Научная статья на тему 'On the second memoir of évariste Galois’ last letter'

On the second memoir of évariste Galois’ last letter Текст научной статьи по специальности «Математика»

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Ключевые слова
ЭССЕНЦИАЛЬНАЯ ЭЛЛИПТИЧЕСКАЯ ФУНКЦИЯ / ПОНИЖЕНИЕ СТЕПЕНИ МОДУЛЯРНОГО УРАВНЕНИЯ / ПРОЕКТИВНАЯ СПЕЦИАЛЬНАЯ ЛИНЕЙНАЯ ГРУППА НАД ПРОСТЫМ ПОЛЕМ / ЭЛЛИПТИЧЕСКИЕ И КОЭЛЛИПТИЧЕСКИЕ ПОЛИНОМЫ / РЕШЕНИЕ ОБЩЕГО КВИНТИЧЕСКОГО УРАВНЕНИЯ / ESSENTIAL ELLIPTIC FUNCTION / DEPRESSING THE DEGREE OF THE MODULAR EQUATION / PROJECTIVE SPECIAL LINEAR GROUP OVER A PRIME FIELD / ELLIPTIC AND COELLIPTIC POLYNOMIALS / SOLVING THE GENERAL QUINTIC EQUATION

Аннотация научной статьи по математике, автор научной работы — Adlaj Semjon F.

Évariste Galois' last letter, addressed to Auguste Chevalier, on the eve of the (so-called) duel on May 30, 1832 (which, perhaps, simpler and more accurately described by Alfred, who did not allow a priest to deprive him from the final moments on the following day with his elder brother Évariste, as murder), was written on seven pages and was divided into three memoirs. The first memoir consumes a little less than two pages. It gave rise to what has come to be known as Galois theory (as, in particular, told by Melvin Kiernan). Yet Galois went on with stunningly amazing constructions in the second memoir, which consumed a bit more than two pages. The third (and longest!) memoir begins on the fifth page and remains mysteriously unresolved, yet it undoubtedly inspired Alexander Grothendieck to formulate his period conjecture. The letter is concluded with a paragraph on the latest "principal contemplations", concerning "the applications of the theory of ambiguity to transcendental analysis", where Galois delivers his last puzzle to us, saying that "one recognizes immediately lots of expressions to look for". Unfortunately, the severity of the time pressure upon him permitted only succinct last instructions with no more last examples. Still and disgracefully, many "historians" keep on incessantly and mundanely telling us (and each other) that we ought not "overestimate" the significance of the letter, which was (contrary to their advice) eloquently and veraciously described by Hermann Weyl as "the most substantial piece of writing in the whole literature of mankind"!

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О втором мемуаре последнего письма Эвариста Галуа

Последнее письмо Эвариста Галуа, адресованное Огюсту Шевалье, накануне (так называемой) дуэли 30 мая 1832 года (которая, пожалуй, проще и точнее была охарактеризована как убийство Альфредом, не допустившим на следующий день священника к своему старшему брату Эваристу в его последние мгновения), было написано на семи страницах и разделено на три мемуара. Первый мемуар занимает чуть меньше двух страниц. Впоследствии сей мемуар стал известен как теория Галуа (о которой, в частности, рассказал Мелвин Кирнан). Однако, Галуа продолжил своё письмо потрясающе удивительными конструкциями во втором мемуаре, который занял чуть более двух страниц. Третий (и самый длинный!) мемуар начинается на пятой странице и остаётся загадочным и нерасшифрованным, но он, несомненно, вдохновил Александра Гротендика сформулировать свою гипотезу о периодах. Письмо заканчивается абзацем о последних «главных размышлениях», касающихся «приложений теории неоднозначности к трансцендентному анализу», где Галуа преподносит нам последнюю загадку, говоря, что «мы можем тотчас же рассмотреть большое множество выражений». К сожалению, неумолимость давлеющего времени не позволила ему привести какие-либо конкретные примеры, а смогла лишь дать краткие последние инструкции, о том, что делать с письмом. Несмотря на это, многие «историки» назойливо и примитивно твердят нам (и друг другу), что мы не должны «переоценивать» значение письма, которое (вопреки их советам) красноречиво и правдиво описывалось Германом Вейлем как «самая значимая рукопись во всей истории человечества»!

Текст научной работы на тему «On the second memoir of évariste Galois’ last letter»

Computer tools in education, 2018 № 4:11-26

http://ipo.spb.ru/journal doi:10.32603/2071-2340-4-11-26

ON THE SECOND MEMOIR OF EVARISTE GALOIS' LAST LETTER

Adlaj S. F.

Federal Research Center "Informatics and Control", Moscow, Russia

Abstract

Evariste Galois' last letter, addressed to Auguste Chevalier, on the eve of the (so-called) duel on May 30,1832 (which, perhaps, simpler and more accurately described by Alfred, who did not allow a priest to deprive him from the final moments on the following day with his elder brother Evariste, as murder), was written on seven pages and was divided into three memoirs. The first memoir consumes a little less than two pages. It gave rise to what has come to be known as Galois theory (as, in particular, told by Melvin Kiernan). Yet Galois went on with stunningly amazing constructions in the second memoir, which consumed a bit more than two pages. The third (and longest!) memoir begins on the fifth page and remains mysteriously unresolved, yet it undoubtedly inspired Alexander Grothendieckto formulate his period conjecture. The letter is concluded with a paragraph on the latest "principal contemplations", concerning "the applications of the theory of ambiguity to transcendental analysis", where Galois delivers his last puzzle to us, saying that "one recognizes immediately lots of expressions to look for". Unfortunately, the severity of the time pressure upon him permitted only succinct last instructions with no more last examples. Still and disgracefully, many "historians" keep on incessantly and mundanely telling us (and each other) that we ought not "overestimate" the significance of the letter, which was (contrary to their advice) eloquently and veraciously described by Hermann Weyl as "the most substantial piece of writing in the whole literature of mankind"!

