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Problems in Modern Galois Theory111The abstract of this report was given as a lecture at the 1932 International Congress of Mathematics in Zurich.

Nikolai Chebotaryov, Translation by Yonathan Stone The translator would like to thank Jesse Wolfson for suggesting this and for providing helpful feedback on earlier drafts. In addition, this translation was supported in part by NSF Grant DMS-1944862.
(First published in 1932, translated in 2020)

Given the recent centennial of Evariste Galois’ death, I am presented with the opportunity to present the current state of his most important creation, known by the name of “Galois theory.” At the same time, I will try to make a handful of predictions regarding future developments in Galois theory. The original goal in the development of Galois theory, namely the problem of representing the roots of algebraic equations using radical expressions, was very nearly reached by both Galois and his early followers. The main tools used by Galois in his investigations, the description of algebraic number fields by their corresponding groups, managed to demonstrate its power additionally for distant branches of mathematical analysis. In this vein, new topics such as “Riemann surfaces,” “automorphic functions,” “continuous transformation groups,” and so on have been created.

Besides this there are also new problems in classical Galois theory itself, which in turn prompt a deeper analysis of Galois’ theory’s core ideas. The problem of finding equations with prescribed [Galois] groups has required studying the theory of generalized rational functions (the problem of Lüroth-Steinitz.) A generalization of the problem of solving by radicals, namely the problem of Klein forms, has linked the theory of finite groups with the theory of continuous groups. Connecting both of these branches of group theory is “Linear group theory,” a true bridge.

In this report, I would like to present the current machinery available, which may aid the mastery of problems in Galois theory. In doing so I will broaden the definition of “Galois theory” slightly beyond describing the usual application of group theory to algebraic equations. That is, I will include all questions juxtaposing the notions of “the rational” and the “the algebraic irrational.” Among this are some very nice results concerning algebraic function fields of several variables, which until now have only been facilitated using methods in algebraic geometry. We can thank the old German and the Italian geometers for solving some of these problems with the help of algebraic geometry, whereas methods for solving such problems are not available to us algebraists.

I have based the selection of this material primarily on my own tastes, and make no claims regarding the objectivity of the following selection:

§1 Foundations of Galois Theory.
§2 Equations with prescribed [Galois] group.
§3 On the analytic form of prime numbers belonging to a prescribed permutation class.
§4 The resolvent problem.
§5 Further questions in the general theory of fields.

§1 Foundations of Galois Theory

  1. 1.

    One can separate the work which deals with the foundations of Galois theory into two types. The first of these includes the tasks which seek new paths to justify the classical Galois theory, while those of the second kind deepen the definition of the Galois group, facilitating its application to far more areas than is possible using just the classical theory.

  2. 2.

    Belonging to the first kind, the work of F. Mertens [50], S. Schatunowski [62], and A. Loewy [46, 47] is of particular note. Mertens develops the definition of the Galois group and proves the associated fundamental theorems without using the notion of the normal field [extension], the Galois resolvent, etc. He builds upon the definition of irreducibility in extended domains. Given an equation f(x)=0f(x)=0 with x1x_{1} as a root, he finds a factor f1(x;x1)f_{1}(x;x_{1}) of the polynomial f(x)xx1\frac{f(x)}{x-x_{1}} that is irreducible over K[x1]K[x_{1}]. He proceeds to find a K[x1,x2]K[x_{1},x_{2}]-irreducible factor of the polynomial f1(x;x1)xx2\frac{f_{1}(x;x_{1})}{x-x_{2}}, where x2x_{2} is a root of f1(x;x1)f_{1}(x;x_{1}). Continuing this process, he arrives at the family

    Z0=f(x),Z1=f1(x;x1),Z2=f2(x;x1,x2),,Zn1=fn1(x;x1,,xn1)Z_{0}=f(x),Z_{1}=f_{1}(x;x_{1}),Z_{2}=f_{2}(x;x_{1},x_{2}),...,Z_{n-1}=f_{n-1}(x;x_{1},...,x_{n-1}) (1.1)

    of polynomials, which forms a family of fundamental relations. A polynomial φ(x1,x2,,xn)\varphi(x_{1},x_{2},...,x_{n}) is then equal to zero (in the variables xix_{i}) if and only if it can be represented in the form

    P0Z0(x1)+P1Z1(x2)++Pn1Zn1(xn),P_{0}\cdot Z_{0}(x_{1})+P_{1}\cdot Z_{1}(x_{2})+...+P_{n-1}\cdot Z_{n-1}(x_{n}), (1.2)

    where the PiP_{i}’s are polynomials. The Galois group is thus defined to consist of those permutations that transform each of the Zi(xi+1)Z_{i}(x_{i+1}) into a polynomial of the form (1.2). The order of this Galois group is equal to the product of degrees of the polynomials in (1.1).

  3. 3.

    Schatunowski establishes a theory formally covering the same ideas as Mertens, yet at the same time assumes a much more general point of view. His work builds upon Kronecker’s idea of functional relations, which, given a root xix_{i} of the equation

    f(x)=xn+a1xn1++an1x+an=0,f(x)=x^{n}+a_{1}x^{n-1}+...+a_{n-1}x+a_{n}=0, (1.3)

    consists of considering any quantity depending on xix_{i} as a function of an undetermined variable, while taking congruence modulo f(x)f(x) as the equals sign. Since one considers functions of several roots of equation (1.3) in Galois theory, Schatunowski aims to construct a family of functional relations in the variables x1,,xnx_{1},...,x_{n}, such that the quotient according to these relations is isomorphic to the algebraic number field generated by the roots of equation (1.3). The ideal generated by

    ψ1=x1+x2++xn+a1,\displaystyle\psi_{1}=x_{1}+x_{2}+...+x_{n}+a_{1}, ψ2=x1x2++xn1xna2,,\displaystyle\psi_{2}=x_{1}x_{2}+...+x_{n-1}x_{n}-a_{2},..., (1.4)
    ψn=x1x2xn(1)nan\displaystyle\psi_{n}=x_{1}x_{2}...x_{n}-(-1)^{n}a_{n}

    is not suited for this, since the f(xi)f(x_{i}) are not 0\equiv 0 modulo this ideal. The ideal generated by

    f(x1),f(x2),,f(xn)f(x_{1}),f(x_{2}),...,f(x_{n}) (1.5)

    also fails to serve this purpose, since the statement

    ψi0( mod f(x1),f(x2),,f(xn))\psi_{i}\equiv 0(\text{ mod }f(x_{1}),f(x_{2}),...,f(x_{n}))

    fails to hold, whereas ψiV0( mod f(x1),f(x2),,f(xn))\psi_{i}V\equiv 0(\text{ mod }f(x_{1}),f(x_{2}),...,f(x_{n})) does hold, where VV denotes the Vandermonde determinant of x1,,xnx_{1},...,x_{n}. In accordance with modern convention we say that (1.4) and (1.5) are not prime ideals.
    Schatunowski constructs the desired system of relations by starting with what he calls Cauchy relations. One obtains these relations in the following manner: As the first relation one takes f(x1)f(x_{1}); as the second relation the quotient of the division of f(x1)f(x_{1}) by x1x2x_{1}-x_{2}; as the third relation the quotient of the second relation, ordered by powers of x2x_{2}, by x2x3x_{2}-x_{3}, etc. The Cauchy relations then give rise to residue classes which in turn are isomorphic to the corresponding number field if and only if equation (1.3) is without affect. [German: affektlos] In this case each of these ideals is irreducible over the ideal preceding it. If this is not the case Schatunowski considers the general Mertensian relations. The degrees of these relations provide information regarding the transivity and primitivity relations of equation (1.3). For instance, the [Galois] group is kk-times transitive whenever the first kk relations coincide with those of Cauchy.
    Schatonowski’s work contains the introductory foundations of what is known as the theory of polynomial ideals nowadays. It deals with the rings whose relations are reducible. Such a ring is called a “semifield” if one can adjoin a (finite) number of new relations such that the ring becomes a field.
    Paritcularly notable among terms introduced by Schatunowski is the notion of an extension of the second kind. He uses this to refer to rings that are obtained by adjoining a finite number of moduli to a base ring. In other words, one sets certain nonvanishing elements of the base ring equal to zero. It may be more natural to refer to these extensions as quotient rings, in accordance with the term quotient group. It is known that a field does not admit any extensions of the second kind. In this, it is assumed that all fields can only have characteristic zero. However, if we consider the prime characteristic pp, this fails upon adding the new modulus pp, and a field remains a field.
    Assuming the Mertens-Schatunowskian definition of the Galois group, one can easily prove the following theorem, originally due to I. Schur ([70], see also [80]):
    The [Galois] group of a factor field is a subgroup of the group of the original field.

  4. 4.

    The Loewyian justification of Galois theory has some overlap with the Mertens-Schatunowskian theory, in particular the avoiding the assumption of normal fields. Rather than taking a single primitive element, Loewy takes several algebraic elements as possible generators for a field PP, which he refers to as conductors222Translated from the German “Dirigenten”.-YS. The first conductor ρ1\rho_{1} is a root of an equation with coefficients in the domain of rationality; the second conductor is a root of an equation of the type f(ρ1;z)=0f(\rho_{1};z)=0; the third of the type f(ρ1,ρ2;z)=0f(\rho_{1},\rho_{2};z)=0, etc. Provided all these equations are irreducible, Loewy uses “transformations of the field PP” to refer to the replacement of a conductor ρi\rho_{i} with a conjugate root belonging to all equations in which ρi\rho_{i} occurs (which also necessitates the replacement of all subsequent conductors). He proves that such a transformation disturbs none of the relations between the conductors. However, it is in fact possible that such a transformation maps some elements of the field PP outside of PP. The transformations that map elements PP to PP form a group, which is called the group of automorphic transformations. From a group theoretic standpoint this means the following: A non-normal field PP is not at all determined by its [Galois] group; it is determined by its Galois group 𝔊\mathfrak{G} and the subgroup \mathfrak{H} corresponding to a primitive element of PP. The automorphic group of PP is isomorphic to 𝔎/\mathfrak{K}/\mathfrak{H}, where 𝔎\mathfrak{K} denotes the normalizer of \mathfrak{H} in 𝔊\mathfrak{G}. The collection of all transformations of PP, using the above definition, do not form a group in the familiar sense. Loewy calls these algebraic structures mixed groups and investigates their structural properties [47]. Each mixed group 𝔗\mathfrak{T} contains a kernel 𝔊\mathfrak{G} that is defined to be the largest ordinary group contained inside 𝔗\mathfrak{T} and consists of some of the cosets (residue classes) of 𝔊\mathfrak{G}. It is important, that a factor group of 𝔗\mathfrak{T} by any (not neccesarily normal) subgroup \mathfrak{H} of 𝔊\mathfrak{G} remains a mixed group, whose kernel is given by 𝔑/𝔊\mathfrak{N}/\mathfrak{G}, where 𝔑\mathfrak{N} denotes the normalizer of \mathfrak{H} in 𝔊\mathfrak{G}. These facts permit viewing a mixed group as a more adequate picture of a field.
    A similar group construction was introduced by H. Brandt [7], which is called the Brandt groupoid.

  5. 5.

    Before we transition to the work of the second kind, we must set out the modern notion of the term “Galois group”, which deviates from older notions. It is difficult for me to say who this new notion originates from. The older Galois theory views the elements of the Galois group, the transformations (or permutations), as interchanges among the roots of a generating equation (which may well be reducible), which do not disturb any relations between the roots. On the other hand, the modern Galois theory considers assignments that are simultaneously undergone by all elements of a field KK, without disturbing the established relations between them. In other words, each element of a Galois group is a map of a (normal) field KK to itself, or, as one says in group theory, an automorphism. That is, an assignment of all elements of a field to elements of the same field, such that sums and products and taken to sums and products respectively.

  6. 6.

    Of utmost importance in Galois theory is the mutual correspondance between subfields of KK and subgroups of its Galois group. More specifically one can formulate this in the following manner ([43]; [74], appendix; [3]): One assigns to each subfield UU of KK the largest subgroup (U)\mathfrak{H}(U) of 𝔊\mathfrak{G} which fixes all elements of UU. On the other hand one can assign to each subgroup \mathfrak{H} of 𝔊\mathfrak{G} the largest subfield U()U(\mathfrak{H}) of KK, whose elements remain unchanged by \mathfrak{H}. If U1>U2U_{1}>U_{2}, then (U1)<(U2)\mathfrak{H}(U_{1})<\mathfrak{H}(U_{2}), and vice-versa. Moreover it holds that

    U[(U)]>U,[U()]>.U[\mathfrak{H}(U)]>U,\mathfrak{H}[U(\mathfrak{H})]>\mathfrak{H}. (1.6)

    However, one can only readily develop Galois theory, whenever

    U[(U)]=U,U[\mathfrak{H}(U)]=U, (1.7)
    [U()]=.\mathfrak{H}[U(\mathfrak{H})]=\mathfrak{H}. (1.8)

    So that (1.8) holds, KK is required to be finite over its domain of rationality (Krull, [43]).
    So that (1.7) holds, KK must be of the first kind over its domain of rationality (Baer-Hasse, [74], appendix).
    If KK possesses the field of rational numbers as a subfield (one says that KK has characteristic zero), then KK is of the first kind in any case. On the other hand, if KK has characteristic pp (that is, there exists a prime number pp, that is equal to zero inside KK), then KK is of the first kind if and only if a generating element of KK satisfies an irreducible equation with entirely distinct roots333This coincides precisely with the modern notion of separability.-YS.
    K is finite over its domain of rationality, if there exists a finite number of basis elements, so that each element of KK has a linear representation with in terms of the basis elements and coefficients from the domain of rationality.

  7. 7.

    For the case of KK being infinite, Krull [43] broadened the fundamental theorem of Galois theory by considering only the closed subgroups of \mathfrak{H} in lieu of all subgroups. By this he means the following. Given γ\gamma an element of 𝔊\mathfrak{G} and xx a finite normal subfield of KK, a mapping of xx to itself is induced by γ\gamma. If both γ\gamma and γ\gamma^{*} induce the same mapping of xx, we say that γ\gamma^{*} is contained in an xx-neighborhood of γ\gamma. This definition of neighborhood satisfies all the Hausdorff neighborhood axioms:

    1. a)

      Each element γ\gamma is contained in each of its own neighborhoods.

    2. b)

      The intersection of two neighborhoods of γ\gamma contains a new neighborhood of γ\gamma. Moreover, it itself is a neighborhood of γ\gamma, since the intersection of the x1x_{1}- and x2x_{2}-neighborhoods is the x3x_{3}-neighborhood, where x3x_{3} is both finite and normal as it is the union444The author uses the German word “Vereinigung”, or union, but in this case the notion of a compositum of fields seems more appropriate.-YS of x1x_{1} and x2x_{2}.

    3. c)

      Given δ\delta an element of a xx-neighborhood of γ\gamma, there exists a neighborhood of δ\delta which is entirely contained inside the xx-neighborhood of γ\gamma. Moreover, the xx-neighborhoods of γ\gamma and δ\delta coincide, since they contain the largest number of elements of 𝔊\mathfrak{G} that act on the field xx in precisely the same way.

