended without difficulty to infinite-dimensional spaces; and he also indicates that linear algebra thus understood can of course be applied to an arbitrary commutative base field.

On the other hand, with the introduction by Banach, in 1922, of the spaces bearing his name,\footnote{These are complete normed vector spaces over the field of real numbers or that of complex numbers.} spaces not isomorphic to their dual are encountered, albeit in a problem which is topological as much as it is algebraic. Already between a finite-dimensional vector space and its dual there is no “canonical” isomorphism, that is determined by its structure, which had long been reflected in the distinction between cogredient and contragredient. Nevertheless it seems beyond doubt that the distinction between a space and its dual was definitively established only after the work of Banach and its school; also in these works the importance of the notion of codimension comes to light. As for duality or “orthogonality” between the vector subspaces of a space and those of its dual, the way in which it is formulated today presents not just a superficial analogy with the modern formulation of the principal theorem of Galois theory (cf. Algebra, V) and with so-called Pontrjagin duality in locally compact Abelian groups; the latter goes back to Weber, who, in the course of arithmetical researches, lays in 1886 its foundations for finite groups; in Galois theory the “duality” between subgroups and subfields takes form in the work of Dedekind and Hilbert; and orthogonality between vector subspaces derives visibly, first from duality between linear varieties in projective geometry and also from the notion and properties of completely orthogonal varieties in a Euclidean space or a Hilbert space (whence its name). All these strands are reassembled in the contemporary period, in the hands of algebraists such as

E. Noether, Artin and Hasse and topologists such as Pontrjagin and Whitney (not without the ones influencing the others) to arrive, in each of these fields, at the stage of knowledge whose results are expounded in this Treatise.

At the same time a critical examination is made, which is destined to eliminate, on each point, the hypotheses which are not completely indispensable, and especially those which would close the way to certain applications. Thus the possibility is perceived of substituting rings for fields in the notion of vector spaces and, creating the general notion of module, of treating at the same time these spaces, Abelian groups, the particular modules already studied by Kronecker, Weierstrass, Dedekind and Steinitz and even groups with operators and for example of applying the Jordan-Hölder theorem to them; at the same time, with the distinction between right and left modules, we pass to the non-commutative, which arises from the modern development of the theory of algebras by the American school (Wedderburn, Dickson) and especially the German school (E. Noether, E. Artin).

BIBLIOGRAPHY

1. O. Neugebauer, Vorlesungen über Geschichte der antiken Mathematik, Vol. I: Vorgriechische Mathematik, Berlin (Springer), 1934. 2. Euclidis Elementa, 5 vols., ed. J. L. Heiberg, Lipsiae (Teubner), 1883–88. 2 bis. T. L. Heath, The thirteen books of Euclid’s Elements ..., 3 vols., Cambridge, 1908. 3. Francisci Vietae, Opera mathematica ..., Lugduni Batavorum (Elzevir), 1646. 4. P. Fermat, Oeuvres, vol. I, Paris (Gauthier-Villars), 1891: (a) Ad locos planos et solidos Isagoge (pp. 91–110; French transl. ibid., vol. III, p. 85); (b) Appendix ad methodum ... (pp. 184–188; French transl., ibid., vol. III, p. 159). 5. R. Descartes, La géométrie, Leyde (Jan Maire), 1637 (=Oeuvres, ed. Ch. Adam and P. Tannery, vol. VI, Paris (L. Cerf), 1902). 6. G. Desargues, Oeuvres ..., vol. I, Paris (Leiber), 1864: Brouillon proiect d’une atteinte aux éuénemens des rencontres d’un cône auec un plan (pp. 103–230). 7. G. W. Leibniz, Mathematische Schriften, ed. C. I. Gerhardt, vol. I, Berlin (Asher), 1849. 8. L. Euler: (a) Introductio in Analysin Infinitorum, vol. 2, Lausannae, 1748 (=Opera Omnia (1), vol. IX, Zürich-Leipzig-Berlin (O. Füssli and B. G. Teubner), 1945); (b) Institutionum Calculi Integralis, vol. 2, Petropoli, 1769 (=Opera Omnia (1), vol. XII, Leipzig-Berlin (B. G. Teubner), 1914). 9. J.-L. Lagrange, Oeuvres, Paris (Gauthier-Villars), 1867–1892: (a) Solutions analytiques de quelques problèmes sur les pyramides triangulaires, vol. III, pp. 661–692; (b) Solution de différents problèmes de calcul intégral, vol. I, p. 471; (c) Recherches d’arithmétique, vol. III, pp. 695–795.