Keywords: Essential elliptic function, depressing the degree of the modular equation, projective special linear group over a prime field, elliptic and coelliptic polynomials, solving the general quintic equation.

Citation: S. F. Adlaj, "On the Second Memoir of Evariste Galois' Last Letter," Computer tools in education, no. 4, pp. 11-26, 2018. doi:10.32603/2071-2340-4-11-26

1The quote concerns Galois' last letter. It is taken from page 79 of a 154-page survey on [15, The Development of Galois Theory from Lagrange to Artin] by M. B. Kiernan.

The sections of the second memoir dealing with elliptic integrals were never written, nor, apparently, was any part of the third memoir. The outline of this material in the letter to Chevalier was very sketchy, and did not influence later mathematics.1

1. AN ESSENTIAL ELLIPTIC FUNCTION AND ITS MODULAR INVARIANT

Given a parameter p e C \ {-1,0,1}, introduce an essential elliptic function, as in [1, 2, 4, 6, 9], that is a (meromorphic) function R = Rp = Rp(-) = R(■,p), possessing a (double) pole at the origin and satisfying the differential equation

R'2 = 4R (R + p)(R + 1/p). (1)

Denote the lattice of the function Rp by Ap, and call the parameter p the elliptic modulus. The map

z- (1,Rp(z),R'p(z)),

extends, with 0 — (0,0,1), to a map from the period-parallelogram C/Ap into the complex projective space PC2. The (extended) map induces, onto its image Ep, which we shall call the associated elliptic curve,2 an isomorphism of Riemann surfaces, as well as, an isomorphism of groups.3 This map, further, enables an identification (exploiting the j-invariant) of isomorphism classes of projective complex elliptic curves with homothety classes of lattices L/Cx, which might, in turn, be identified with the fundamental domain r\H, for the action of the modular group r := PSL(2, Z), upon the upper half plane H, as is well explained in [17]. From now on, we exploit the identification of the points on the torus C/Ap, which might be viewed as the domain of Rp, with the points on the elliptic curve Ep, which might be viewed as the image of the functional pair (Rp, Rp). Keeping in mind that the value of the function Rp determines, up to a sign, via equation (1), the value of its derivative R'p, we might further identify a pair of (not necessarily distinct) points on Ep, sharing a first coordinate, with their corresponding pair of points in the domain of Rp, which image (under Rp) coincide with that very first coordinate. Fix the elliptic modulus p, and express the defining equation for the (already introduced) elliptic curve Ep as

Ep : y2 = 4xq(x), q(x) := x2 + (p + 1/p) x + 1.

The justification for such canonical representation of elliptic curves (not to be confused with the Weierstrass normal form) is provided in the afore-indicated references [1, 2, 4, 6, 9].4 Two distinct points (x1, y1) and (x2, y2) might be summed (on Ep) to a point (x3, y3), which first coordinate satisfy the addition formula

x3 = fii^^i )2. (2)

4 x1x2 x1 - x2

Now, denoting by n ■ (x, y) the multiplication of the point (x, y) by n, and denoting by (n ■ x, n ■ y) the n-multiple of the point (x, y) on Ep, so that (n ■ x, n ■ y) = n ■ (x, y), the doubling formula expresses the first coordinate 2 ■ x of the point 2 ■ (x, y), as calculated in [1],

p2(x) f x2 - 1)2

2■ x = ——, p2(x):= —— , q2(x):= xq(x). (3)

q2(x) I 2 j

When n is an arbitrary integer, the multiplication by n amounts to successively multiplying by its prime factors (counted with their respective multiplicities), so we want to deduce a multiplication by an odd prime formula. Assuming n to be odd (not necessarily prime!), exceeding

2Without, necessarily, further specifying whether the association pertains to the elliptic function Rp, its lattice Ap or the elliptic modulus p.

3The curve Ep is, thereby, said to be a one-dimensional complex Lie group.

4We shall, furthermore, employ this representation for attaining an explicit inverse of the modular invariant.

2, we might (recursively) deduce such a formula, expressing the first coordinate of the n-odd-multiple point as a degree n2 fractional transformation of the first coordinate of the point to be multiplied, that is,

n ^ x = PnOc), xn2r( M , qn(x) := rn(x)2,

qn (x) (xj

(n -1)2 (xqn-i(x) - pn-i(x)) , , ,

rn(x) :=-----—-, ri(x) := 1. (4)

n (n - 2) rn-2(x)

An explicit formula for n ■ x relies on an explicit formula for (n -1) ■ x as a fractional transformation with (coprime) polynomials pn-1 and qn-1 appearing in its numerator and denominator, respectively. Since n is odd, by assumption, the formula for (n - 1) ■ x might always be attained via the doubling formula applied to [n-r) ■ x. Note that the sequence {rn : n is odd} need not be extended to include elements rn with even indices, unlike pn and qn which are (successively) defined for all integer indices n (employing the doubling formula whenever the indices are even), and that, furthermore, if we choose the polynomials qn to be monic for all even n then so do become all (subsequent) polynomials rn (and qn). The roots of each rn are precisely the first coordinates of the points, aside from the identity point, on Ep, of order dividing n, so, in particular, the degree of rn is (n2 - 1)/2, and if m divides n then the polynomial rm(x) divides the polynomial rn (x).