    If γ\gamma and δ\delta are distinct elements of 𝔊\mathfrak{G}, there exists a neighborhood of γ\gamma not containing the element δ\delta. This is because γ\gamma and δ\delta being distinct implies the existence of elements in KK that behave differently under γ\gamma and δ\delta. As each of these elements generates a finite field [extension], it follows that each of the fields corresponds to a different neighborhood of γ\gamma and δ\delta.
    This definition permits the definition of accumulation elements. Given \mathfrak{H} a subgroup of 𝔊\mathfrak{G}, an accumulation element of \mathfrak{H} should contain elements of \mathfrak{H} in each of its neighborhoods. An accumulation element of \mathfrak{H} is not necessarily contained in \mathfrak{H} itself. However, in the case where a subgroup \mathfrak{H} of 𝔊\mathfrak{G} contains all of its accumulation elements, it is called closed. Each group which corresponds to a subfield of KK is closed. Conversely, to each closed group \mathfrak{H} there is a corresponding subfield UU of KK, so that [U()]=\mathfrak{H}[U(\mathfrak{H})]=\mathfrak{H} holds true. Thus, in order to be able to broaden the fundamental theorems of Galois theory to infinite fields [extensions], one must only consider those subgroups of \mathfrak{H} which are closed.

  8. 8.

    The conditions for the presence of the relation (1.7) were investigated thoroughly by R. Baer [3]. He found that, in any case, there exists an intermediate field [extension] SS, which he called the rigid field between KK and the domain of rationality. The rigid field is characterized by KK being orderly (that is (1.8) always holds) when one takes SS to be the domain of rationality, while all elements of SS remain invariant under automorphisms of KK. I cannot elaborate on the additional interesting statements of this work here.

  9. 9.

    It is very difficult to define the Galois group in the case where the field in question KK has a higher degree of transcendence than its domain of rationality. The reason for this lies in the fact that the universal norm of such a field (that is the field, which contains all fields conjugate to subfields of KK) is an infinite field [extension] whose definition is difficult to summarize analytically. To theoretically construct a group which possesses the desired main properties of the Galois group, one can sketch the following scheme. Let x1,x2,,xnx_{1},x_{2},...,x_{n} be the generating elements of a field KK, among which certain algebraic relations may be established, which we will denote by (I). One can determine each subfield UU of KK in an analogous sense through generating elements ξ1,ξ2,,ξm\xi_{1},\xi_{2},...,\xi_{m}, where the ξi\xi_{i} are expressed rationally through the xix_{i}:

    ξi=xi(x1,x2,,xn)(i=1,2,,m).\xi_{i}=x_{i}(x_{1},x_{2},...,x_{n})\quad\quad(i=1,2,...,m).

    The equations

    ξi(x1,x2,,xn)=ξi(y1,y2,,yn)(i=1,2,,m)\xi_{i}(x_{1},x_{2},...,x_{n})=\xi_{i}(y_{1},y_{2},...,y_{n})\quad\quad(i=1,2,...,m) (II)

    determined a new field, whose generators [x1,x2,,xn;y1,y2,,yn;y1,y2,,yn;][x_{1},x_{2},...,x_{n};y_{1},y_{2},...,y_{n};y_{1}^{\prime},y_{2}^{\prime},...,y_{n}^{\prime};...] are related by the relations (I) and (II). This fields can be called the relative norm of KK (with respect to UU). The assignment of (x1,,xn)(x_{1},...,x_{n}) to (y1,,yn)(y_{1},...,y_{n}) is designated a transmutation of KK or a permutation of its relative norm. If UU runs through all subfields of KK, then the sought after universal norm is generated by the relative norms. The compositum of all previously constructed permutations is a group possessing all main features of the Galois group.

  10. 10.

    One can construct the Galois group of a field of algebraic functions in a slightly different manner. Instead of considering the functions of the field, one envisions the totality of their coordinate systems, which form a so-called absolute Riemann surface (see [86]). In this case each transformation of the Galois group assigns to each value of a function of KK a new value, such that the relations between values of different functions are preserved. As each function is determined by the totality of its values, such transformations also determine the functions to which the given functions are assigned. The various monodromy groups which do not disturb certain domains of rationality are contained in this group. It can very well occur that a transformation leads several functions of KK outside of KK. In the case of an independent variable this is reflected when a function determined up to a multiplicative constant by its zeroes and poles [of the form]

    f𝔭1𝔭2𝔭m𝔭1𝔭2𝔭mf\simeq\frac{\mathfrak{p}_{1}^{\prime}\mathfrak{p}_{2}^{\prime}...\mathfrak{p}_{m}^{\prime}}{\mathfrak{p}_{1}\mathfrak{p}_{2}...\mathfrak{p}_{m}}

    is assigned to a product

    𝔭1¯𝔭2¯𝔭m¯𝔭1¯𝔭2¯𝔭m¯\frac{\overline{\mathfrak{p}_{1}^{\prime}}\;\overline{\mathfrak{p}_{2}^{\prime}}\;...\overline{\mathfrak{p}_{m}^{\prime}}}{\overline{\mathfrak{p}_{1}}\;\overline{\mathfrak{p}_{2}}\;...\overline{\mathfrak{p}_{m}}}

    where the numerator and denominator are contained in different ideal classes. Each transformation assigning divisors to equivalent divisors belongs to the so-called group of intrinsic transformations [38], which play an analogous role to the group of automorphic transformations introduced by A. Loewy [47].

  11. 11.

    Of importance is the theory of algebraic functions of a group, which is closely related to the Galois group which has just been defined.
    Let 𝔲1𝔭,𝔭,𝔲2𝔭,𝔭,,𝔲p𝔭,𝔭\mathfrak{u}_{1}^{\mathfrak{p},\mathfrak{p}^{\prime}},\mathfrak{u}_{2}^{\mathfrak{p},\mathfrak{p}^{\prime}},...,\mathfrak{u}_{p}^{\mathfrak{p},\mathfrak{p}^{\prime}} be the linearly independent Abelian integrals of the first kind defined on the Riemann surface of KK. The Jacobi inversion problem consists in the solution of the system of equations

    𝔲i𝔭1,𝔭1+𝔲i𝔭2,𝔭2++𝔲i𝔭p,𝔭p𝔳i(i=1,2,,p),\mathfrak{u}_{i}^{\mathfrak{p}_{1},\mathfrak{p}_{1}^{\prime}}+\mathfrak{u}_{i}^{\mathfrak{p}_{2},\mathfrak{p}_{2}^{\prime}}+...+\mathfrak{u}_{i}^{\mathfrak{p}_{p},\mathfrak{p}_{p}^{\prime}}\equiv\mathfrak{v}_{i}\quad(i=1,2,...,p), (1.9)

    where the lower limits 𝔭i\mathfrak{p}_{i} are given and the upper limits 𝔭i\mathfrak{p}_{i}^{\prime} are sought for and the congruences are taking from the period systems as relations. When none of the points 𝔭i\mathfrak{p}_{i} are collinear, this problem is clearly solvable ([54];[4]). If we take the 𝔭i\mathfrak{p}_{i}, 𝔭i\mathfrak{p}_{i}^{\prime} to be coordinates of the points PP, PP^{\prime} in a pp-dimensional space, then each coordinate system of the parameters 𝔳i\mathfrak{v}_{i} determines a transformation assigning each point PP to a certain point PP^{\prime} (in this case one must not regard points differing by the order of their coordinate values as different, so that these points may be defined unambiguously using the values of the symmetric functions of 𝔭i\mathfrak{p}_{i}). The group of these transformations is locally isomorphic555The author uses the term im Kleinen isomorph, where the adjective im Kleinen seems to be a weaker statement that local when used to qualify other definitions. Whether this is the same as locally isomorphic seems uncertain and as such any clarification would be greatly appreciated.-YS to the pp-parameter group of translations and admits an analytical expression in terms of the addition formulas of the Abelian functions. It is a subgroup of an extended Galois group which transforms the coordinates of the point PP independently of each other. We will refer to this group as the Jacobian group in the sequel.

§2 Equations with prescribed [Galois] group

  1. 1.

    The problem of finding equations with prescribed [Galois] groups belongs to the most important problems of modern Galois theory and to this day has not been solved. It can be summarized in the following three ways:

    1. I.

      One finds any equations, whose [Galois] groups are isomorphic to a given group 𝔊\mathfrak{G}.

    2. II.

      One finds the most general parametric form of the coefficients of an equation whose [Galois] group is isomorphic to 𝔊\mathfrak{G} or a subgroup of 𝔊\mathfrak{G}. Being able to present the coefficients in this form should provide a necessary and sufficient condition for the [Galois] group of the equation to be isomorphic with 𝔊\mathfrak{G} or one of its subgroups.

    3. III.

      One outlines a procedure for the determination of equations, whose [Galois] group is isomorphic to 𝔊\mathfrak{G}. This procedure should produce all equations of this kind if continued sufficiently.

  2. 2.

    Problem II always admits a solution whenever the generalized Lüroth theorem (also called the rational minimal basis theorem) holds for a given group 𝔊\mathfrak{G}. This theorem may be formulated in the following manner:
    For Kn(x1,x2,,xn)K_{n}(x_{1},x_{2},...,x_{n}) the field of rational functions of the variables x1,x2,,xnx_{1},x_{2},...,x_{n}, every subfield of Kn(x1,x2,,xn)K_{n}(x_{1},x_{2},...,x_{n}) is isomorphic to Km(x1,x2,,xm)K_{m}(x_{1},x_{2},...,x_{m}) (mn)(m\leq n). (One can also say: this field is purely transcendental)
    This theorem was proven in the case n=1n=1 by Lüroth [48]. The proof for n=2n=2 was found by Castelnuovo [15]. Both G. Fano [21] and F. Enriques [20] found a counterexample to the case n=3n=3. However, the full scope of this theorem is not required for the solving Problem II. Restricting ourselves to the case where the subfield in question contains the field of elementary symmetric functions in x1,x2,,xnx_{1},x_{2},...,x_{n}, the validity of the theorem becomes fully equivalent to the solvability of task II. Until now the validity of this theorem “in a narrower setting” remains open (see [74], remark of B.L. Van der Waerden). If this also does not hold true in general, one can determine whether any abstractly given finite group is “Lürothian” or not. That is, whether the field K(a1,a2,,an;φ)K(a_{1},a_{2},...,a_{n};\varphi) is purely transcendental, where 𝔊\mathfrak{G} is represented as the permutation group of x1,x2,,xnx_{1},x_{2},...,x_{n}, a1,a2,,ana_{1},a_{2},...,a_{n} denote the elementary symmetric functions of x1,x2,,xnx_{1},x_{2},...,x_{n}, and φ\varphi is a function of x1,x2,,xnx_{1},x_{2},...,x_{n} belonging to 𝔊\mathfrak{G}.

  3. 3.

    E. Noether [55] deduced Problem I from Problem II by using Hilbert’s irreducibility theorem, which states for any irreducible polynomial one can choose numerical values for some of the variables so that the polynomial is irreducible in the remaining variables.
    One can tighten this result by not just deducing Problem I, but also Problem III from Problem II. For that one uses the following procedure specified by M. Bauer [5],[6]. It is known that the Galois group of an algebraic equation

    xn+a1xn1++an1x+an=0x^{n}+a_{1}x^{n-1}+...+a_{n-1}x+a_{n}=0 (2.1)

    is transformed into one of its subgroups when one regards the values of its domain of rationality not absolutely, but modulo a prime number (or a prime ideal). That is, one replaces the domain of rationality with one of its factor rings [16][70][80]. Then again, it also known that the Galois group of a field of characteristic pp [German: Primzahlmodulkongruenz, or prime number modular congruence] is cyclic, and that a generating permutation of the latter group consists of cycles, whose orders are equal to the irreducible components of our congruence. As a result, if

    f(x)Xn1(p)Xn2(p)Xnk(p)( mod p),f(x)\equiv X_{n_{1}}^{(p)}X_{n_{2}}^{(p)}...X_{n_{k}}^{(p)}\quad(\text{ mod }p), (2.2)

    holds, where Xni(p)X_{n_{i}}^{(p)} denotes a modulo pp irreducible polynomial of degree nin_{i} (n1+n2++nk=nn_{1}+n_{2}+...+n_{k}=n), then the [Galois] group of (2.1) contains a permutation whose cycles have order n1,n2,,nkn_{1},n_{2},...,n_{k}.

  4. 4.

    We assume that the field K(a1,a2,,an;φ)K(a_{1},a_{2},...,a_{n};\varphi) is purely transcendental (see the definitions in no. 2). There thus exist rational functions π1,π2,,πn\pi_{1},\pi_{2},...,\pi_{n} of a1,a2,,an;φa_{1},a_{2},...,a_{n};\varphi so that a1,a2,,an;φa_{1},a_{2},...,a_{n};\varphi can themselves be expressed in terms of the πi\pi_{i}. Next let 𝔊1,𝔊2,,𝔊s\mathfrak{G}_{1},\mathfrak{G}_{2},...,\mathfrak{G}_{s} be a system of subgroups of 𝔊\mathfrak{G}, so that each proper subgroup of 𝔊\mathfrak{G} is a subgroup of at least one of the 𝔊i\mathfrak{G}_{i}. Such a system can be certainly be constructed, for instance by taking all proper subgroups of 𝔊\mathfrak{G} as the 𝔊i\mathfrak{G}_{i}.
    Let φi\varphi_{i} be a function of x1,x2,,xnx_{1},x_{2},...,x_{n} belonging to 𝔊i\mathfrak{G}_{i} (i=1,2,..,s)(i=1,2,..,s), and let Fi(xi)F_{i}(x_{i}) be the polynomial of smallest degree, whose coefficients are rational functions of π1,π2,,πn\pi_{1},\pi_{2},...,\pi_{n} and for which φi\varphi_{i} is a root (i=1,2,,si=1,2,...,s). One can see that the degree of Fi(zi)F_{i}(z_{i}) is equal to the index (𝔊:𝔊i)(\mathfrak{G}:\mathfrak{G}_{i}) (i=1,2,,s)i=1,2,...,s).
    The [Galois] group of the equation Fi(zi)=0F_{i}(z_{i})=0, as a transitive permutation group, contains a permutation Si¯\overline{S_{i}}, which fixes no indices. This permutation corresponds to at least one permutation in 𝔊\mathfrak{G}. Let SiS_{i} be such a permutation, and let n1,n2,,nkn_{1},n_{2},...,n_{k} be the orders of its cycles. Take any prime number pi>n2p_{i}>n-2 and let

    f(x)Xn1(pi)Xn2(pi)Xnk(pi)( mod pi),f(x)\equiv X_{n_{1}}^{(p_{i})}X_{n_{2}}^{(p_{i})}...X_{n_{k}}^{(p_{i})}\quad(\text{ mod }p_{i}), (2.3)

    where Xnj(pi)X_{n_{j}}^{(p_{i})} denotes a modulo pip_{i} irreducible polynomial of degree njn_{j}. This determines the congruence classes modulo pip_{i} for the aia_{i}. Using the expressions for the coefficients of the equation F(z)=0F(z)=0, and we obtain the congruence

    F(z)0( mod pi),F(z)\equiv 0\quad(\text{ mod }p_{i}),

    which surely has one or more rational roots. Let φi\varphi_{i} be one of these roots. Then φi\varphi_{i} is transformed into the other rational roots by means of some permutations Σ1,Σ2,,Σν\Sigma_{1},\Sigma_{2},...,\Sigma_{\nu} of the symmetric permutation group 𝔖\mathfrak{S} of x1,,xnx_{1},...,x_{n}.
    By fixing (2.3), the “broad” class of permutations containing pip_{i} is determined, that is the totality of all permutations similar to SiS_{i} within 𝔖\mathfrak{S}. However, by fixing the congruence class of φi\varphi_{i}, we determine a division 666From the German Abteilung. According to Pioneers of Representation Theory: Frobenius, Burnside, Schur, and Brauer by Charles W. Curtis this is a term a term introduced by Frobenius. A division of a [Galois] group is the union of conjugacy classes of a given group element and all of the powers of this element coprime to its order.-YS. If 𝔘\mathfrak{U} is a division of SiS_{i}, then

    Σ11𝔘Σ11,Σ21𝔘Σ21,,Σν1𝔘Σν1\Sigma_{1}^{-1}\mathfrak{U}\Sigma_{1}^{-1},\Sigma_{2}^{-1}\mathfrak{U}\Sigma_{2}^{-1},...,\Sigma_{\nu}^{-1}\mathfrak{U}\Sigma_{\nu}^{-1}

    are precisely those divisions of 𝔊\mathfrak{G} possessing the cycle type of SiS_{i}. One of these division must correspond to the division of a permutation S¯i\overline{S}_{i} of our choosing. Plugging the values of φiΣj(j=1,2,,ν)\varphi_{i}^{\Sigma_{j}}(j=1,2,...,\nu) into the expressions for the coefficients of Fi(zi)0F_{i}(z_{i})\equiv 0, then at least one of the resulting congruences Fi(zi)0( mod pi)F_{i}(z_{i})\equiv 0(\text{ mod }p_{i}) corresponds to S¯i\overline{S}_{i} and thus has no rational roots. In other words pip_{i} belongs to a permutation class of K(x1,x2,,xn)K(x_{1},x_{2},...,x_{n}) which is not contained in 𝔊i\mathfrak{G}_{i}.
    Taking i=1,2,,si=1,2,...,s, we obtain the congruence classes modulo P=p1p2psP=p_{1}p_{2}...p_{s} for a1,a2,,an;φa_{1},a_{2},...,a_{n};\varphi and thus for π1,π2,,πn\pi_{1},\pi_{2},...,\pi_{n}. Fixing the πi\pi_{i} within the congruence classes we have just determined and plugging them into the equation f(x)=0f(x)=0, we obtain precisely 𝔊\mathfrak{G} as the group of this equation. On the one hand, it is contained in 𝔊\mathfrak{G} by virtue of the parametric expressions of the aia_{i}, but on the hand is not contained in any of the groups 𝔊1,𝔊2,,𝔊s\mathfrak{G}_{1},\mathfrak{G}_{2},...,\mathfrak{G}_{s} due to the established congruence conditions.