10. G. Cramer, Introduction à l’analyse des lignes courbes, Geneva (Cramer and Philibert), 1750.

11. E. Bezout, Théorie générale des équations algébriques, Paris, 1779.

12. C. F. Gauss, Werke, Göttingen, 1870–1927: (a) Disquisitiones arithmeticae, vol. I; (b) Selbstanzeige zur Theoria residuorum biquadraticorum, Commentatio secunda, vol. II, pp. 169–178.

13. A.-L. Cauchy, Mémoire sur les fonctions qui ne peuvent obtenir que deux valeurs égales et de signes contraires par suite des transpositions opérées entre les variables qu’elles renferment, J. Ec. Polytech., cahier 17 (volume X), 1815, pp. 29–112 (=Oeuvres complètes (2), vol. I, Paris (Gauthier-Villars), 1905, pp. 91–169).

14. A.-L. Cauchy, in Leçons de calcul différentiel et de calcul intégral, rédigées principalement d’après les méthodes de M. A.-L. Cauchy by Abbé Moigno, vol. II, Paris, 1844.

15. P. G. Lejeune-Dirichlet, Werke, vol. I, Berlin (G. Reimer), 1889, pp. 619–644.

16. C. G. J. Jacobi, Gesammelte Werke, Berlin (G. Reimer), 1881–1891: (a) De formatione et proprietatibus determinantium, vol. III, pp. 355–392; (b) De functionibus duarum variabilium . . ., vol. II, pp. 25–50.

17. M. Chasles, Aperçu historique sur l’origine et le développement des méthodes en géométrie . . ., Bruxelles, 1837.

18. A. F. Möbius, Der baryzentrische Calcul . . ., Leipzig, 1827 (=Gesammelte Werke, vol. I, Leipzig (Hirzel), 1885).

19. H. Grassmann: (a) Die lineale Ausdehnungslehre, ein neuer Zweig der Mathematik, dargestellt und durch Anwendungen auf die übrigen Zweige der Mathematik, wie auch auf die Statik, Mechanik, die Lehre vom Magnetismus und die Kristallonomie erläutert, Leipzig (Wigand), 1844 (=Gesammelte Werke, vol. I, 1st Part, Leipzig (Teubner), 1894); (b) Die Ausdehnungslehre, vollständig und in strenger Form bearbeitet, Berlin, 1862 (=Gesammelte Werke, vol. I, 2nd Part, Leipzig (Teubner), 1896).

20. W. R. Hamilton, Lectures on quaternions, Dublin, 1853.

21. J. J. Sylvester, Collected Mathematical Papers, vol. I, Cambridge, 1904: No. 25, Addition to the articles . . ., pp. 145–151 (=Phil. Mag., 1850).

22. A. Cayley, Collected Mathematical Papers, Cambridge, 1889–1898: (a) Sur quelques théorèmes de la géométrie de position, vol. I, pp. 317–328 (=Crelle’s J., vol. XXXI (1846), pp. 213–227); (b) A memoir on the theory of matrices, vol. II, pp. 475–496 (=Phil. Trans., 1858).

23. K. Weierstrass, Mathematische Werke, vol. II, Berlin, (Mayer und Müller),

1895: Zur Theorie des aus nn Haupteinheiten gebildeten complexen Grössen, pp. 311–332. 24. R. Dedekind, Gesammelte mathematische Werke, 3 vols., Braunschweig (Vieweg), 1930–32. 25. H. J. Smith, Collected Mathematical Papers, vol. I, Oxford, 1894: On systems of linear indeterminate equations and congruences, p. 367 (=Phil. Trans., 1861). 26. L. Kronecker, Vorlesungen über die Theorie der Determinanten . . ., Leipzig (Teubner), 1903. 27. G. Peano, Calcolo geometrico secondo l’Ausdehnungstheorie di Grassmann preceduto dalle operazioni della logica deduttiva, Torino, 1888. 28. G. Ricci and T. Levi-Civita, Méthodes de calcul différentiel absolu et leurs applications, Math. Ann., vol. LIV (1901), p. 125. 29. E. Cartan, Sur certaines expressions différentielles et le problème de Pfaff, Ann. E.N.S. (3), vol. XVI (1899), pp. 239–332 (=Oeuvres complètes, vol. II_1, Paris (Gauthier-Villars), 1953, pp. 303–396). 30. H. Poincaré, Les méthodes nouvelles de la mécanique céleste, vol. III, Paris (Gauthier-Villars), 1899, Chapter XXII. 31. O. Toeplitz, Ueber die Auflösung unendlichvieler linearer Gleichungen mit unendlichvielen Unbekannten, Rend. Circ. Mat. Pal., vol. XXVIII (1909), pp. 88–96.

Transcribed from the printed edition, 1998, Springer. Not translated.