The (monic) polynomial rn, which we have just introduced, has its coefficients in the field F := Q(p+1/p), that is, the field of rational functions in the transcendental (or algebraic) element P + 1/p, over the field of rational numbers Q.5 When n is an odd prime, as we now opt as being the default assumption, the roots of rn are the first coordinates of the points of order n on Ep. The assumption which will not be lifted (throughout this paper) that p2 e C \ {0,1} guarantees that the roots (of rn) are pairwise distinct. We shall call the polynomial rn the division polynomial of level n, and, whenever an emphasis on its dependence upon the elliptic modulus p is desired, we shall denote it as rn(■, P), still being at large viewing it either as a function of two variables or as a p-parametric polynomial function in a single variable.

The field F[ym], obtained by adjoining a root jm of rn to the base field F, is the splitting field for the elliptic polynomial of level n:

(n-1)/2

rmn(x) := n (x - l ■ Jm) . l=1

The polynomial rmn divides rn, and the first index (m) of rmn might be employed to designate n + 1 pairwise coprime elliptic polynomial factors of rn:

n

rn (x) = J] rmn (x).6

m=0

Put d(x) := x - 1/x, and d2(x) := x + 1/x - 2. Let d2 denote the discriminant of the quadratic polynomial q(x), which coincides with the discriminant of the cubic polynomial q2(x), so d2 = d(P)2 = d2(p2). The homothety class of the lattice Ap is represented by a (unique) point t in the

5No further restriction is imposed upon assuming that the coefficients of polynomials, in p + 1/p, appearing in the numerator and the denominator of a rational expression, in F, are integers.

6The elliptic polynomials were introduced in 2014 at the 7th annula PCA conference (http://pca.pdmi.ras.ru/2014/ program) in a talk titled "Modular Polynomial Symmetries", and at the 17th workshop on computer algebra (http: //compalg.jinr.ru/Dubna2014/abstracts.html) in a talk titled "Elliptic and Coelliptic Polynomials".

fundamental domain r\H, as we already mentioned. The (Klein) modular invariant j, which maps the upper half plane H onto C, is a modular form of weight zero. Its domain might be extended to include all rational real points, as well as, the point at (complex) infinity. All these points map (under j) to (complex) infinity. We shall emphasize that the modular invariant j is a (holomorphic) bijection between the (or any) extended fundamental domain and the Riemann sphere C u w.7 The domain of j might be further extended to include the lower half plane via setting j(-t) = j(t). The value of j at a point t, corresponding to the homothety class of the lattice Ap is

4 id2 + 1)3

j (T) = 27d^~' (5)

and since the said discriminant d2 is invariant under the substitutions p ^ -p and p ^ 1/p, so must be j (t). Moreover, j (t) is invariant under the substitutions p2 ^ 1 - p2. Thus, the homothety class of the lattice Ap as p2 undergoes the inversions (meaning linear fractional transformations of order 2)

1

S: x ^ —, T: x ^ 1 - x, (6)

x

is preserved. The latter two inversions generate a (6 element) group isomorphic with the symmetry group S3 of a triangle. The three functional (trigonometric) pairs

2 2 2 2 2 2 {-tan2, - cot2}, {sin2, cos2}, {csc2,sec2}

might be viewed as the three vertices, which are rotated via either the composition S o T or its inverse To S. The first vertex is invariant under the action of S which transposes the second vertex with the third, while the second vertex is invariant under the action of T which transposes the third vertex with the first, and the third is invariant under the action of the third inversion

x

SoToS = ToSoT: x>

x -1

which transposes the first vertex with the second. Generally, twelve distinct values of p correspond to a single point t in the fundamental domain. The exceptions are the values, corresponding to the corners of the fundamental domain. These are the six values p e {±i, ±1/ \/2, ± \/2}, corresponding to t = i :=%/—!, and the four values p e {±iZ, ±iZ2}, corresponding to t = Z.8 An isomorphism between elliptic curves as their elliptic modulus p undergoes permissible transformations (generated by S and T) might explicitly be given as a linear map between first coordinates. Evidently, the isomorphism corresponding to the transformation p ^ 1/p is given by the identity map x ^ x, and the isomorphism corresponding to the transformation p ^ -p is given by the map x ^ -x. The isomorphism corresponding to the transformation p ^ \J 1 - p2 is given by the map x ^ -(px + 1)/^1 - p2. Alternatively denoting the elliptic modulus p by sin0,9 the latter map between first coordinates:

l (x) = —x tan 0 - sec 0 (7)

is said to induce an isomorphism of elliptic curves, as the elliptic modulus p undergoes the transformation sin0 —>■ cos0.10

7The latter statement merely defines a modular form of weight zero.

8A reformulation involving a (instead of p) would be less cumbersome, perhaps, and so we give it here. Generally, six distinct values of a correspond to a single point t in the fundamental domain. The exceptions are the three values a e {0, ±1/ V2}, corresponding to t = i, and the two values a e {±1/ v/3}, corresponding to t = Z.

9The angle 0 is then called the modular angle.

10One readily verifies that the inverse of the linear map l is l-1 (x) = -x cot0 - csc0 correspond to the (reverse) transformation of the elliptic modulus cos 0 ^ sin0.