  5. 5.

    In particular, if one wants to construct equations without affect, one can follow a process due to M. Bauer. Take three arbitrary prime numbers p,q,rp,q,r (rn2r\geq n-2) and impose the following three congruence conditions on the polynomial f(x)f(x):

    f(x)\displaystyle f(x) Xn(p)(mod) p,\displaystyle\equiv X_{n}^{(p)}\quad\text{(mod) $p$},
    f(x)\displaystyle f(x) Xn1(q)(xb)(mod) q,\displaystyle\equiv X_{n-1}^{(q)}(x-b)\quad\text{(mod) $q$},
    f(x)\displaystyle f(x) X2(r)(xb1)(xb2)(xbn2)(mod) r.\displaystyle\equiv X_{2}^{(r)}(x-b_{1})(x-b_{2})...(x-b_{n-2})\quad\text{(mod) $r$}.

    The [Galois] group of the equation f(x)=0f(x)=0 thus contains an nn-cycle, an (n1)(n-1)-cycle and a transposition and thus the symmetric group [5][6][80].

  6. 6.

    The procedure outlined in No. 4 allows the construction of all possible equations with [Galois] group 𝔊\mathfrak{G} provided one continues the process sufficiently. This follows from the following result of Frobenius [23]:
    If the [Galois] group of the equation f(x)=0f(x)=0 contains a permutation with the cycles of length n1,n2,,nkn_{1},n_{2},...,n_{k} (Σni=n)\Sigma n_{i}=n), then there exist infinitely many prime numbers pp such that the congruence f(x)0 (mod p)f(x)\equiv 0\text{ (mod $p$)} splits into irreducible polynomials of degree n1,n2,,nkn_{1},n_{2},...,n_{k}.
    The somewhat vague term “all equations” can be made precise by giving ourselves the problem of finding all equations with [Galois] group 𝔊\mathfrak{G}, such that their coefficients don’t exceed a certain bound. To this end one must tighten the result of Frobenius in the following sense:
    One finds bounds under which a prescribed number of prime numbers with the desired properties are located.
    Such bounds have been provided by L. Kronecker [42] and F. Mertens [49] in the case of arithmetic progressions. I have carried out this estimate for the problem of Frobenius [81]. The result is as follows. If

    x=Max{2(2Adgdhd+2W)1a}x=\text{Max}\left\{2\left(\frac{2A_{d}}{g_{d}h_{d}}+2W\right)^{\tfrac{1}{a}}\right\} (2.4)

    for all dfd\mid f, then the interval (1,x)(1,x) surely contains VV prime numbers belonging to the division of SS. The constants Ad,gd,hd,WA_{d},g_{d},h_{d},W depend on certain subfields of KK and on the number VV. In order to express this bound explicitly in terms of the coefficients of equation (2.1), it is neccesary to estimate certain constants of K. R. Remak [61] very recently constructed an upper and a lower bound for the regulator of a field, which is particularly important for estimating formula (2.4).

  7. 7.

    If we seek only a solution to Problem I the solvability of Lüroth’s problem is unneccesary. If φ\varphi is a function belonging to 𝔊\mathfrak{G} which satisfies the equation F(φ)=0F(\varphi)=0, then the coefficients of the polynomial F(φ)F(\varphi) are given by rational functions of the coefficients a1,a2,,ana_{1},a_{2},...,a_{n} of the polynomial f(x).f(x). Taking f(x)Xn1(pj)Xn2(pj)Xnk(pj)(mod pj)f(x)\equiv X_{n_{1}}^{(p_{j})}X_{n_{2}}^{(p_{j})}...X_{n_{k}}^{(p_{j})}\quad\text{(mod $p_{j}$)}, we can determine the aia_{i} modulo pjp_{j}. Plugging these values into the congruence F(z)0(mod pj)F(z)\equiv 0\quad\text{(mod $p_{j}$)}, we obtain at least one rational root. If the congruence has multiple roots, we choose the one that corresponds to the desired division. Letting jj run through 1,2,,s1,2,...,s, we can determine a1,a2,,an;φa_{1},a_{2},...,a_{n};\varphi moduli p1,p2,,psp_{1},p_{2},...,p_{s} and thus modulo P=p1p2psP=p_{1}p_{2}...p_{s}, and can thus be represented in the form ai=ai(0)+Ptia_{i}=a_{i}^{(0)}+Pt_{i}, φ=ϖ0+Pu\varphi=\varpi_{0}+Pu, where a1(0),a2(0),,an(0);φ0a_{1}^{(0)},a_{2}^{(0)},...,a_{n}^{(0)};\varphi_{0} denote constants. Substituting this into the equation F(φ)=0F(\varphi)=0, we obtain the Diophantine equation Φ(t1,t2,,tn;u)=0\Phi(t_{1},t_{2},...,t_{n};u)=0. The Problem now follows from the solution of this equation. Note that this equation possesses the following properties:

    1. i)

      It can always be solved using fractions. That is, one can replace the aia_{i} with the elementary symmetric functions of the nn arbitrary rational numbers. This means the solution has nn “degrees of freedom.”

    2. ii)

      It can always be solved using pp-adic numbers, where the prime number pp can be chosen arbitrarily.

    The solvability of the equation Φ=0\Phi=0 does not depend on the choice of function belonging to 𝔊\mathfrak{G}.

  8. 8.

    Much work has been devoted to the solution of the problems in question in the cases of a few special groups. In the first place we have the work of D. Hilbert [35], in which Problem I is solved for symmetric and alternating groups of any order using the irreducibility theorem. The genuine construction of equations with alternating groups was recently carried out to near completion by I. Schur [72]. That is, given n0mod 4n\equiv 0\text{mod $4$}, Schur shows that the equation

    En(x)=1+x1!+x22!++xnn!=0E_{n}(x)=1+\frac{x}{1!}+\frac{x^{2}}{2!}+...+\frac{x^{n}}{n!}=0

    possesses the alternating group as its Galois group. On the other hand he shows (Crelle: 165, 1931) that when n1(mod) 2n\equiv 1\text{(mod) 2}, the equation

    1(n1)x2!+(n2)x33!+(1)nxn(n+1)!=01-{n\choose 1}\frac{x}{2!}+{n\choose 2}\frac{x^{3}}{3!}-...+(-1)^{n}\frac{x^{n}}{(n+1)!}=0

    also has the alternating group as its Galois group.

  9. 9.

    In the solution of Problem II it is important to solve Lüroth’s problem using rational functions with rational coefficients. This question in the case of solvable groups of prime degree is addressed in the work of S. Breuer [10][11] and Ph. Furtwängler [27]. Furtwängler proposed the following sufficient condition in the case of cyclic groups of prime degree pp:

    The problem permits a solution whenever it is possible to construct an integer number system e0,e1,,ep2e_{0},e_{1},...,e_{p-2}, such that 1)1) the Hankel determinant is

    |e0,e1,,ep2ep2,e0,,ep3e1,e2,,e0|=±p,\left|\begin{matrix}e_{0},&e_{1},&...,&e_{p-2}\\ e_{p-2},&e_{0},&...,&e_{p-3}\\ ...&...&...&...\\ e_{1},&e_{2},&...,&e_{0}\end{matrix}\right|=\pm p,

    and 2)2) the congruences i=0p2eigi0(mod p)\sum\limits_{i=0}^{p-2}e_{i}g^{i}\equiv 0\text{(mod $p$)} hold, where gg is a primitive root of pp.
    This criterion is not always satisfied, for instance in the case of p=47p=47. Later, Furtwängler gives some general instructions for the construction of rational minimal bases of metacyclic groups.
    Breuer derived several similar criteria by using his theorem about the decomposition of a field of rational functions of nn variables into two subfields, where one depends on the full metacyclic functions of the generating variables.

  10. 10.

    Problems I and III have been extended to the setting of relative fields. First of all, the solution of problem III can be regarded as solved for relative fields when a known rational basis contains certain roots of unity in the coefficients rather than being rational-valued (see for instance E. Fischer, [22]). This is however not an extension of the problem. A solution to problems I and III can only be considered a satisfactory extension to relative fields if we are capable of also saying something about the absolute Galois group.
    One can call the work of O. Ore [57] and H. Hasse [31][30] as the first in this direction, even though they are not directly concerned with this problem. Hasse starts with a number field kk and a number of its prime ideals 𝔭i\mathfrak{p}_{i}. He then finds infinitely many extension fields KK, in which the 𝔭i\mathfrak{p}_{i} decompose into prime ideals of prescribed order and multiplicity. He then significantly tightens this result by taking the prescribed decompositions to be regular and requires K/kK/k to be relatively abelian. He provides the existence proof under certain restrictive conditions.

  11. 11.

    The general form of problem I can be formulated for relative fields in the following sense (see [83]):
    Problem A. Let an algebraic number field kk be given, whose [Galois] group [over \mathbb{Q}] is given by 𝔤\mathfrak{g}. Furthermore, let an abstract group 𝔊\mathfrak{G} and a normal subgroup \mathfrak{H} be given, such that the factor group 𝔊/\mathfrak{G}/\mathfrak{H} is isomorphic to 𝔤\mathfrak{g}. One must find neccesary and sufficient conditions such that there exists an extension field KK of kk whose [Galois] group [over \mathbb{Q}] is isomorphic to 𝔊\mathfrak{G}.
    The following example shows that this problem is not solvable in a few cases. Let kk be cyclic of prime degree ll. Let 𝔊\mathfrak{G} be cyclic of order l2l^{2}. The critical prime numbers of kk are clearly 1(mod l)\equiv 1(\text{mod }l), but not 1(mod l2)\equiv 1(\text{mod }l^{2}). It follows from the number theoretic monodromy theorem that KK contains at least one inertia group of order l2l^{2} (see [82]). The prime number pp corresponding to this inertia group must also be critical in kk, which is impossible since it is known that it satisfies the congruence p1(mod l2)p\equiv 1\quad(\text{mod }l^{2}).
    This example also shows that the solvability of problem A is not just determined by the structure of the group 𝔊\mathfrak{G} but also via certain arithmetic properties of the field kk.

  12. 12.

    Especially important results regarding solving problem A concerning abelian groups were obtained by A. Scholz [64][63]. His investigations are mostly concerned with two-step solvable groups (that is, groups whose commutator subgroups are abelian) and are far-reaching in two directions. First of all he established a very utilitarian classification of two-tiered groups. The easiest of his classes, which he called disposition groups, allows for a solution to problem A independently of the arithmetic properties of the field kk [64]. One can define the disposition group as a group 𝔊\mathfrak{G}, whose normal abelian subgroups \mathfrak{H} are the direct product of all cyclic groups that that are conjugated by them. In addition each of these cyclic groups is required to have exactly \mathfrak{H} as its normalizer.
    Scholz proved the following two theorems on disposition groups:

    1. i)

      A disposition group 𝔊\mathfrak{G} is fully determined as soon as one knows the group 𝔊/\mathfrak{G}/\mathfrak{H} and the order of a generating element of \mathfrak{H}.

    2. ii)

      Given an algebraic number field with [Galois] group 𝔊/\mathfrak{G}/\mathfrak{H}, one can always find a extension field KK, whose [Galois] group is isomorphic to 𝔊\mathfrak{G}.

    Scholz later showed that the first of these theorems can be expanded to the case where neither 𝔊/\mathfrak{G}/\mathfrak{H} nor \mathfrak{H} are required to be abelian, but are completely arbitrary.
    Secondly, Scholz investigated other types of two-tiered groups extensively [63]. He namely found two maximal types among all two-tiered groups (that is those types, such that every two-tiered group can be represented as a factor group or a product of groups of this type): ring groups and branch groups. Ring groups are always factor groups of certain powers of disposition groups. Branch groups on the other hand possess a feature that does not allow such a representation: their commutator subgroup is not properly contained in any abelian subgroup. There the question of whether relative fields with [Galois] branch groups exist remains open.

  13. 13.

    I have made a contribution towards problem A [83]. In this I somewhat broadened the definition of the disposition group by throwing out the requirement that each generating cyclic subgroup of \mathfrak{H} permits no normalizer besides 𝔊\mathfrak{G}. From this arise the so-called Scholz groups, corresponding to the purely branched fields (that is those containing no unbranched extension fields of kk) with relative discriminants, whose prime ideal divisors within kk are not critical. The question of the uniqueness of a Scholz group given the factor group 𝔊/\mathfrak{G}/\mathfrak{H}, the order of a generating element of \mathfrak{H} and its normalizer, remains open. The question of the existence of a relative field with a given Scholz group can be reduced to to the existence of principal prime ideals 𝔭\mathfrak{p} with prescribed values of a Hasse norm remainder symbol(p,K𝔭)\left(\frac{p,K}{\mathfrak{p}}\right) (see Hasse [32] III). However this question exceeds the scope of the currently known analytical ideal theory.

  14. 14.

    If the group 𝔊\mathfrak{G} does not belong to the type of Scholz group, then one can only expect the existence of a corresponding extension field when it contains an absolute Teilklassenkörper or its relatively critical prime ideals are also critical within kk. In this case we are subject to the full control of the individual oddities of the field kk.
    The [Galois] groups the of absolute class fields are also not allowed to be completely arbitrary. On the one hand they are restricted by the aforementioned monodromy theorem, due to which all interia groups generate the full Galois group of the field, while the interia groups of a relatively unbranched field induce an unambiguous mapping on the inertia groups of the base field kk. Operating on this principle, I carried out a classification of the possible types of [Galois] groups of absolute class fields [82]. On the other hand, F. Pollaczek [60] and Scholz [66] discovered and developed a restriction of the absolute class fields based on the properties of the Grundeinheitensystem.

§3 On the analytic form of prime numbers belonging to a prescribed permutation class

  1. 1.

    It is known that an algebraic number field is not fully determined by its Galois group. The known invariants that fully determine a field are the so-called Artin symbols (K𝔭)\left(\frac{K}{\mathfrak{p}}\right) ([32] III, p. 6), that is the permutation classes containing individual prime numbers. There are infinitely many such invariants, which implies that they cannot be independent from one another. The existing relations between them can be derived provided we know the analytical form in which we can represent the prime numbers belonging to certain permutation classes, that is corresponding to the same value (K𝔭)\left(\frac{K}{\mathfrak{p}}\right). It can be proven, that such analytical forms depend on the structural properties of the corresponding [Galois] groups 𝔊\mathfrak{G}. This connection yields a deep insight into the arithmetic structure of a group with known Galois group.

  2. 2.

    First I will recall the classical case of an abelian field. For a prime number to belong to a given permutation (in this case each permutation class consists of only one permutation), it must be representable in the form of one of the arithmetic progressions ax+bax+b unambiguously corresponding to the element (permutation) of the Galois group in question. The number aa is one and the same for all permutations and consists of the prime numbers that come up in the driscriminant of the group, while the bb are assigned to the different elements (permutations) of the Galois group.

  3. 3.

    The other, now classic, case is that of complex multiplication of elliptic functions. Given a number field that is relatively abelian over an imaginary quadratic field, then each prime number belonging to a given permutation class can be represented by one or more quadratic forms, whose discriminants depend on the field (more precisely: equal to the discriminant of the imaginary quadratic field) and whose classes are assigned to the permutation classes.

  4. 4.

    This fact was suspected by Kronecker (“Jugendtraum”, or “youthhood dream”) and proven by R. Fueter [24][25]. The principles that it is based on follow from the general class field theory. Consider only those numbers of a field kk which satisfy certain congruences modulo an ideal 𝔣\mathfrak{f} (which one calls leader777Führer in the original German.-YS. Taking these numbers as principal ideals, and letting hh equal the number of classes in the newly defined sense, it follows that there exists a relatively abelian field KK of relative degree hh. This field, a so-called class field, has the property a prime ideal of kk decomposes fully in KK if and only if it lies in the principal class (Ph. Furtwängler, [26]; T. Takagi, [76]). Conversely we can regard any relatively abelian field over kk as a class field with a suitably chosen leader (Fueter, [24]; Takagi, [76]; Hasse, [32]).

  5. 5.

    We can ask ourselves the general question concerning the analytic form of prime numbers belonging to classes generating by powers of a permutation SS. Let a normal algebraic number field KK be given, and denote its [Galois] group by 𝔊\mathfrak{G}. Furthermore let 𝒮\mathcal{S} be a permutation in 𝔊\mathfrak{G}. For a prime number pp to belong to the classes generated by powers of 𝒮\mathcal{S}, it is necessary and sufficient for the subfield K𝒮K_{\mathcal{S}} of KK belonging to 𝒮\mathfrak{Z}_{\mathcal{S}} to contain a prime ideal divisor 𝔭\mathfrak{p} of pp of the first degree, where 𝒮\mathfrak{Z}_{\mathcal{S}} denotes the cyclic subgroup of 𝔊\mathfrak{G} generating by the powers of 𝒮\mathcal{S}.
    Let 𝔞1,𝔞2,,𝔞k\mathfrak{a}_{1},\mathfrak{a}_{2},...,\mathfrak{a}_{k} be a system of representatives of all distinct ideal classes of K𝒮K_{\mathcal{S}}, and let (μ1(i),μ2(i),,μn(i))(\mu_{1}^{(i)},\mu_{2}^{(i)},...,\mu_{n}^{(i)}) be respective bases of the ideals 𝔞i(i=1,2,,h)\mathfrak{a}_{i}(i=1,2,...,h). Then we have that N(μ1(i)x1+μ2(i)zx2++μn(i)xn)N(\mu_{1}^{(i)}x_{1}+\mu_{2}^{(i)z}x_{2}+...+\mu_{n}^{(i)}x_{n}) is the form (admitting a decomposition) of nn-th degree in the variables x1,x2,,xnx_{1},x_{2},...,x_{n}, whose coefficients have the number N(𝔞i)N(\mathfrak{a}_{i}) as their greatest common divisor. The quotient

    N(μ1(i)x1+μ2(i)x2++μn(i)xn)N(𝔞i)=fi(x1,x2,,xn)(i=1,2,,h)\frac{N(\mu_{1}^{(i)}x_{1}+\mu_{2}^{(i)}x_{2}+...+\mu_{n}^{(i)}x_{n})}{N(\mathfrak{a}_{i})}=f_{i}(x_{1},x_{2},...,x_{n})\quad(i=1,2,...,h) (3.1)

    is thus a primitive form of nn-th degree. If we allow the xix_{i} to take on any integer values, then the norm fi(x1,x2,,xn)f_{i}(x_{1},x_{2},...,x_{n}) takes on the values of the norms of all ideals, whose classes are opposite to the class of 𝔞i\mathfrak{a}_{i}. Since if bb lies in the opposite class to that of 𝔞i\mathfrak{a}_{i}, it follows that b𝔞ib\mathfrak{a}_{i} is a principal ideal, which may be associated with a number μ1(i)x1+μ2(i)x2++μn(i)xn\mu_{1}^{(i)}x_{1}+\mu_{2}^{(i)}x_{2}+...+\mu_{n}^{(i)}x_{n} from the ideal 𝔞i\mathfrak{a}_{i}. Thus, it holds that

    N(b)N(𝔞i)=N(μ1(i)x1+μ2(i)x2++μn(i)xn)=N(𝔞i)f(x1,x2,,xn).N(b)N(\mathfrak{a}_{i})=N(\mu_{1}^{(i)}x_{1}+\mu_{2}^{(i)}x_{2}+...+\mu_{n}^{(i)}x_{n})=N(\mathfrak{a}_{i})f(x_{1},x_{2},...,x_{n}).

    Given 𝔭\mathfrak{p} a prime ideal of KsK_{s} of first degree, it holds thus that N(𝔭)=pN(\mathfrak{p})=p, one wishes to find the representative 𝔞i\mathfrak{a}_{i}, whose class is opposite to the class of 𝔭\mathfrak{p}. Thus 𝔭\mathfrak{p} can be represented in the form fi(x1,x2,,xn)f_{i}(x_{1},x_{2},...,x_{n}). Conversely, if 𝔭\mathfrak{p} can be represented in the form fi(x1,x2,,xn)f_{i}(x_{1},x_{2},...,x_{n}), then N(𝔞i)pN(\mathfrak{a}_{i})p can be represented in the form N(μ1(i)x1+μ2(i)x2++μn(i)xn)N(\mu_{1}^{(i)}x_{1}+\mu_{2}^{(i)}x_{2}+...+\mu_{n}^{(i)}x_{n}). The number μ1(i)x1+μ2(i)x2++μn(i)xn\mu_{1}^{(i)}x_{1}+\mu_{2}^{(i)}x_{2}+...+\mu_{n}^{(i)}x_{n} is divisible by 𝔞i\mathfrak{a}_{i}, and the norm of the quotient ideal μ1(i)x1+μ2(i)x2++μn(i)xn𝔞i\frac{\mu_{1}^{(i)}x_{1}+\mu_{2}^{(i)}x_{2}+...+\mu_{n}^{(i)}x_{n}}{\mathfrak{a}_{i}} is equal to pp. It follows from this that there exists an ideal with norm pp. This ideal must be a prime ideal of degree 1.

  6. 6.

    To set up the conditions for a prime number pp to be a member of the division of 𝒮\mathcal{S}, we must exclude its membership to the powers 𝒮k\mathcal{S}^{k} of 𝒮\mathcal{S}, whose exponents kk are not relatively prime to the order ff of 𝒮\mathcal{S}. For this to occur pp in K𝒮K_{\mathcal{S}} must contain at least one prime ideal of first degree, while this does not happen for any K𝒮kK_{\mathcal{S}^{k}}, (k,f)1(k,f)\neq 1. Given

    gi(x1,x2,,xn),hi(x1,x2,,xn),g_{i}(x_{1},x_{2},...,x_{n}),\quad h_{i}(x_{1},x_{2},...,x_{n}),... (3.2)

    the corresponding forms for the fields K𝒮kK_{\mathcal{S}^{k}}, constructed in the same way as fi(x1,x2,,xn)f_{i}(x_{1},x_{2},...,x_{n}), we have that pp belongs to the division of 𝒮\mathcal{S} if and only if it admits a representation in terms of one of the forms (3.1), but none in terms of the forms (3.2).

  7. 7.

    How can one characterize the membership of a prime number pp to the class of 𝒮\mathcal{S}? I can do this only if I know a number aa such that pf1 (mod a)p^{f}\equiv 1\text{ (mod $a$)}, but that this congruence fails for any power of pp whose exponent is less than ff. Using this to construct the subfield K(η)K(\eta) of the aa-th roots of unity, it follows that pp remains irreducible in K(η)K(\eta). If pb (mod a)p\equiv b\text{ (mod $a$)}, then ηpηb (mod p)\eta^{p}\equiv\eta^{b}\text{ (mod $p$)} holds. Now we form the element

    ξ=ηω+ηbω𝒮++ηbf1ωSf1,\xi=\eta\omega+\eta^{b}\omega^{\mathcal{S}}+...+\eta^{b^{f-1}}\omega^{S^{f-1}},

    where ω\omega denotes an element of KK, and Φ(ξ)=0\Phi(\xi)=0 is an equation satisfied by ξ\xi. If one takes as established that pp belongs to the division of 𝒮\mathcal{S}, then pp belongs to the class of 𝒮\mathcal{S} if and only if the congruence Φ(ξ)0 (mod p)\Phi(\xi)\equiv 0\text{ (mod $p$)} has rational roots. That is, if pp has at least one prime ideal divisor of first degree in K(ξ)K(\xi). One can hence set up a system of forms such that pp can be represented by it if and only if pp belongs to the class of 𝒮\mathcal{S}. One can certainly find the corresponding number aa for each pp; there are however different forms corresponding to different pp. I can therefore not set up a finite number of forms that are valid for all prime numbers.

  8. 8.

    The classically regarded criteria in No. 2 and 3 do not follow from this criterion. To set up a more general criterion we regard the case where 𝔊\mathfrak{G} possesses an abelian normal subgroup \mathfrak{H}. Then one can understand KK as a relatively abelian field with respect to the field kk corresponding to \mathfrak{H}. KK is thus a class field of kk. By the general reciprocity law of E. Artin [2] there is a one-to-one correspondence between the permutations in \mathfrak{H} and the ideal classes (more specifically: the residue classes of a certain ideal class subgroup) of kk, which has the character of an isomorphism. The forms (3.1) corresponding to kk decompose thusly in the system of forms 𝔅i\mathfrak{B}_{i}, of which each represents one of the aforementioned residue classes. The number of these systems of forms is equal to the order of \mathfrak{H}. The Artin reciprocity law says that a prime number pp can be represented by one of the forms in the system 𝔅i\mathfrak{B}_{i} if and only if it belongs to the class of SiS_{i}, where SiS_{i} is one of the permutations in \mathfrak{H} corresponding to the system 𝔅i\mathfrak{B}_{i}. This system of forms has the advantage that the degree of its forms in generally smaller. For instance, if KK is absolutely abelian, then kk is the rational field, so that the norms coincide with the numbers themselves. The partitioning of numbers of the rational field in the “narrower” sense is nothing else but their distribution among the congruence classes by a certain relation, which one calls leader. If kk is quadratic, we arrive at the quadratic forms, in complete concurrence with the general theory.

  9. 9.

    We still note that the forms corresponding to the field kk allow for the so-called form composition. For instance, given

    N(𝔞)=f1(x1,x2,,xn),N(𝔟)=𝔣2(𝔶1,𝔶2,,𝔶𝔫)N(\mathfrak{a})=f_{1}(x_{1},x_{2},...,x_{n}),\quad N(\mathfrak{b)=f_{2}(y_{1},y_{2},...,y_{n})}

    then it follows that

    N(𝔞𝔟)=f1(x1,x2,,xn)cf˙2(y1,y2,,yn).N(\mathfrak{a}\mathfrak{b})=f_{1}(x_{1},x_{2},...,x_{n})c\dot{f}_{2}(y_{1},y_{2},...,y_{n}).

    On the other hand, if 𝔞𝔟\mathfrak{a}\mathfrak{b} lies in the opposing ideal class to 𝔞3\mathfrak{a}_{3}, then N(𝔞𝔟)=f3(z1,z2,,zn)N(\mathfrak{a}\mathfrak{b})=f_{3}(z_{1},z_{2},...,z_{n}), where z1,z2,,znz_{1},z_{2},...,z_{n} are certain integer-valued bilinear expressions in x1,x2,,xnx_{1},x_{2},...,x_{n} and y1,y2,,yny_{1},y_{2},...,y_{n}. One can obtain these by considering the bilinear expression i,jμi(1)μj(2)xixj\sum\limits_{i,j}\mu_{i}^{(1)}\mu_{j}^{(2)}x_{i}x_{j}, where (μ1(1),μ2(1),,μn(1))(\mu_{1}^{(1)},\mu_{2}^{(1)},...,\mu_{n}^{(1)}), (μ1(2),μ2(2),,μn(2))(\mu_{1}^{(2)},\mu_{2}^{(2)},...,\mu_{n}^{(2)}) denote the bases of the ideals 𝔞1,𝔟2\mathfrak{a}_{1},\mathfrak{b_{2}} respectively. By expressing the μi(1)μj(2)\mu_{i}^{(1)}\mu_{j}^{(2)} using a basis (μ1(3),μ2(3),,μn(3))(\mu_{1}^{(3)},\mu_{2}^{(3)},...,\mu_{n}^{(3)}) of the ideal 𝔞1𝔟2\mathfrak{a}_{1}\mathfrak{b}_{2}: μi(1)μj(2)=scijsμs(3)\mu_{i}^{(1)}\mu_{j}^{(2)}=\sum\limits_{s}c^{s}_{ij}\mu_{s}^{(3)}, i.e. 𝔞1𝔞2𝔞𝔟=i,j,scijsxixjμs(3)\mathfrak{a}_{1}\mathfrak{a}_{2}\mathfrak{a}\mathfrak{b}=\sum\limits_{i,j,s}c_{ij}^{s}x_{i}x_{j}\mu_{s}^{(3)}, one then sets the zsz_{s} equal to the coefficients of μs(3)\mu_{s}^{(3)}: zs=i,jcijsxixjz_{s}=\sum\limits_{i,j}c_{ij}^{s}x_{i}x_{j}. It is easy to understand that this composition of forms corresponds to the multiplication of their corresponding forms.

  10. 10.

    To obtain a simplest analytic expression of prime numbers belonging to different permutation classes of a field we must find maximal abelian normal subgroups of its [Galois] group 𝔊\mathfrak{G}. We note that a permutation 𝒮\mathcal{S} in 𝔊\mathfrak{G} can be contained in a abelian normal subgroup of 𝔊\mathfrak{G} if and only if its class is abelian, i.e. all permutations in its class commute with each other. If 1,2,,k\mathfrak{C}_{1},\mathfrak{C}_{2},...,\mathfrak{C}_{k} are all the abelian classes in 𝔊\mathfrak{G}, we have that each abelian normal subgroup consists of those permutations in the classes which commute with one another. For instance, given 1\mathfrak{C}_{1} and 2\mathfrak{C}_{2} commuting, then the join, that is the smallest group containing 1\mathfrak{C}_{1} and 2\mathfrak{C}_{2}, is an abelian normal subgroup of 𝔊\mathfrak{G}. The uniqueness of a maximal abelian normal subgroup cannot be guaranteed since the commutativity of classes is not a transitive property.
    The following example shows that cases exist where 𝔊\mathfrak{G} contains multiple different maximal abelian subgroups. Define 𝔊\mathfrak{G} using 3 generating elements s1,s2,s3s_{1},s_{2},s_{3}, where are subject to the following relations:

    s1p=s2p=s3p=1,s1s2=s2s1,s1s3=s3s1,s2s3=s3s2s1s_{1}^{p}=s_{2}^{p}=s_{3}^{p}=1,s_{1}s_{2}=s_{2}s_{1},s_{1}s_{3}=s_{3}s_{1},s_{2}s_{3}=s_{3}s_{2}s_{1}

    (pp is a prime number). Both subgroups (s1,s2)(s_{1},s_{2}) and (s1,s3)(s_{1},s_{3}) are abelian normal subgroups of 𝔊\mathfrak{G}. Both are maximal since they are only properly contained in 𝔊\mathfrak{G}, which is not abelian. On the other hand, they are distinct from one another.