Since two elliptic moduli p and 1/p correspond to a single elliptic function Rp (and to a single elliptic curve Ep), only six elliptic functions R correspond to twelve values of the elliptic modulus, corresponding to a single point t in the fundamental domain. Only three distinct functions R correspond to the exceptional value t = i, and only two distinct functions R correspond to the exceptional value t = The term elliptic modulus, endowed upon the parameter p, is now seen to coincide with the same term appearing in connection with the Jacobi elliptic functions. The Jacobi elliptic sine function, corresponding to elliptic modulus p and denoted by snp = snp(-), satisfies the differential equation

snp2 = I1 - snp) f1 - p2snp),

and coincides, up to homothety and translation (of its argument), with a square root of the function R (analytically continued). Explicitly,

ß snß

2

z

Vßi

1 = R (z + ф} zo, -ß),11 zo : 711

R_ß(z) I V^ 0 П' 0- 2M(ß)'

where M(x) is the arithmetic-geometric mean of 1 and x; enlightening details about the function M are presented in [12]. As the elliptic modulus p = sin в undergoes the transformations, which we earlier discussed, corresponding elliptic functions R(-, - sin в), R(-, i tan в) and R(-, - sec в) coincide, up to homothety, translation and multiplicative constants, with the squares of the Jacobi elliptic functions snp, cnp and dnp. Putting к := 2 icsc(2e), the squares of the latter two Jacobi elliptic functions might be, explicitly, expressed as

2 к i z + z0 \

cnp(z)2 = 1--z-—-г-= i cot в R ——, i tan в ,

H R (z / л/к, i tan в + i tan в у/к )

2 sin в tan в f i--\

dnp(z)2 = 1 + —f-г-= cos в R v - cos в (z + z0), - sec в .

R V- cos в z, - sec в - sec в Respectively, they satisfy the differential equations:

cnp2 = f 1 - cnp) f 1 - p2 + p2cnp), dnp2 = f 1 - dnp) fp2 - 1 + dnp), as well as, the functional equations:

snp + cnp = 1 = p2snp + dnp.

Here, one must also bear in mind a simple and basic functional equation:

R(iz, p) = -R(z, -p).

2. AN EXPLICIT FAST INVERSION OF THE MODULAR INVARIANT

An explicit fast inverse k of the modular invariant j was given in [3] as a composition

k := k0 о ki о k2,

nNote that the leftmost side of the equality is unaltered by switching from a branch of the square root function, applied to p, in the expression for the argument of the (known to be odd) function snp, to the other.

where

iM( ^ - x2) ^x+4-Vx , 3 i x

ko(x):=-rr—.-, fci(x):=---, k2(x):=- —— + k3(x) -1,

M(x) 2 2 k3(x)

k3(x) := V Vx2 - x3 -x.

Strictly speaking, the function M is (doubly) infinitely-valued as its calculation entails choosing one of two branches of the square root function at infinitely many steps. Consequently, the function k is, as well, an infinitely-valued function. However, its values, up to a sign, differ by the action of the modular group r. We mean that by flipping the sign, if necessary, we might assume that the function k never assumes values in the lower half plane, and, furthermore, its values might be brought via the action of the modular group r to a single value in the (or any) fundamental domain. In other words, while k is not strictly a left inverse of j, it is a right inverse, that is,

Vx e C, j o k (x) = x,12

for the modular invariant j does not separate points, in its domain, as long as they differ by the action of the modular group r, and no troubles arise in extending the latter equality to the whole Riemann sphere, including the point at (complex) infinity.

Before we move on to the modular equation, we must clarify the calculation of the inverse function k for the two special values of j at the corners: j(Z) = 0 and j(i) = 1. So, we point out that the (set) values of the composition, ki o k2 at 0 and 1, coincide with exceptional (set) values of p at t = z and t = i, respectively. Certainly, k2 has a removable singularity at zero and must be evaluated to -1 there, whereas k2(1) = 1/2. Thus, z e k(0) = k0 o k1(-1), and i e k(1) =

k0 o k1(1/2).13

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An elementary proof of the fast inversion formula, being discussed here, is given in [16].

3. EXPLICITLY AND EFFICIENTLY SOLVING THE MODULAR EQUATION

Recalling our default assumption that n is an odd prime, the functional pair (j(t), j(ut)) is known to be algebraically dependent (over Q), and is said to satisfy the modular polynomial of level n, that is

On (j (t), j (ut)) = 0,

where the modular polynomial On possesses integer (rational) coefficients. Moreover, as explained in [18], On is symmetric in its two variables, that is On(x, z) = On(z,x).14 When t is

12 An analogy is afforded by a branch of the logarithmic function which is (regradless of the choice of the branch) a right (but not left) inverse of the exponential function. While the values of the logarithm, at a given point, constitute a discrete subset of a line, the values of the functions k and M do not. We have already indicated that the function M is (doubly) infinitely-valued, suggesting that its values (at a given point) constitute a discrete subset of C (not contained in any one-dimensinal subset over R), and so is the function k.

13Implying, unsurprisingly, that the values 0 and 1 are fixed by the (identity) function j o k.

14For a couple examples, the modular polynomials Og (x, y) and O^ (x,y), of degrees 3 and 5, were calculated by Smith (1879) and Berwick (1916), respectively:

O*(x,y) = x3y3 — 2232 (x3y2 + x2y3) — x4 — y4 + 1069956 (x3y + xy3) — 2587918086 x2y2 — 36864000 (x3 + y3) — 8900222976000 (x2y + y2x) — 452984832000000 (x2 + y2) + 770845966336000000 x y — 1855425871872000000000 (x + y), O|(x, y) = x5 y5 — 3720 (x5y4 + y4x5) + 4550940 (x5y3 + y5x3) — 1665999364600 x4y4 — 2028551200 (x5y2 + y5 x2) — 107878928185336800 (x4y3 + y4x3) — x6 — y6 + 246683410950 (x5 y + y5 x) — 383083609779811215375 (x4y2 + y4x2) + 441206965512914835246100 x3y3 — 1963211489280 (x5 + y5) — 128541798906828816384000 (x4y +

fixed, and so is j(t), the polynomial ®n(j(t),x) might be viewed as a polynomial in a single variable x over the (base) field Q( j(t)),15 and we shall call its roots, the roots of the modular equation of level n.