  11. 11.

    As an example we will consider the general cubic number field KK. Its alternating group possesses a quadratic subfield kk, and by using Fueter-Takagi theory one can regard KK as a ring class field of kk. Corresponding to the ring classes of kk in consideration we have a system of binary quadratic forms, which decompose into the 3 subsystems 𝔅1,𝔅2,𝔅3\mathfrak{B}_{1},\mathfrak{B}_{2},\mathfrak{B}_{3}, to which one can associate each of the three permutations in \mathfrak{H}. Given DD the discriminant of the system of forms, we have that (Dp)=±1\left(\frac{D}{p}\right)=\pm 1 is the necessary and sufficient condition for pp to admit a representation through one of these forms. The principal system is the system from 𝔅1,𝔅2,𝔅3\mathfrak{B}_{1},\mathfrak{B}_{2},\mathfrak{B}_{3}, say 𝔅1\mathfrak{B}_{1}, which satisfies the property 𝔅1𝔅1=𝔅1\mathfrak{B}_{1}\mathfrak{B}_{1}=\mathfrak{B}_{1}. Then all prime numbers relatively prime to the discriminant of KK belong to the following three types:

    1. i)

      (Dp)=1\left(\frac{D}{p}\right)=-1, pp does not belong to \mathfrak{H}, hence belonging to one of the transpositions.

    2. ii)

      (Dp)=+1\left(\frac{D}{p}\right)=+1, pp can be represented through one of the forms 𝔅2,𝔅3\mathfrak{B}_{2},\mathfrak{B}_{3}. pp belongs to one of the 3-cycles.

    3. iii)

      (Dp)=+1\left(\frac{D}{p}\right)=+1, pp can be represented through one of the forms 𝔅1\mathfrak{B}_{1}. pp belongs to one of the identity permutation.

    The cubic field was investigated in this respect by Dedekind [17], Voronoi [85] and Takagi. More recently Hasse [33] investigated the cubic field from a class field theoretic perspective, by also considering the critical prime ideals. This work was kindly brought to my attention by B. Delaunay.

  12. 12.

    I want to mention a very elegant procedure due to A. Speiser [73] which serves the purpose of determining the order 𝔣\mathfrak{f} of a permutation whose class contains a prime number pp. I allow myself to modify the proof somewhat. Given

    f(x)=xn+a1xn1+a2xn2++an1x+an=0f(x)=x^{n}+a_{1}x^{n-1}+a_{2}x^{n-2}+...+a_{n-1}x+a_{n}=0 (3.3)

    the equation to be examined, we consider the difference equation

    y(m+n)+a1y(m+n1)++an1y(m+1)+any(m)=0.y(m+n)+a_{1}y(m+n-1)+...+a_{n-1}y(m+1)+a_{n}y(m)=0. (3.4)

    We know its general solution to be given by

    y(m)=C1α1m+C2α2m++Cnαnm,y(m)=C_{1}\alpha_{1}^{m}+C_{2}\alpha_{2}^{m}+...+C_{n}\alpha_{n}^{m}, (3.5)

    where α1,α2,,αn\alpha_{1},\alpha_{2},...,\alpha_{n} are the roots of equation (3.3) and C1,C2,,CnC_{1},C_{2},...,C_{n} are arbitrary constants. Setting y(1)=y(2)=y(n1)=0,y(n)=1y(1)=y(2)=y(n-1)=0,y(n)=1, we have Ci=1f(αi)C_{i}=\frac{1}{f^{\prime}(\alpha_{i})}. Now take GF[p𝔣]GF[p^{\mathfrak{f}}] as a base field. If uu is the smallest (integer-valued) period of the function y(m)y(m) modulo pp, it follows that αiu1 (mod p) (i=1,2,,n)\alpha_{i}^{u}\equiv 1\text{ (mod $p$) ($i=1,2,...,n$)}, and vice-versa. This is true since if y(u)y(u+1).y(u+n1)0 (mod p)y(u)\equiv y(u+1)\equiv....\equiv y(u+n-1)\equiv 0\text{ (mod $p$)}, y(u+n)1 (mod p)y(u+n)\equiv 1\text{ (mod $p$)}, it follows that Ci1αiuf(αi) (mod p)C_{i}\equiv\frac{1}{\alpha_{i}^{u}f^{\prime}(\alpha_{i})}\text{ (mod $p$)}, i.e. aiu1 (mod p)a_{i}^{u}\equiv 1\text{ (mod $p$)}. However, since (αiαip)(\alpha_{i}\to\alpha_{i}^{p}) is a generating permutation for the [Galois] group of the congruence f(x)0 (mod p)f(x)\equiv 0\text{ (mod $p$)} and its order is hence equal to the smallest number 𝔣\mathfrak{f}, for which aip𝔣αi (mod p)a_{i}^{p^{\mathfrak{f}}}\equiv\alpha_{i}\text{ (mod $p$)} holds, it follows that 𝔣\mathfrak{f} is the smallest exponent for which p𝔣1 (mod u)p^{\mathfrak{f}}\equiv 1\text{ (mod $u$)} holds.

  13. 13.

    Hasse has recently layed new groundwork for the question concerning the arthimetic structure of number fields, by connecting the theory of number fields with the so-called “algebras” (i.e. hypercomplex systems) [34][9]. Each field has a corresponding “cyclic” hypercomplex system, introduced by E. Noether under the name crossed product. However, we conversely have that multiple fields with different Galois groups, in particular cyclic fields, correspond to the same cyclic algebra, meaning this is the deepest connection in which we can bring arithmetic properties of fields those of cylic fields.

§4 The resolvent problem

  1. 1.

    There is a question in the general algebraic field theory which includes the resolvent problem as a special case:
    Let KK be a given field of a rational functions in the variables x1,x2,,xnx_{1},x_{2},...,x_{n}. One must determine the true transcendence degree of KK in relation to a certain one of its subfields kk. That is, one finds the smallest number mm such that KK can be expressed as a direct product of a field of algebraic functions in mm variables, which split in kk, and a certain subfield of kk (see below §5).
    To clarify the connection between this question and the resolvent problem, we will consider the the field KK of all rational functions in the variables x1,x2,,xnx_{1},x_{2},...,x_{n}, while kk consists of the elementary symmetric functions a1,a2,,ana_{1},a_{2},...,a_{n} of the variables x1,x2,,xnx_{1},x_{2},...,x_{n} and their rational functions. One must find an equation of nn-th degree (resolvent) whose coefficients are rational functions of a1,a2,,ana_{1},a_{2},...,a_{n} and as few as possible (mm) are functionally independent, and whose roots generate the whole field KK. In other words, we are dealing with the Tschirnhaus transformation of the equation

    xn+a1xn1++an1x+an=0x^{n}+a_{1}x^{n-1}+...+a_{n-1}x+a_{n}=0 (4.1)

    with the unrestricted variable coefficients a1,a2,,ana_{1},a_{2},...,a_{n} into an equation, whose coefficients possess a number of degrees of freedom that are as small as possible.
    It is of use to expand this task by introducing irrational functions of a1,a2,,ana_{1},a_{2},...,a_{n} into the coefficient field kk, however are also not of a higher transcendence degree than mm. An example of this is D\sqrt{D}, where DD denotes the discriminant of equation (4.1).
    This problem can be summarized as a natural extension of the original task of Galois theory, the solution by radicals. This is because the representation of roots through radical expressions has the advantage that it permits the determination of roots through a sequence of operations that each only is concerned with one variable. To this end one can create a table that assigns to each radicand its radical, such that these tables enable the computation of roots of all solvable equations of a given degree.

  2. 2.

    The aforementioned property is in no way characteristic of solvable equations. One can rather set up the detection of roots through operations of a totally different kind, for which this property applies to all of them. First of all one can mention the general equation of fifth degree. It was known for a long time (Bring, [12]), that one can convert it into the so called Bring-Jerrard form

    y5+py+q=0y^{5}+py+q=0 (4.2)

    by applying a Tschirnhaus transformation, whose coefficients are roots of the equations of fourth degree, that is permit representations via radical expressions (see J. J. Sylvester, [75]). On the other the hand the connection between equations of fifth degree and the division problem of periods of elliptic functions (thus the arguments of modular functions) into 5 is well known. This allows the general equation of fifth degree to be solved in a transcendental way (see [29],[86]).

  3. 3.

    This problem was solved by F. Klein in a way that allows a perspective into the general resolvent problem [41]. He namely converted the general equation of fifth degree into a slightly different normal form

    y5+15y410γy2+3γ2=0y^{5}+15y^{4}-10\gamma\cdot y^{2}+3\gamma^{2}=0 (4.3)

    via the use of only quadratic irrationalities, one of which is D\sqrt{D} and the other is 5\sqrt{5}.
    The second, much more important contribution from Klein towards the resolvent problem consists of developing the deeper reason for why the resolvent problem is solvable for equations of fifth degree. Specifically he linked this problem to the so-called form problem, which consists of the following. If we regard the largest finite group 𝔊\mathfrak{G} of binary linear transformations, the icosahedral group, one can associate to it an equation of degree 60

    (𝔇30+522𝔇2510005𝔇2010005𝔇10522𝔇5+1)2=z𝔇5(𝔇10+11𝔇51)5(\mathfrak{D}^{30}+522\mathfrak{D}^{25}-10005\mathfrak{D}^{20}-10005\mathfrak{D}^{10}-522\mathfrak{D}^{5}+1)^{2}=z\cdot\mathfrak{D}^{5}(\mathfrak{D}^{10}+11\mathfrak{D}^{5}-1)^{5} (4.4)

    whose coefficients depend on a form zz of the variables x1,x2x_{1},x_{2}, which are invariant under the transformations of 𝔊\mathfrak{G}, while the roots are mapped to each other via these transformations. The Galois group of this equation is isomorphic as the icosahedral group to the alternating group of fifth degree. From this one can conclude that each equation of fifth degree can be converted to the form (4.4) (or also (4.3)) by using a rational transformations, whose coefficients may contain D\sqrt{D}, where DD denotes the discriminant of this equation.
    The basic idea of reducing fifth degree equations to a parametric resolvent comes from the fact that the composition series of the symmetric group of fifth degree consists of two factors, where one is a group of degree 2, while the other is isomorphic to the icosahedral group, which can be represented as a group of linear fractional transformations.

  4. 4.

    This idea was applied by Klein to other equations, in particular the simple group of order 168, which can be represented using ternary linear homogeneous transformations. This group corresponds to a special class of equations of 7-th degree that have this group as their Galois group. Since the group of ternary linear homogeneous transformations is isomorphic to the group of linear fractional transformations of two variables, we can similarly conclude that the equations we’re concerned with possess a two parameter resolvent.
    Slightly more complicated was the matter of the alternating equations of 6-th degree. The alternating group of 6-th degree does not possess a representation by ternary linear homogeneous transformations. It was for this reason that Klein suspected that the general equation of 6-th degree does not possess a 2 parameter resolvent, and sought out 3 parameter resolvents. A. Wiman [89] noticed, that in spite of that this group admits a representation in terms of linear fractional transformations in two variables. This is because one can construct this group as a factor group of a certain group of order 1080, which can be represented as a linear homogeneous group of three variables. Its corresponding normal subgroup \mathfrak{H} of order 3 lies in the center of the group and thus appears as a group whose transformations only affect the multiplication of the variables with the 3rd roots of unity. Now looking at how this affects the relations between the variables, we have that they form a group of linear fractional transformations. Acting on the original variables with the transformations in \mathfrak{H}, we see that the relations remain unchanged. The group of linear fractional transformations we have just constructed it thus isomorphic to the factor group, that is the altnerating group of 6-th degree.

  5. 5.

    The question regarding the representation of finite groups by linear fractional transformations was investigated in general by I. Schur [69][70]. It was proven that this task could always be completed using a finite number of operations. That is, in order to find all such representations of a given finite group 𝔊\mathfrak{G} one must find a covering group 𝔎\mathfrak{K} corresponding to 𝔊\mathfrak{G} possessing the following properties:

    1. I.

      𝔊\mathfrak{G} is isomorphic to a factor group 𝔎/𝔐\mathfrak{K}/\mathfrak{M}.

    2. II.

      𝔐\mathfrak{M} is contained in the center of 𝔎\mathfrak{K}.

    3. III.

      The commutator subgroup of 𝔊\mathfrak{G} is the factor group 𝔇/𝔐\mathfrak{D}/\mathfrak{M}, 𝔇\mathfrak{D} denoting the commutator subgroup of 𝔎\mathfrak{K}.

    Each group 𝔊\mathfrak{G} corresponds to only a finite number of distinct covering groups 𝔎\mathfrak{K}. If one finds all representations of 𝔎\mathfrak{K} by linear homogeneous transformations, each such representation induces a representation of 𝔊\mathfrak{G} by linear fractional transformations. This is the general method for the formation of all representations of 𝔊\mathfrak{G} of this kind.

  6. 6.

    A. Wiman [90] studied the question of representing the symmetric and alternating groups of higher degrees. It was shown that for n8n\geq 8 the symmetric groups 𝒮n\mathcal{S}_{n} can be represented as linear homogeneous groups of no less than n1n-1 variables, with the same statement holding true for the alternating groups.

  7. 7.

    D. Hilbert [36] posed a problem (“13. problem”) that has many points of contact with the Klein problem discussed above. Let the roots of equation (4.1) be regarded as functions of nn variables. One asks if these functions can be written as superpositions of functions of a smaller number kk of variables and rational operations. Later [37] he found the following values for kk for n9n\leq 9:

    n 5 6 7 8 9 k 1 2 3 4 4 .\begin{tabularx}{433.62pt}[]{ X|X|X|X|X|X| }$n$&5&6&7&8&9\\ \hline\cr$k\leq$&1&2&3&4&4\\ \end{tabularx}.

    Wiman [91] generalized this result by showing that for all n9n\geq 9 we have the inequality kn5k\leq n-5, i.e. any general equation of degree n9n\geq 9 can be reduced by at least 5 variables via application of a Tschirnhaus transformation. (See also R. Garver, [28]).

  8. 8.

    I [84] have set myself the goal to examine the connection between the reducibility of an equation and the ability to represent their Galois group as a transformation group of as few variables as possible somewhat closer. To this I will introduce the term Einkleidungsgruppe888This translates as outfitting group or investiture group.-YS (short E.G.):
    Given 𝔊\mathfrak{G} a finite group, we call a continuous group Γ\Gamma an E.G. of 𝔊\mathfrak{G} if and only if it satisfies the following conditions:

    1. i)

      Γ\Gamma contains a subgroup isomorphic to 𝔊\mathfrak{G}.

    2. ii)

      There is no proper subgroup of Γ\Gamma possessing property 1).

    3. iii)

      There is no proper factor group of Γ\Gamma possessing property 1).

    I then proved the following
    Theorem. An algebraic equation with unrestricted variable coefficients possesses a kk parameter resolvent if and only if its Galois group has an E.G. that can be represented in kk-dimensional space.
    To prove the first part of this theorem we will assume that the group 𝔊\mathfrak{G} is simple, which is sufficient for our purposes. In this case it follows that each E.G. is also a simple group. Since if a continuous group Γ\Gamma containing 𝔊\mathfrak{G} as a subgroup contains a proper normal subgroup Γ1\Gamma_{1}, it follows that Γ1\Gamma_{1} either contains all of 𝔊\mathfrak{G} or not elements of 𝔊\mathfrak{G} besides the identity. In the first case this contradicts condition 2). In the second case it follows that Γ/Γ1\Gamma/\Gamma_{1} has a subgroup isomorphic to 𝔊\mathfrak{G}, contradicting condition 3).
    One can moreover show the following: If a continuous group Γ\Gamma having 𝔊\mathfrak{G} as a subgroup can be represented in kk-dimensional space (abbreviated: Γ\Gamma is a kk-group), then the subgroup of Γ\Gamma which is an E.G. of 𝔊\mathfrak{G} is also a kk-group. It is evident that a subgroup of a kk-group is a kk-group. To show that a simple factor group of a kk-group is once again a kk-group, we recall a theorem initially proven in generality by E.E. Levi [44]: If a continuous group Γ\Gamma has a simple factor group Γ1\Gamma_{1}, it also has a subgroup isomorphic to Γ1\Gamma_{1}.

  9. 9.

    If 𝔊\mathfrak{G}, presented as transformations of the roots as variables, permits an E.G. that is not just isomorphic, but similar to a kk-group, one immediately obtains a solution to the problem. One can namely set up kk functions z1,z2,,zkz_{1},z_{2},...,z_{k} of the variables x1,x2,,xnx_{1},x_{2},...,x_{n} which describe a group isomorphic to Γ\Gamma, by applying the transformations in Γ\Gamma to the xix_{i}. In doing so, due to the investigations of Lie-Engel ([45], p. 522), one can find the ziz_{i} in a rational way, since they form systems of imprimitivity of Γ\Gamma. If the group Γ\Gamma is transitive, one can take the ziz_{i} to be rational functions of x1,x2,,xnx_{1},x_{2},...,x_{n}. Otherwise they depend on an irrationality θ\theta which itself depends on the group Γ\Gamma. If for instance we take ziz_{i} as a rational function of x1,x2,,xnx_{1},x_{2},...,x_{n}, then they generate all elements of the field coinciding with k[x1,x2,,xn]k[x_{1},x_{2},...,x_{n}] conjugate to ziz_{i}. On the other hand these elements depend solely on z1,z2,,znz_{1},z_{2},...,z_{n}, since they are generated by application of the transformations in the group 𝔊\mathfrak{G}, while the transformations in 𝔊\mathfrak{G} appear in the group Γ\Gamma as transformations taking the ziz_{i} into functions of the ziz_{i}. It follows from this that ziz_{i} satisfies an equation whose coefficients depend on only kk parameters, while the xix_{i} can be expressed rationally by the ziz_{i}.

  10. 10.

    If Γ\Gamma is an E.G. of the group 𝔊\mathfrak{G} and isomorphic, but not similar to a kk-group, one can apply Cartan’s principle, which consists of the following [14]:
    If two continuous groups Γ\Gamma and Γ1\Gamma_{1} are isomorphic, one can extend the group Γ\Gamma in such a way that one obtains the group Γ1\Gamma_{1} by applying the transformations of Γ\Gamma to the variables corresponding to the functions of the extended group.
    By “extension of a group” one understands the following. If x1,x2,,xnx_{1},x_{2},...,x_{n} are the variables corresponding to the group Γ\Gamma, one introduces new sequences of variables

    x1,x2,,xn,x1(1),x2(1),,xn(1),x1(m1),x2(m1),,xn(m1),\begin{matrix}x_{1},&x_{2},&...,&x_{n},\\ x_{1}^{(1)},&x_{2}^{(1)},&...,&x_{n}^{(1)},\\ ...&...&...&...\\ x_{1}^{(m-1)},&x_{2}^{(m-1)},&...,&x_{n}^{(m-1)},\end{matrix} (4.5)

    so that one obtains the the extended group Γ\Gamma by simultaneously applying transformations in the original group Γ\Gamma to each sequence:

    x1(λ),x2(λ),,xn(λ)(λ=0,1,2,,m1).x_{1}^{(\lambda)},x_{2}^{(\lambda)},...,x_{n}^{(\lambda)}\quad(\lambda=0,1,2,...,m-1).

    To construct a kk parameter resolvent in this case, instead of the variables x1(λ),x2(λ),,xn(λ)(λ=0,1,2,,m1)x_{1}^{(\lambda)},x_{2}^{(\lambda)},...,x_{n}^{(\lambda)}(\lambda=0,1,2,...,m-1) we introduce the new variables a1(λ),a2(λ),,an(λ)a_{1}^{(\lambda)},a_{2}^{(\lambda)},...,a_{n}^{(\lambda)} using the formulae

    x1(λ)=a0(λ)+a1(λ)x1++an1(λ)x1n1,\displaystyle x_{1}^{(\lambda)}=a_{0}^{(\lambda)}+a_{1}^{(\lambda)}x_{1}+...+a_{n-1}^{(\lambda)}x_{1}^{n-1}, (4.6)
    x2(λ)=a0(λ)+a1(λ)x2++an1(λ)x2n1,\displaystyle x_{2}^{(\lambda)}=a_{0}^{(\lambda)}+a_{1}^{(\lambda)}x_{2}+...+a_{n-1}^{(\lambda)}x_{2}^{n-1},
    (λ=1,2,,m1)\displaystyle...\quad\quad\quad\quad\quad\quad\quad\quad\quad\quad\quad\quad\quad\quad\quad\quad\quad(\lambda=1,2,...,m-1)
    xn(λ)=a0(λ)+a1(λ)xn++an1(λ)xnn1.\displaystyle x_{n}^{(\lambda)}=a_{0}^{(\lambda)}+a_{1}^{(\lambda)}x_{n}+...+a_{n-1}^{(\lambda)}x_{n}^{n-1}.

    If we apply the transformations UU in Γ\Gamma to the variables in (4.5), the ai(λ)a_{i}^{(\lambda)} undergo certain transformations that become the identity when we replace the transformations UU with transformations from 𝔊\mathfrak{G}. Plugging these expressions into one of the functions

    zi(x1,x2,,xn;x1(1),x2(1),,xn(1);;x1(m1),x2(m1),xn(m1)),z_{i}(x_{1},x_{2},...,x_{n};x_{1}^{(1)},x_{2}^{(1)},...,x_{n}^{(1)};...;x_{1}^{(m-1)},x_{2}^{(m-1)},...x_{n}^{(m-1)}),

    say z1z_{1}, which is subject to a transformation from a kk-group whenever one applies a transformation from Γ\Gamma to the xi(λ)x_{i}^{(\lambda)}, one finds that the functions z1,z1s1,,z1sN1z_{1},z_{1}^{s_{1}},...,z_{1}^{s_{N-1}} only depend on kk parameters, where 𝔊=1+s1++sN1\mathfrak{G}=1+s_{1}+...+s_{N-1}. Since the ai(λ)a_{i}^{(\lambda)} remain invariant under these transformations we can replace them with arbitrary rational numbers, provided one requires that the differences z1siz1z_{1}^{s_{i}}-z_{1} (i=1,2,,N1)(i=1,2,...,N-1) are all non-zero. From this we obtain a Galois resolvent with kk parameters. However, in order to obtain kk-parameter equation from this that comes from performing a Tschirnhaus transformation on equation (4.1)(\ref{4.1}), we must construct a function from the z1siz_{1}^{s_{i}} that belongs to the group that x1x_{1} belongs to.

  11. 11.

    It is not out of the question that the transition of the xix_{i} to the ZiZ_{i} is not rational, but instead contains an irrationality θ\theta, which itself depends on the invariants of the extended group Γ\Gamma. We will refer to the irreducible equation R(θ)=0R(\theta)=0 satisfied by θ\theta as the near resolvent. This raises the important question of whether or not a near resolvent contains more essential parameters than the equation (4.1) itself. I cannot answer this question in general today. It is only known that for symmetric 𝔊\mathfrak{G} the near resolvent has 0 parameters, thus is numerical, and for alternating 𝔊\mathfrak{G} has at most 1 parameter.

  12. 12.

    Now we will prove the second part of the stated theorem. Let Z1,Z2,,ZnZ_{1},Z_{2},...,Z_{n} be the roots of a kk-paramter resolvent of equation (4.1), which is written in the fashion of a normal equation. The ZiZ_{i} are functions of x1,x2,..,xnx_{1},x_{2},..,x_{n} belonging to the unity group. Acting on the xix_{i} using the permutations in the group 𝔊\mathfrak{G}, we obtain induced permutations on the ZiZ_{i} which form a group isomorphic to 𝔊¯\overline{\mathfrak{G}}, which differs from 𝔊\mathfrak{G} only by a different designation of the variables.
    At first we will take Z1,Z2,,ZnZ_{1},Z_{2},...,Z_{n} as independent variables and will attach to 𝔊¯\overline{\mathfrak{G}} the continuous group Γ\Gamma in the following way: Consider a system A,B,,A,B,..., a system of permutations in 𝔊¯\overline{\mathfrak{G}} which generate the whole group 𝔊¯\overline{\mathfrak{G}} using composition. We consider each of these permutations, say AA, as a linear homogeneous transformation and depict them in a normal form:

    uiϵkiui(i=1,2,,n),u_{i}\to\epsilon^{k_{i}}u_{i}\quad\quad(i=1,2,...,n),

    where ϵ=e2πim\epsilon=e^{\tfrac{2\pi i}{m}} is a root of unity and uiu_{i} denotes a linear function in Z1,Z2,,ZnZ_{1},Z_{2},...,Z_{n}. We then take

    uiekitui(i=1,2,,n)u_{i}\to e^{k_{i}t}u_{i}\quad\quad(i=1,2,...,n)

    as the generating transformation for the group Γ1\Gamma_{1}, which then becomes AA after setting t=2πimt=\frac{2\pi i}{m}. Returning to the original variables Z1,Z2,,ZnZ_{1},Z_{2},...,Z_{n} and do this with all generating transformations A,B,A,B,..., we obtain a continuous group Γ\Gamma which is an E.G.E.G. for 𝔊¯\overline{\mathfrak{G}}. Γ\Gamma, being a linear group of the nn variables, only has a finite number of parameters.
    Next we regard the ZiZ_{i} as functions of the xix_{i} and view the xix_{i} as coordinates of a space \mathfrak{R}, whereby two points (x1,x2,,xn)(x_{1},x_{2},...,x_{n}) and (x1,x2,,xn)(x_{1}^{\prime},x_{2}^{\prime},...,x_{n}^{\prime}) are considered not distinct from one another if and only if

    Zi(x1,x2,,xn)=Zi(x1,x2,,xn)(i=1,2,..,n).Z_{i}(x_{1},x_{2},...,x_{n})=Z_{i}(x_{1}^{\prime},x_{2}^{\prime},...,x_{n}^{\prime})\quad\quad(i=1,2,..,n).

    Since amongst the Z1,Z2,,ZnZ_{1},Z_{2},...,Z_{n} there is only a set of kk which is functionally independent, it follows that the space \mathfrak{R} only has kk dimensions. The group Γ\Gamma induces a continuous group in \mathfrak{R}, that is locally999See previous footnote concerning isomorphisms “im kleinen”. -YS isomorphic to Γ\Gamma[67], and contains the group isomorphic to 𝔊\mathfrak{G} as a subgroup, since for instance Z1Z_{1} belongs to the identical group of 𝔊\mathfrak{G}. Thusly we have that 𝔊\mathfrak{G} admits a kk-group as an E.G., QED.

  13. 13.

    In the proof of this theorem it is important that every coordinate system of the parameters of the group Γ\Gamma determines the point of the space \mathfrak{R} in a well-defined manner. For that reason the Schreier definition [67] applies to our group, meaning all of Schreier theory is applicable. However, if this condition is not satisfied, we could for instance encounter a scenario in which a non-cyclic monodromy group of an algebraic function of a single variable admits a single-parameter continous group as an E.G. As an example, the continuous group defined by the equations

    x+y+z=C1,x2+y2+z2=C2,x3+y3+z3=C3x+y+z=C_{1},\quad x^{2}+y^{2}+z^{2}=C_{2},\quad x^{3}+y^{3}+z^{3}=C_{3}

    contains the symmetric permutation group of third degree, which is not even abelian.

  14. 14.

    Let a finite group 𝔊\mathfrak{G} without a center be given. How does one go about determining the E.G. belonging to it that is representable in as few dimensions as possible? To answer this question one should note that each of the sought after continuous groups is always isomorphic “im kleinen” to a linear homogeneous group Γ\Gamma. At the same time we have that Γ\Gamma must either contain 𝔊\mathfrak{G} itself as a subgroup, or it must have a finite subgroup which contains 𝔊\mathfrak{G} as the factor group with respect to its center. The follows from the theory of groups “isomorphic im kleinen” due to Schreier [67], according to which all groups “isomorphic im kleinen” are factor groups of a covering group with respect to discrete subgroups lying in the center of the covering group. It then follows from the work of I. Schur [69][70] that one must consider all “covering groups”. Their quantity is known to be finite.
    This question admits a fairly straightforward answer in the case where 𝔊\mathfrak{G} is a simple group. Since in this case we have that its E.G. is also simple. However, from the work of W. Killing [40] and E. Cartan [13], it follows that besides a finite number of easily specified exceptions there exist only three types of simple groups: 1) full unimodular linear groups ; 2) orthogonal groups; 3) symplectic groups. It is otherwise known (Cartan, [13]) that nn-dimensional groups of type 1) are (n1)(n-1)-groups and those of types 2) and 3) are (n2)(n-2)-groups. It follows that one only needs to examine linear homogeneous groups of at most n1n-1 dimensions for possible E.G.’s for 𝔊\mathfrak{G}, where nn is the degree of (4.1). On the other hand, Wiman ([91]; see also R. Garver, [28]) proved that the altenerating group of nn-th degree (n8n\geq 8) cannot be represented by linear homogeneous transformations of degree less than (n1)(n-1). This does not yet allow us to see the task of finding a resolvent in less than (n3)(n-3) parameters as impossible. This is because one must consider the covering groups themselves and not just representability of the alternating group. We have convinced ourselves using the n=6n=6 case that this sometimes allows a reduction in the number of parameters in the resolvent. However, I must once again particularly emphasize that the Sylvester-Hilbert-Wiman problem, which for n9n\geq 9 allows a reduction of at least 5 parameters, cannot be regarded as a special case of the Klein problem. In other words we cannot claim a priori that a reduction in parameters assisted by a chain of resolvents can only be accomplished using a single resolvent. The theorem valid in classical Galois theory regarding natural irrationalities cannot be directly extended to the resolvent problem. The accomplishment of the task via chains of resolvents requires an extensive study of the resolvent problem in the case where the coefficients of equation (4.1) are not free, but connected by some relations. (See §5, No. 8). In that case it can arise that the finite group to be embedded in an E.G. does not coincide with the monodromy group of equation (4.1). In No. 13 we saw an example of this phenomenon.

  15. 15.