Now, let the value of j (t) be given by equation (5) then the values

. : 4 id2m + 1)3 d2 . d2(o2 ) o2 . Sm(-p) - sm (0) n

]m =—m-> =d m)> pm = smc-i/py-smco)'0 *m *n' (8)

Sm (x ):= nx - (6 x 2 + « x + 2) r'm n(x), 16 „ ;= 4 L + I) , rmn (x) I pi

are the (n+1) roots of the modular equation of level n.17 Evidently, each such root jm is invariant as p2m is subjected to the action of the triangle group S3, which is generated by the two inversions S and T given in (6). This action on p2m corresponds to the action of S3 as the permutation group of the three symbols {0, p, 1/p}, appearing on the right hand side of the defining expression for p2„ . One might be satisfied to verify that a value of one of the roots jm would coincide with j(nT). The elliptic curves Ep and Epm are said to be related by cyclic isogeny of degree n.

The projective special linear group Gn := PSL(2, Zn), where Zn is the (prime) field of integers modulo n (which we had earlier introduced), is the Galois group of the modular equation of level n. Not merely a Galois group in the conventional sense, but is the Galois group in a most spectacular sense. Galois, who was apparently the discoverer of finite fields, indicated, in his last letter [13], sufficient and necessary condition for depressing the degree of the modular equation of prime level.18 For this very purpose he did introduce the, being discussed, projective special linear groups over prime fields Gn, and observed that they were simple for all primes strictly exceeding the prime 3.19 For primes n > 5, he pointed out the three exceptions for which the groups Gn possessed subgroups of indices coinciding with the cardinality of the field n. These

y4x) - 26898488858380731577417728000 (x3 y2 + y3 x2) - 1284733132841424456253440 (x4 + y4) + 192457934618928299655108231168000 (x3 y + y3x) - 5110941777552418083110765199360000 x2y2 -280244777828439527804321565297868800 (x3 + y3) - 36554736583949629295706472332656640000 (x2y + y2x) -6692500042627997708487149415015068467200 (x2 + y2) + 264073457076620596259715790247978782949376 x y -53274330803424425450420160273356509151232000 (x + y) - 141359947154721358697753474691071362751004672000. Our reason for using the asterisk is to point out that j(i) was assumed to equal 123. There is no sound justification for this "popular choice", and so if we switch to the "correct" normalization with j(i) = 1, then the corresponding polynomials ®3(x, y) and ®s(x, y) become:

$3(x,y) = 2176782336 x3y3 - 2811677184 (x3y2 + y3x2) - 729 (x4 + y4) + 779997924 (x3y + y3x) - 1886592284694 x2y2 -15552000 (x3 + y3) - 3754781568000 (x2y + y2x) - 110592000000 (x2 + y2) + 188194816000000 x y- 262144000000000 (x + y), $5(x,y) = 8916100448256 x5y5 - 19194382909440 (x5y4 + y5x4) + 13589034024960 (x5y3 + y5x3) -4974647446705766400 x4y4 - 3505336473600 (x5 y2 + y5 x2) - 186414787904261990400 (x4y3 + y4x3) - x6 -y6 + 246683410950 (x5 y + y5 x) - 383083609779811215375 (x4y2 + y4x2) + 441206965512914835246100 x3 y3 -1136117760 (x5 + y5) - 74387615108118528000 (x4y + y4x) - 15566255126377738181376000 (x3y2 + y3x2) -430254526762844160 (x4 + y4) + 64453772899964735127552000 (x3y + y3x) - 1711644060233550509015040000 x2y2 -54313315434020926285414400 (x3 + y3) - 7084552847250663218872320000 (x2y + y2x) - 750608416927050074633011200 (x2 + y2) +29617595563122405481849552896 x y - 3457795560648760910413824000 (x + y) - 5309626171273360722362368000. Aided with computers, Andrew V. Sutherland went on to calculate the coefficients of three hundred modular polynomials, which he made generously accessible at https://math.mit.edu/~drew/ClassicalModPolys.html.

15 So, in fact, it might be viewed as a polynomial over the ring Z [ j (t)] .

16As before, the prime mark denotes differentiation with respect to the argument x, as p is assumed to be fixed.

17More details are given in author's article "Multiplication and division on elliptic curves, torsion points and roots of modular equations", which is accessible at http://www.ccas.ru/depart/mechanics/TUMUS/Adlaj/ECMD.pdf.

18The nowadays-established term "depressing" means lowering. Its conception is a simple (yet ingenious) idea with which Galois alone must be fully credited, and, as we shall soon see, is the single most crucial (yet rarely brought to awareness) step towards actually solving the quintic.

19The very concept of simplicity, being again introduced by Galois, provides the basic principle in classifying (finite)

were the primes 5, 7 and 11. For any prime n strictly exceeding 11, proper subgroups of index n +1, and no lower (as Galois had also shown), are guaranteed to exist in Gn. Equivalently said,20 a modular equation, of prime level n > 5, is depressible, from degree n + 1 to degree n (and no lower), iff n e {5,7,11}. Via explicitly constructing a permutation representation for the three exceptional groups, embedding them, respectively, in the three alternating groups A5, A7 and A11,21 Galois must, in particular, be solely credited for solving the general quintic via exhibiting it as a modular equation of level 5.

4. AN APPLICATION: SOLVING THE QUINTIC

While Galois' contribution for formulating sufficient and necessary criterion for solubility of an algebraic equation via radicals was brought to light by Liouville, his decisive contribution to actually solving the quintic (before Hermite and Klein did) is, surprisingly, too poorly recognized (if not at all unrecognised!).22 Betti, in 1851 [10], futily asked Liouville not to deprive the public any longer of Galois' (unpublished) results, and, in 1854 [11], went on to show that Galois' construction yields a solution to the quintic via elliptic functions.23 One might associate with each quintic, given in Bring-Jerrard form, a corresponding value for the (Jacobi) elliptic modulus p, as Hermite did, in 1858 [14], implementing this very Galois' construction, which time has come to clarify. The group G5 acts (naturally) on the projective line PZ5, which six elements we shall, following Galois, label as 0,1,2, 3,4 and w. Then collecting them in a triple-pair {(0, w), (1,4), (2,3)}, the group G5 is seen to generate four more triple-pairs {(1, w), (2,0), (3,4)}, {(2, w), (3,1), (4,0)}, {(3, w), (4,2), (0,1)}, {(4,w), (0,3), (1,2)}. Together, the five triple-pairs constitute the five-element set upon which G5 acts.24 Galois did not (in his last letter) write down

groups. We note here that the projective special linear group is simple for all finite, not necessarily prime, fields except the fields Z2 and Z3. Galois, thereby, initiated the classification of finite simple groups, which referred to as "an enormous theorem", was (prematurely) announced in 1981 (by Daniel Gorenstein) before it was completed in 2004 (by Michael Aschbacher and Stephen Smith).

20The equivalence, of statement that follows to the few statements preceding it, was established by Galois.

For n = 5,7,11, the subgroup of index n in Gn turns out to be isomorphic to A4, S4 and A5, respectively. These are precisely the symmetry groups of the platonic solids. The tetrahedron, being self-dual, has A4 as its symmetry group. S4 is the symmetry group for the hexahedron and the octahedron, whereas A5 is the symmetry group for the dodecahedron and the icosahedron.

22Galois' brother Alfred and schoolmate Auguste Chevalier managed to involve Liouville (who was 135 weeks elder to Galois) in disentangling the manuscripts, which they faithfully copied and forwarded to several mathematicians (including Gauss and Jacobi). Liouville acknowledged in September 1843 that he "recognized the entire correctness of the method", which was, subsequently (in 1846), published in the Journal de Mathematiques Pures et Appliquees XI, giving birth to Galois theory. Liouville declared an intention to proceed with publishing the rest of Galois' papers. Yet, most unfortunately, subsequent publication never ensued, and neither Gauss nor Jacobi has ever fulfilled Galois modest request to merely announce the significance (tacitly alleviating the burden of judging the correctness) of his (not necessarily published) contributions. In 1847, Liouville published (instead) his own paper "Lecons sur les fonctions doublement periodiques".

23In 1830, Galois competed with Abel and Jacobi for the grand prize of the French Academy of Sciences. Abel (posthumously) and Jacobi were awarded (jointly) the prize, whereas all references to Galois' work (along with the work itself!) have (mysteriously) disappeared. The very fact that Galois' lost works contained contributions to Abelian integrals is either unknown (to many) or deemed (by some) no longer relevant to our contemporary knowledge. For the sake of being fair to a few exceptional mathematicians, we must cite (without translating to English) Grothendick (as a representative), who (in his autobiographical book Recoltes et Semailles) graciously admits that "Je suis persuade d'ailleurs qu'un Galois serait alle bien plus loin encore que je n'ai ete. D'une part a cause de ses dons tout a fait exceptionnels (que je n'ai pas recus en partage, quant a moi)."

24Indeed, it is the five-element set (not merely a five-element set) which Hermite had no choice but to employ. Galois' construction for each of the two remaining cases, where n = 7 or n = 11, allows an alternative, as will, next, be exhibited.

the four triple-pairs, which we did write after the first, and we now, guided by his conciseness and brevity, confine ourselves to writing down only the first pair-set that he presented for each of the two remaining cases, where n = 7 and n = 11, respectively: {(0, w), (1,3), (2,6), (4,5)} and {(0, w), (1,2), (3,6), (4,8), (5,10), (9,7)}. Unlike the case n = 5, an alternative might be presented for n = 7, which is {(0,w), (1,5), (2,3), (4,6)}, and for n = 11, which is {(0,w), (1,6), (3,7), (4,2), (5,8), (9,10)}. The absolute invariant for the action of the subgroup r2, of the modular group r, consisting of linear fractional transformations congruent to the identity modulo 2, is fi2. A fundamental domain r2\H for the action of r2, might be obtained by subjecting a fundamental domain r\H (of T) to the action of the quotient group T/T2 = S3.25 In particular, fi2 viewed as function on H, is periodic, with period 2. The definition of the modular equation, initially introduced for the invariant j, might be extended to other invariants such as fi2 or fi1/4. Sohnke, in a remarkable work [19], had determined the modular equations for fi1/4, for all odd primes up to, and including, the prime 19. That work, along with Betti's work, inspired Hermite to (successfully) relate a (general) quintic, in Bring-Jerrard form, to a modular equation of level 5, yet he had little choice but to admit the importance of a sole Galois idea (in depressing the degree of the modular equation).26 The modular polynomial for fi1/4, of level 5, is

05(x,y) := x6 - y6 + 5x2y2 (x2 - y2) + 4xy(1 -x4y4),27 (9)

and the period of fi1/4 (as an analytically continued function) is 16. Denoting the roots of 05(x, y = fi1/4(T)), for a fixed t e H, by

1/4 1/4i t + 16 m\ y5 = fi (5t), ym = -fi1/4 -5- , 0 < m < 4,

one calculates the minimal polynomial for x1 := (y5 - y0)(y4 - y1)(y3 - y2) y. It turns out to be

x5 -2000fi2 (1 - fi2)2 x + 1600 >/5fi2 (1 - fi2)2 (1 + fi2).