    The Einkleidungsproblem for finite groups by continuous groups is of significant interest in itself. I cannot say at this point whether a finite group admits a finite or infinite number of non-isomorphic continuous groups as E.G.s. The representation theory of continuous groups is of use for the solution to this problem (Cartan, [13]; Schur, [71]; R. Brauer, [8]; H. Weyl, [88]). It is however very inconvenient that each continuous group admits infinitely many irreducible linear homogeneous representations.
    The converse of this problem was already posed a while ago. This is the problem of classifying all finite groups, that are contianed in a given continuous group. C. Jordan [39] proved the following fundamental theorem for this problem:
    Each continuous linear homogeneous group Γ\Gamma contains only those non-isomorphic finite subgroups 𝔊\mathfrak{G} whose factor groups by abelian normal subgroups belong only finitely many times to the group Γ\Gamma.

§5 Further questions in the general theory of fields

  1. 1.

    The questions in the theory of algebraic number fields that regard the algebraic numbers with respect to their rationality are usually solvable using Galois theoretic methods. However, if the fields in question contain certain transcendental (variable) elements, then the corresponding structural questions for these fields do not admit a straightforward group theoretic description. Even though I nonetheless include these questions in Galois theoretic body of ideas, I do it for the following reasons: It is first of all not natural to define Galois theory as the body of ideas whose problems can be solved using the Galois group, since the Galois group is a solution tool. That is to say that these same problems may be solved using significantly different means, meaning a solution tool is in no way suitable for delimiting an area of study. Secondly we cannot say a priori whether a problem in consideration is not solvable using an appropriately defined notion of the Galois group. It is far more appropriate to define Galois theory as the body of problems, whose problems concern themselves with the rational dependence of fields and individual field elements.

  2. 2.

    Identity of two algebraic fields. A field is by no means determined by its Galois group. On the contrary one can construct distinct fields with isomorphic [Galois] groups. The question concerning the identity of fields thus actually lies outside of the realm of Galois theory. If KK is a number field this question is essentially number-theoretic. Its answer would be best achieved if we construct a complete system of invariants for number fields. For the latter problem there are two known methods. The first follows from Dedekind-Frobenius theory (see §3). This method is inconvenient due to the infinite number of invariants, that are linked to one another using very few known relations. The second method is based on the behavior of the field discriminant. However, there is no known invariant system of this kind which determines a field uniquely. Besides this we have that the field discriminant cannot take on every integer value, and to this day we do not know what number values it can take on.

  3. 3.

    There is however a purely algebraic method for the solution of the identity problem. Given KK and K1K_{1} fields to consider, with isomorphic [Galois] groups 𝔊\mathfrak{G}, we have in general that the compositum KK1KK_{1} has the direct product 𝔊×𝔊\mathfrak{G}\times\mathfrak{G} as its Galois group. If KK and K1K_{1} have an irrational intersection, we have that the [Galois] group of KK1KK_{1} becomes a proper subgroup of 𝔊×𝔊\mathfrak{G}\times\mathfrak{G}. In particular, if KK and K1K_{1} are identical, it follows that the [Galois] group of KK1KK_{1} is isomorphic to 𝔊\mathfrak{G}. From this one can derive derive a usesful criterion for whether KK and K1K_{1} are identical. Specifically, if

    xn+a1xn1++an1x+an=0,yn+b1yn1++bn1y+bn=0x^{n}+a_{1}x^{n-1}+...+a_{n-1}x+a_{n}=0,y^{n}+b_{1}y^{n-1}+...+b_{n-1}y+b_{n}=0 (5.1)

    are the equations whose individual roots generate the fields KK and K1K_{1} respectively, it follows that K=K1K=K_{1} if and only if one of the quantities

    x1ky1+x2ky2++xnkyn(k=1,2,,n1)x_{1}^{k}y_{1}+x_{2}^{k}y_{2}+...+x_{n}^{k}y_{n}\quad\quad(k=1,2,...,n-1)

    is rational, where x1,x2,,xnx_{1},x_{2},...,x_{n} and y1,y2,,yny_{1},y_{2},...,y_{n} denote the roots of the equations in (5.1). Each of the quantities x1ky1+x2ky2++xnkynx_{1}^{k}y_{1}+x_{2}^{k}y_{2}+...+x_{n}^{k}y_{n} satisfies an equation of degree n!n!, whose coefficients are rational expressions of the ai,bia_{i},b_{i}. The fields KK and K1K_{1} are thus identical if and only if this equation possesses at least one rational root. Moreover, if 𝔊\mathfrak{G} has known normal subgroups, one can reduce the degree of this (“mixed”) equation using mixed resolvents [78].

  4. 4.

    We will examine the n=3n=3 and n=4n=4 cases more closely. Given

    x3+px+q=0,y3+p¯y+q¯=0x^{3}+px+q=0,y^{3}+\overline{p}y+\overline{q}=0

    as the equations under consideration, we first require that the product of their discriminants is a perfect square. The quantity z=x1y1+x2y2+x3y3z=x_{1}y_{1}+x_{2}y_{2}+x_{3}y_{3} satisfies on the mixed equations

    z33pp¯z272qq¯±DD¯=0.z^{3}-3p\overline{p}z-\frac{27}{2}q\overline{q}\pm\sqrt{D\overline{D}}=0.

    Provided that zz is one of its rational roots, and if z3pp¯0z^{3}-p\overline{p}\neq 0, one can determine the coefficients of the rational map y=α0+α1x+α2x2y=\alpha_{0}+\alpha_{1}x+\alpha_{2}x^{2} from the equations

    3α02pα2=0,2pα13qα2=z1,2pα03qα1+2p2α2=u,3\alpha_{0}-2p\alpha_{2}=0,-2p\alpha_{1}-3q\alpha_{2}=z_{1},-2p\alpha_{0}-3q\alpha_{1}+2p^{2}\alpha_{2}=u,

    where u=x12y1+x22y2+x32y3=3(qp¯zp2q¯)z2pp¯u=x_{1}^{2}y_{1}+x_{2}^{2}y_{2}+x_{3}^{2}y_{3}=\frac{3(q\overline{p}z-p^{2}\overline{q})}{z^{2}-p\overline{p}}.
    Now we will consider the case n=4n=4. Given equations

    x4+p2x2+p3x+p4=0,x¯4+p¯2x¯2+p¯3x¯+p¯4=0x^{4}+p_{2}x^{2}+p_{3}x+p_{4}=0,\overline{x}^{4}+\overline{p}_{2}\overline{x}^{2}+\overline{p}_{3}\overline{x}+\overline{p}_{4}=0

    to consider, we will initially solve the problem for the cubic equations

    z3p2z24p4zp32+4p2p4=0,z¯3p¯2z¯24p¯4z¯p¯32+4p¯2p¯4=0,z^{3}-p_{2}z^{2}-4p_{4}z-p_{3}^{2}+4p_{2}p_{4}=0,\overline{z}^{3}-\overline{p}_{2}\overline{z}^{2}-4\overline{p}_{4}\overline{z}-\overline{p}_{3}^{2}+4\overline{p}_{2}\overline{p}_{4}=0,

    which we know are satisfied by the quantities z=x1x2+x3x4z=x_{1}x_{2}+x_{3}x_{4} and z¯=x¯1x¯2+x¯3x¯4\overline{z}=\overline{x}_{1}\overline{x}_{2}+\overline{x}_{3}\overline{x}_{4} respectively. Next, if we introduce the expressions

    ζ=z1z¯1+z2z¯2+z3z¯3,u=z12z¯1+z22z¯2+z32z¯3,u¯=z1z¯12+z2z¯22+z3z¯32\zeta=z_{1}\overline{z}_{1}+z_{2}\overline{z}_{2}+z_{3}\overline{z}_{3},\quad u=z_{1}^{2}\overline{z}_{1}+z_{2}^{2}\overline{z}_{2}+z_{3}^{2}\overline{z}_{3},\quad\overline{u}=z_{1}\overline{z}_{1}^{2}+z_{2}\overline{z}_{2}^{2}+z_{3}\overline{z}_{3}^{2}

    it follows that the equation

    F(T)=T4(2p2p¯2+2ζ)T28p3p¯3T13ζ283p2u¯83p¯2u+148p2p¯2ζ+p22p¯22+16p22p¯4+16p¯22p4+643p4p¯4=0F(T)=T^{4}-(2p_{2}\overline{p}_{2}+2\zeta)T^{2}-8p_{3}\overline{p}_{3}T-\tfrac{1}{3}\zeta^{2}-\tfrac{8}{3}p_{2}\overline{u}-\tfrac{8}{3}\overline{p}_{2}u+\tfrac{14}{8}p_{2}\overline{p}_{2}\zeta+p_{2}^{2}\overline{p}_{2}^{2}+16p_{2}^{2}\overline{p}_{4}+16\overline{p}_{2}^{2}p_{4}+\tfrac{64}{3}p_{4}\overline{p}_{4}=0

    has at least one rational root. If we also have F(T)0F^{\prime}(T)\neq 0, it follows that one can determine the coefficients α0,α1,α2,α3\alpha_{0},\alpha_{1},\alpha_{2},\alpha_{3} of the map x=α0+α1x+α2x2+α3x3x=\alpha_{0}+\alpha_{1}x+\alpha_{2}x^{2}+\alpha_{3}x^{3} from the equations

    4α02p2α23p3α3=0,2p2α13p3α2+(2p224p4)α3=T,4\alpha_{0}-2p_{2}\alpha_{2}-3p_{3}\alpha_{3}=0,-2p_{2}\alpha_{1}-3p_{3}\alpha_{2}+(2p_{2}^{2}-4p_{4})\alpha_{3}=T,
    2p2α03p3α1+(2p224p4)α2+5p2p3α3=θ,-2p_{2}\alpha_{0}-3p_{3}\alpha_{1}+(2p_{2}^{2}-4p_{4})\alpha_{2}+5p_{2}p_{3}\alpha_{3}=\theta,
    3p3α0+(2p224p4)α1+5p2p3α2+(2p23+3p32+6p2p4)α3=Z,3p_{3}\alpha_{0}+(2p_{2}^{2}-4p_{4})\alpha_{1}+5p_{2}p_{3}\alpha_{2}+(-2p_{2}^{3}+3p_{3}^{2}+6p_{2}p_{4})\alpha_{3}=Z,

    where:

    θ=x12x¯1+x22x¯2+x32x¯3+x12x¯1,\theta=x_{1}^{2}\overline{x}_{1}+x_{2}^{2}\overline{x}_{2}+x_{3}^{2}\overline{x}_{3}+x_{1}^{2}\overline{x}_{1},
    Z=x13x¯1+x23x¯2+x33x¯3+x43x¯4.Z=x_{1}^{3}\overline{x}_{1}+x_{2}^{3}\overline{x}_{2}+x_{3}^{3}\overline{x}_{3}+x_{4}^{3}\overline{x}_{4}.
  5. 5.

    Given KK an algebraic function field, we have that Galois theory admits no applications to the solution of the identity problem. If KK possesses just one independent variable, this problem is solvable with the aid of function-theoretic means. If its genus is namely p>1p>1, it follows that KK is determined by 3p33p-3 independent continuous parameter values. For the equations generating such fields there are known normal forms. If we find a normal form for each of the fields to be compared, the problem is solved by their compilation ([3], p. 90-92).
    If KK depends on multiple independent variables then the problem remains unsolved in general. The old German and the Italian geometers obtained several extraordinarily important results in this area. Yet I fear that even today, regarding this, we must repeat the following phrase, contained in the Zürich lecture of F. Enriques [19]:
    «Malheuresement la plupart de ces problèmes demeurent aujourd’hui sans réponse, et les contributions qu’on a portées dans ce champ de recherches resemblement en vérité à de rares flambeaux au milieu d’une obscurité épaisse.»
    [English: Unfortunately, the majority of these problems remain unanswered, and the contributions we have reached in this area of research truly resemble rare torches in the middle of a thick darkness.]

  6. 6.

    Rational minimal basis. If we consider the field KnK_{n} of all rational functions in nn independent variables x1,x2,,xnx_{1},x_{2},...,x_{n}, the question seeking all possible types of its subfields arises. One can easily set up “trivial” examples of such subfields: that is one takes some number mnm\leq n of functionally independent elements of KnK_{n} (i.e. rational functions of x1,x2,,xn)x_{1},x_{2},...,x_{n}) as generating elements of a subfield. The field constructed in this manner is obviously either isomorphic to KnK_{n} or with the field KmK_{m} of rational functions in mm (m<nm<n) variables. One can however expect the existence of other kinds of fields: one can take a subfield generated by some number elements in KnK_{n} that may be linked with one another by algebraic relations. The question arises whether the “trivial” instances of subfields comprise all subfields exhaustively. In other words, one asks after the existence of a system of independent elements of the subfield, by which all elements of this subfield may be represented. Such a system is called a rational minimal basis.
    This question was answered affirmingly for n=1n=1 by Lüroth ([48]; see also E. Netto, [53]). G. Castelnuovo [15] extended this result to case of n=2n=2. His proof relies on the methods of algebraic geometry. In the case n=3n=3 we have a counterexample due to G. Fano [21] and F. Enriques [20], which they obtained by constructing a subfield of a field of rational functions in three variables admitting no rational minimal basis.
    The problem of the rational minimal basis has an application in the classical Galois theory, namely to the question after the existence of fields with prescribed Galois groups (§2). To answer the latter question it is necessary to solve the problem of the rational minimal basis solely in the case where the subfield under consideration contains the field of elementary symmetric functions of a system of generating elements for KnK_{n}. Given this restriction we have that the problem of the rational minimal basis is neither settled nor refuted (see [74]).
    This problem can also be understood in terms of the problem of identity of fields. That is, if among the generating elements of a subfield K¯\overline{K} of KnK_{n}, mm (mnm\leq n) are functionally independent, the question is reduced to proving the identity (more specifically: isomorphism) of K¯\overline{K} and KmK_{m}.

  7. 7.

    Simplest solution of equations of multiple variables. Let KK be a field of rational functions in nn variables x1,x2,,xnx_{1},x_{2},...,x_{n}, which satisfy the algebraic relation f(x1,x2,,xn)=0f(x_{1},x_{2},...,x_{n})=0 (the case of several relations can very easily be reduced to this case). One wishes to choose new generating elements y1,y2,..,yny_{1},y_{2},..,y_{n} for KK in such a way that the equation relating the yiy_{i} is of as small of a degree as possible in one of them, say y1y_{1}. What can one say about this degree?
    This question was treated comprehensively by Enriques [19] at the first international congress of mathematicians (Zürich, 1897). I will allow myself to recall some of the nice results considered there.
    1) We consider x1,x2x_{1},x_{2} as variables and x3,x4,,xnx_{3},x_{4},...,x_{n} as parameters. If the genus of the equation f(x1,x2)=f(x1,x2,x3,,xn)=0f(x_{1},x_{2})=f(x_{1},x_{2},x_{3},...,x_{n})=0 is identically zero, one can choose a variable tt in such a way that x1,x2x_{1},x_{2} may be expressed rationally by t,x3,x4,,xnt,x_{3},x_{4},...,x_{n} and a square root of a rational function of x3,x4,,xnx_{3},x_{4},...,x_{n} (M. Noether, [56]).
    For n=3n=3, one can eliminate the quadratic irrationality using an appropriately chosen tt.
    One can suspect that this theorem is meaningful for finding fields with prescribed Galois group 𝔊\mathfrak{G}. The latter problem seems easier to solve when the group 𝔎/𝔊\mathfrak{K}/\mathfrak{G} is of odd order, where 𝔎\mathfrak{K} denotes the holomorph of the group 𝔊\mathfrak{G}.
    2) If the genus pp of the equation f(x1,x2)=0f(x_{1},x_{2})=0 is >1>1, the field KK can be solved by adjoining an irrationality of degree 2p2\leq 2p-2.
    Solely for the case p=1p=1 it is impossible to specify the upper bound for the degree of this irrationality.