Thereby, a root of the quintic

5 2(1 + fi2) 2(1 + y8) 28

x5 - x + c, c := -

is

55/Vß(1 -ß2) 55/4y2 yr-y8 V5CXr Xr (y5 - yo)(y4 - yi)(y3 - y2)

4(1 + ß2) 2 \J5 V5ß(1 - ß2) 2y y/5 V5(1 - y8)

25The latter quotient group coincides with G2 which is isomorphic with S3.

26Hermite had apparently adopted Cauchy's catholic and monarchist ideology, much in contrast to Galois' passionate rejection of social prejudice. In 1849, Hermite submitted a memoir to the French Academy of Sciences on doubly periodic functions, crediting Cauchy, but a priority dispute with Liouville prevented its publication. Hermite was then elected to the French Academy of Sciences on July 14,1856, and (likely) acquainted, by Cauchy, with ideas stemming from (but not attributed to) Galois "lost" papers. T. Rothman made a pitiful attempt in "Genius and Biographers: The Fictionalization of Evariste Galois", which appeared in the American Mathematical Monthly, vol. 89, 1982, pp. 84-106 (and, sorrowly, received the Lester R. Ford Writing Award in 1983) to salvage Cauchy's reputation (unknowingly) suggesting further evidence of Cauchy's cowardice, and surprising us, along the way, with many (unusual but ill substantiated and biased) judgements telling us much about T. Rothman himself, but hardly anything trustworthy about anyone else!

27A diligent reader would notice a sign discrepancy in our equation once compared with the equation derived in [19].

28One must note that the constant coefficient c is invariant under the inversions fi ^ -1/fi and fi ^ (1 - fi)/(1 + fi). Here, the composition of the latter two inversions is another inversion. The corresponding four-point orbit in a fundamental domain f2 \H is generated via the mapping t ^ 2/(2 - t) .

and so is expressible via the coefficients Am and jm of the elliptic polynomials rm5(x) =: x2 -Amx + jm, 0 < m < 5. In fact, the polynomials rm5 might be so ordered so that, for each m, the value p2m coincides with y8m. The (general) expression for y8m = p2m, as given in (8), might be rewritten for the special case n = 5 as

8 ^ s(Am, Jm, p) ym = p4S(Am, Jm,1/p)'

where

11 + Ax 2W 12A2 ^ 12 ^ 2 s(A, x) = ^-+ x J |4 A + ^-+ 4 + 5jj x + A^— + 3j x + x j,

and the coefficients Am = jm + (2 • jm) and jm = ym (2 • jm) satisfy

5 62 x10 1 Y\ (x2 - Amx + = x12 +--21 x8 -60x6 -25x4 -10x2 + - +

m=0 5 5

( 92 x2 (x6 a3 x5 + a x3 x8 + 4 x6 - 18 x4--5--7 + a2 x4 -5 - 3 x2 - 2--— = r5(x).

The roots jm and 2 • jm, 0 < m < 5, of the division polynomial r5 might be highly efficiently calculated via the algorithm, provided in [1]. Calculating a pair, say y0 and y5, suffices, of course, for calculating all twelve roots via applying the addition formula (2) along with the doubling formula (3).

Let us conclude with a couple of examples, so let t = 2 i, p = (\/2 -1 . The corresponding quintic is

W2 V2

5

x - x + ■

5/75

The corresponding division polynomial r5(x) factors over Q[ V^] into three quartic polynomial-

factors:

r5(x) = (x4 + 4(3 + V^j x3 + 6^5 + 2 V^jx2 -4^29 + 13 V^jx + 9 + 4 v's]

I (x4 + 4 (3 - V5 j x3 + 6 (5 - 2 V5] x2 - 4 (29 - 13 V5j x + 9 - 4 V5].

I 5 5 5,

Each (quartic) factor is an elliptic polynomial pair product. They are (with their argument omitted) r55r5o, r54r51 and r53r52, respectively. The (corresponding) modular polynomial x, y =

p1/4 = \! V2- 1) factors, over Q[y], into a quadratic and a quartic polynomial-factor:

05 [x, y ) = (x2 + y-2 )(x4 + 4 y3 (1 - y2 x2) x - 2 y4 x2 - y8), and the six roots (of the modular polynomial) might be accordingly expressed and ordered:

V2{2 -v5) - x(-i ) _____/V2(2 + v5) - X(1) 29

y3 = \ -, ,4 = iv v2 + 1, y5 = ,,

,3 v x(i) ' v 'V x(-1)

29The image of the square root is assumed, here (but not necessarily earlier!), to be unambigiously taken in the right half-plane, including the boundary of the upper quadrant but excluding it for the lower quadrant.

where _

X(e):= 3 + 2 ]fV5e.