  8. 8.

    “True transcendence degree” of an extension field. Let kk be a field of rational functions in u1,u2,,unu_{1},u_{2},...,u_{n}, that may be linked by an algebraic relation

    f(u1,u2,,un)=0.f(u_{1},u_{2},...,u_{n})=0. (5.2)

    In addition, let KK be an extension field of the same transcendence degree, whose generating elements x1,x2,,xnx_{1},x_{2},...,x_{n} are related to the uiu_{i} by the equations

    φ1(x1,x2,,xn)=u1,φ2(x1,x2,,xn)=u2,,φn(x1,x2,,xn)=un.\varphi_{1}(x_{1},x_{2},...,x_{n})=u_{1},\quad\varphi_{2}(x_{1},x_{2},...,x_{n})=u_{2},...,\varphi_{n}(x_{1},x_{2},...,x_{n})=u_{n}. (5.3)

    One should find a subfield K1K_{1} of KK such that

    1. i)

      The compositum of K1K_{1} and kk is precisely the field KK;

    2. ii)

      THe transcendence degree of K1K_{1} is as small as possible.

    We will refer to the transcendence degree of K1K_{1} as the true transcendence degree of K/kK/k. It is evident that every problem in field theory becomes significantly easier upon reducing the transcendence degree of the field in question. Therein lies the significance of this problem.
    A special case of this problem manifests itself as the so-called resolvent problem (§4). To turn this into the resolvent problem, we must first specialize the equations (5.3) in the following way:

    x1+x2++xn=u1,x1x2+xn1xn=u2,x1x2xn=(1)nun.x_{1}+x_{2}+...+x_{n}=-u_{1},\quad x_{1}x_{2}+...x_{n-1}x_{n}=u_{2},\quad x_{1}x_{2}...x_{n}=(-1)^{n}u_{n}.

    In other words, the xix_{i} are the roots of the equation

    xn+u1xn1++un1x+un=0,x^{n}+u_{1}x^{n-1}+...+u_{n-1}x+u_{n}=0,

    while kk is generated by u1,u2,,unu_{1},u_{2},...,u_{n} and a function Φ\Phi belonging to a given permutation group 𝔊\mathfrak{G}, which itself is connected to the uiu_{i} through an easily presentable equation.
    The resolvent problem and its extension, the problem concerning the chains of resolvents are both tasks at the limits of classical Galois theory. The resolvent problem admits a solution via the theory of continuous groups (§4).

  9. 9.

    Rationality questions for the periods of elliptic and abelian integrals. We first of all consider the case of an elliptic variety. Let K(x,y)K(x,y) be an algebraic function field, where both xx and yy are subject to the equation

    y2(1x2)(1k2x2)=0.y^{2}-(1-x^{2})(1-k^{2}x^{2})=0. (5.4)

    In this case it is common knowledge that one can unformize xx and yy through elliptic functions

    x=sn(u,k),y=cn(u,k)dn(u,k).x=sn(u,k),\quad y=cn(u,k)dn(u,k). (5.5)

    In addition let (x0,y0)(x_{0},y_{0}) be a given point on the variety (5.4), to which the value u=u0u=u_{0} of the argument uu corresponds:

    x0=sn(u0,k),y0=cn(u0,k)dn(u0,k).x_{0}=sn(u_{0},k),\quad y_{0}=cn(u_{0},k)dn(u_{0},k).

    u0u_{0} is unambiguously determined up to a constant multiple of the periods 4K,4K4K,4K^{\prime}. It must be decided whether u0u_{0} is a rational multiple of 4K,4K4K,4K^{\prime}.
    This task may also be formulated as a problem in classical Galois theory. As a matter of fact, we can assume that k,x0,y0k,x_{0},y_{0} are algebraic numbers, since this case alone provides challenges. We additionally assume that the domain of rationality RR contains a the module kk. If u0mK+mKn (modd 4K,4K)u_{0}\equiv\frac{mK+m^{\prime}K^{\prime}}{n}\text{ (modd $4K,4K^{\prime}$)}, where m,m,nm,m^{\prime},n are integers, then x0=sn(mK+mKn,k)x_{0}=sn\left(\frac{mK+m^{\prime}K^{\prime}}{n},k\right) satisfies a so-called divison equation

    Φn(x0,k)=0,\Phi_{n}(x_{0},k)=0, (5.6)

    which is irreducible in the variable kk, but can factor within RR if kk takes on certain values. Now let f(x0)=0f(x_{0})=0 be the irreducible equation satisfied by x0x_{0}. The question is whether there are values of nn for which Φn(x,k)\Phi_{n}(x,k) is divisible by f(x)f(x).

  10. 10.

    If we designate points of the Riemann surface, for which snu=snu0sn\;u=sn\;u_{0} holds as P1P_{1} and P2P_{2}, our condition can be viewed in the following sense:

    nu(P1)nu(P2) (modd 4K,4K),n\;u(P_{1})-n\;u(P_{2})\equiv-\text{ (modd $4K,4K^{\prime}$)},

    where u(P)u(P) is the integral of the first kind. It follows from Abel’s theorem that there exists a function φ(x,y)\varphi(x,y) belonging to the field K(x,y)K(x,y), that has a single zero of order nn at P1P_{1} and a single pole of order nn at P2P_{2}. One can also say that the ideal P1nP2n\frac{P_{1}^{n}}{P_{2}^{n}} is principal. It follows that one can express φ\varphi using a prime function, i.e. in the form φ=enΠ(P1,P2)\varphi=e^{n\cdot\Pi(P_{1},P_{2})}, where Π(P1,P2)\Pi(P_{1},P_{2}) denotes the integral of the third kind with residues +2πi+2\pi i at P1P_{1} and 2πi-2\pi i at P2P_{2}.
    One can construct the function zz of second order, that becomes infinite at P1P_{1} and P2P_{2} (for example, one sets due to Zolotarev z=sn2(u,k)sn2(u,k)=sn2(u0,k)z=\frac{sn^{2}(u,k)}{sn^{2}(u,k)=sn^{2}(u_{0},k)}). This brings Π(P1,P2)\Pi(P_{1},P_{2}) to the form

    z+Az(z1)(zα)(zβ)𝑑z,\int\frac{z+A}{\sqrt{z(z-1)(z-\alpha)(z-\beta)}}dz,

    where α=1dn2u0\alpha=\frac{1}{dn^{2}u_{0}} and β=1cn2u0\beta=\frac{1}{cn^{2}u_{0}}, and it is of interest to recognize whether this integral (for suitable values of AA, whose choice comes from the normalizing of the periods in Π(P1,P2)\Pi(P_{1},P_{2})) is integrable by logarithms.

  11. 11.

    This question was initially posed by Abel [1]. Abel solved this problem in an algebraic way, by using the fact that φ=P1nP2n\varphi=\frac{P_{1}^{n}}{P_{2}^{n}} is a functional unit, i.e. the norm of φ\varphi is constant, and solved the Diophantine equation p2q2Rp^{2}-q^{2}R that arises from φ=p+qRpqR\varphi=\frac{p+q\sqrt{R}}{p-q\sqrt{R}} using the continued fraction expansion of R(x)\sqrt{R(x)}. For this to be possible it is necessary and sufficient that the continued fraction expansion of R(x)\sqrt{R(x)} is periodic. However, this periodicity cannot be confirmed or denied after a finite number of steps without further effort. To do this is was necessary to give an upper bound on the possible period. This task was accomplished by P. Chebyshev [77] for the case when the coefficients of R(x)R(x) are rational and by G. Zolotarev [92] for real R(x)R(x) in generality.
    Chebyshev and Zolotarev produced this result, by performing the following transformations on the variables:

    uu+u0,kk,u02u0,α(β+α11+βα)2,β(β+α11+αβ)2,u\to u+u_{0},k\to k,u_{0}\to 2u_{0},\alpha\to\left(\frac{\beta+\alpha-1}{1+\beta-\alpha}\right)^{2},\beta\to\left(\frac{\beta+\alpha-1}{1+\alpha-\beta}\right)^{2}, (I)
    u(1+k)u,k1k1+k,α((βα)(β1)α1+αβ)2,β((βα)(β1)+α1+αβ)2,u\to(1+k^{\prime})u,k\to\frac{1-k^{\prime}}{1+k^{\prime}},\alpha\to\left(\frac{\sqrt{(\beta-\alpha)(\beta-1)}-\sqrt{\alpha}}{1+\alpha-\beta}\right)^{2},\beta\to\left(\frac{\sqrt{(\beta-\alpha)(\beta-1)}+\sqrt{\alpha}}{1+\alpha-\beta}\right)^{2}, (II)

    over and over. The transformation (II) has the purpose of mapping an even nn to an odd nn, and is nothing more than the Landen transformation. If after several steps the quantity 2k1+k\frac{2\sqrt{k}}{1+k} no longer lies in the field K(α,β)K(\alpha,\beta), this is an indication that the integral transformed in this way corresponds to an odd nn. At this point one must use the transformation (I). The answer is positive if the sequence of these transformations produces a period. On the other hand a finite number of steps produces divisibility criteria that render the task impossible.

  12. 12.

    The question regarding the commensurability of elliptic integrals is applicable to a far removed branch of mathematics, namely Diophantine analysis. Let the equation

    f(x,y)=0f(x,y)=0 (5.7)

    be given, whose coefficients belong to an algebraic number field KK and whose genus is p=1p=1. We are concerned with the existence of values x0,y0x_{0},y_{0} contained in the field KK and satisfying equation (5.7). In short these are called rational points of the curve (5.7). One can transform equation (5.7) into the form

    y2=4x3g2xg3,y^{2}=4x^{3}-g_{2}x-g_{3}, (5.8)

    possibly by extending the field KK. The curve (5.8) can be represented parametrically in the following manner:

    x=p(u),y=p(u).x=p(u),\quad\quad y=p^{\prime}(u). (5.9)

    If values u1,u2u_{1},u_{2} of the argument uu correspond to rational points of (5.8), it follows by the addition theorem that u1±u2u_{1}\pm u_{2} also correspond to rational points. In other words, the arguments of the rational points of the curve (5.8) form an additive module, that we will refer to as KK-rationality module in the sequel. H. Poincaré [59] suspected and L.J Mordell [51] proved that each rationality module possesses a finite basis.
    Given (u1,u2,,un)(u_{1},u_{2},...,u_{n}) such a basis, the question regarding the structure of the additive abelian group 𝔘\mathfrak{U} generated by this basis arises. Since one can reduce every value of the argument uu modulo ω1,ω2\omega_{1},\omega_{2}, where ω1,ω2\omega_{1},\omega_{2} are the periods of p(u),p(u)p(u),p^{\prime}(u), it follows that the number of independent generating elements of this group of infinite order (rank) is nn if and only there exists no congruence of the form

    m1u1+m2u2++mnun0(mod ω1,ω2)m_{1}u_{1}+m_{2}u_{2}+...+m_{n}u_{n}\equiv 0\text{(mod $\omega_{1},\omega_{2}$)} (5.10)

    between the uiu_{i}, where the mim_{i} are integers. However, in general the basis of 𝔘\mathfrak{U} consists of a number ρ\rho of elements A1,A2,,AρA_{1},A_{2},...,A_{\rho} of infinite order, and a number of elements B1,B2,,BσB_{1},B_{2},...,B_{\sigma} (ρ+σn\rho+\sigma\leq n) of finite order. The number ρ\rho was called the rank of rationality of the system u1,u2,,un (mod σ1,σ2)u_{1},u_{2},...,u_{n}\text{ (mod $\sigma_{1},\sigma_{2}$)} by Kronecker, i.e. the largest number of rationally independent elements. The Zolotarevian process allows us to determine rank of rationality in the case n=1n=1101010T. Nagell ([52], p. 96, line 10-11 v.o.) says, on n’a pas de méthode générale pour reconnaître si l’argument d’un point donné (x,y)(x,y) est commensurable avec une période ou non.[English: There is no general method to know if the argument of a given point (x,y)(x,y) is commensurable with a period or not.] This problem has actually solved in the aforementioned investigations by Zolotarev., and hopefully allows for a direct extension to the general case.

  13. 13.

    One can formulate the problems arising from these reflections in the following way:

    1. I.

      One finds a method to decide whether the value aa of the argument uu defined by the equations sna=x0,cna.dna=y0sn\;a=x_{0},cn\;a.dn\;a=y_{0} (or: p(a)=x0,p(a)=y0)p(a)=x_{0},p^{\prime}(a)=y_{0}) is commensurable with the periods or not.
      It is only important to answer the question in the case where the Landen transformation of a given function is periodic. The case is not applicable when the curve (5.4) (or (5.8)) is real.

    2. II.

      One determines the rank of rationality of a module/modulus (u1,u2,,un)(mod ω1,ω2)(u_{1},u_{2},...,u_{n})(\text{mod }\omega_{1},\omega_{2}), where the uiu_{i} are to be determined from the equations p(ui)=xi,p(ui)=yip(u_{i})=x_{i},p^{\prime}(u_{i})=y_{i} and ω1,ω2\omega_{1},\omega_{2} denote the periods of the elliptic function p(u)p(u).

    3. III.

      Let an elliptic function field (perhaps through specification of the module/modulus kk) and an algebraic number field KK containing kk be given. One must find a basis of the corresponding KK-rationality module/modulus. If a basis (u1,u2,,un)(u_{1},u_{2},...,u_{n}) (through explicit specification of the values of p(ui))p(u_{i})) is given, one decided whether it is a basis of the KK-rationality module/modulus or not.

  14. 14.

    One can transfer the formulation of the aforementioned tasks to general algebraic functions without much fuss. First of all it seems reasonable that the question regarding the finiteness of an algebraically specified transformation of the “Jacobian group” descibed in §1, No. 9 is closely related to the question regarding the integrability of abelian integrals by logarithms. On the other hand one can readily transfer the reflections in No. 10 to the general case. This also shows that there is a certain relationship between the Jacobian group and the ideal class groups of an algebraic function field. However, this problem is linked with the question concerning the functional units.111111This connection was brought to my attention by my highly respected teacher Prof. Dr. D. Grave. See for example Verh. Russ. Math. Kongreß in Moscow (1927), p. 215 (Russian).
    A. Weil [87] investigated Diophantine equations f(x,y)=0f(x,y)=0 of arbitrary pp using a similar method. In particular he extended Mordell’s resullt about the finiteness of KK-rationality modules/moduli for arbitrary p1p\geq 1. To do so he used the Jacobian group, while Mordell [51] implicitly used the division of elliptic functions.

  15. 15.

    The Diophantine problem can be considered as a special case of the Hilbert-Doerge irreducibility problem:
    Let an equation f(z,t)=0f(z,t)=0 be given. One must find all values tit_{i} of tt for which f(z,ti)f(z,t_{i}) is a reducible polynomial in a prescribed number field kk.
    According to KK Doerge it follows from the investigations of Weil [87] that for p>1p>1 tt takes on infinitely many such values only if f(z,t)f(z,t) can be transformed using a transformation of the form

    t=cmum+cm+1um+1++c0+c1u++cmumt=c_{-m}u^{-m}+c_{-m+1}u^{-m+1}+...+c_{0}+c_{1}u+...+c_{m}u^{m}

    into an identically decomposing polynomial in zz and uu 121212Amendment while correcting. In this direction significant new results have been obtained by C.R. Siegel (Abh. preuss. Akad., Berlin, 1930, No 1)..
    The work of Doerge under discussion is devoted to the case where zz is a functional unit. Then Doerge obtains very easy conditions for when f(z,t)f(z,t) is only reducible for a finite number of values of tt in kk. It is remarkable that this results in a new direct connection between the Diophantine equations and the functional units.

(Submitted the 12th of September, 1932)

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