Exploiting the identities

fi = (-1]2 = (vT0 - 3)( - 2)(3 + - 2j,

1(1) l(-1) = ( V5 - 2)2 = (3 ^2 + V5 + 2)(3 ^2 - V5 - 2).

x(i) x(-i) = (V5+2)2 = (3 + -2) (3 - +2), along with the alternative expressions

= _ V-(i + 1)x(i) + V(i - 1)x(-i) = V(i - 1)x(i) + V-(i + 1)x(-i) i)

y2 = , . ==-, , :, y3 =

V(1 + i)x(1) - V(1 - i)x(-1)' V(1 - i)x(1) - V(1 + i)x(-1)'

one finds out that

xi = -8 \/5 fi,

and, so, a root of our quintic is

-8 fi -2

2^/5 v5 ß(1 - ß2) vV10

Along the way, we might calculate the (five) discriminants

d 2(fi2) = d 2(fi1) = d 2(fi2) = 32, 2 2 32 x(-1) 2 2 32 x(i) 2 2 32 x(-i) 2 2 32 x(1)

d2(fi2) = . , d2(fi2) = ', d2(fi3) = c , d2(fi5) = ', W x(1) ^ x(-i )5 3 x(i )5 5 x(-1)

observing that they are sixth powers of the respective values

25/6 V5 - 1 V5 + 1 V5 + 1 V5 - 1

21/6x(1) 21/6x(-i) 21/6x(i) 21/6x(-1) and, so using equation (5), we might calculate five special values of the modular invariant:

j (T) = j0 = (^ + 2)20 x(-1)6 (238 Vs - 60 - ^) , j(2 i) = j1 = j4 = (11) , ( 5 i -1) . ( ^ ^20 ( ^ . 861)3

j f5^-1) = j2 = - ( - 2)20 x(i )6 (238 - 60 yfv5 i +

j (5i4+1 j = j3 = - ( - 2)20 x(-i)6 (238 + 60 i + 821 )

20 ( / 861 j3

j (10 i) = j5 = ( v5+2 x(1)6 238 ^+6^ v5- — .30

0These special values might be expressed as cubes if one notes that \/5 ± 2 = (v/5 ± 1) /8.

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We might now let t = i, p = 72, and observe that the modular polynomial 05lx, y = p1/4 =

/772 )

factors, over Q[y], into a quadratic and a quartic polynomial-factor:

05

x, y =

/72

= (x2 - y5x + y2) (x4 - 3 y5x3 - 2 y2x2 + y7x - y4),

before confirming that the roots of the latter quartic polynomial-factor

7s +1

y

(e /75

1

, e = {1,-i, i, -1},

are, respectively, obtainable as fourth roots of the values

72 (e2 75 + 2) X(-e) '

which, in turn, are (as they ought to be) the images of the four afore-calculated values p0, p2, p3 and p5 (where p was 3 - 2 72) if subjected to the (fourth order) linear fractional transformation

1 + Pm 1 - Pm

-, m e {0,2, 3, 5}.

The four corresponding values of the discriminants are

d 2

'2 (e2 n/5 + 2) X-)2

x(e)5 = 32 f x(e)

2 x(-e)

\/5-<

Two more special values of the modular invariant are calculated by (reapplying) formula (5) to a discriminant from, firstly, the complex-conjugate (e = ±i) pair, and, secondly, the real-valued (e = ±1) pair:

J

5i 1

'2927 -1323 75

2

, J (5 i) =

'2927 + 1323 75

2

One might infer, from equation (8), that the modular polynomial, of level 2, ®2 (x, z) vanishes at

)3 ( .

4

(x, zi ) = — 27

(d2 + 1)3 (d2 + 13

where

d2

1d

di2

, l e {0,1,2},

(dg, df, d|) = 16 -2, P3 d , d = d (P) = p - -

d 2' p

P

For x e {j0, j2, j3, j5} we have already calculated the (two) corresponding values z0. Concluding, we calculate the corresponding values z1 and z2, so put

W(S,e) := ^ + 1 [57272 - 340116 72 + 4 f101 - 5463 6 72)e2 75 + ^ 8 x(e)6 v V J

-18 ^800 + 111 â 72 + 4 (100 + 27â 72) e2 75) e \Zt5 j

6

2

3

3

[e V5 + ^ (1190448488 - 858585699 S + 540309076e2 - 374537880S e2 VT0 + 239 i

- e \j~V5 (693172512 - 595746414 S + 407357424e2 - 240819696S e2 VT0) j, and observe that

4 (28/3d(fim)2/3 fim )3 3

Z1( jm) = --24/3d (fim H = V(-1, e),

4 ( 1 )3

z2(jm) = — 28/3fiid(fim)2/3 + —-— = w(1,e)3,

2KJ m 27^ im im 24/3fimd(fim)1/3j V

where e e {1, -i, i, -1} correspond, respectively, to m e {0, 2, 3, 5}, as before, and verify that

(5i) 3 (20i+5) 3

j [yj = Z1(j0) = ^(-1,1)3, j J = Z1(j2) = ^(-1,-i)3,

20 i - 5) 3 3

—= Z1(73) = ^(-1, i)3, j (20 i) = Z1(75) = ^(-1, -1)3,

5 i + 2) 3 (20 i + 4 ) 3

—^J = Z2(j0) = ^(1,1)3, j^^^J = z2(j2) = ^(1,-i)3,

i 20 i-4) 3 (10 i + 1) 3

j J = z2(j3) = ^(1, i)3, j J = Z2(j5) = ^(1, -1)3.

Few of these special values were first presented in [5].

5. CONCLUSION

Nowadays, oblivion has entirely replaced marvelling at Galois key step, towards solving the quintic, in depressing the degree of the modular equation, of level 5, from 6 to 5,31 and Galois is merely mentioned, along with Abel, for determining that the quintic is not generally solvable via radicals. With this paper, we hope that this (crippled) view of Galois (deeply constructive and far from fully appreciated) theory would finally come to an end. A recent exapmle concerns an expression, for "the speed of precession" of a freely moving triaxial rigid body, which attainment relied on identifying the function field where such a general expression would lie, based on exploring its symmetries [7]. Only a (minor) consequence of such Galois guided algebraic approach, was identifying a Galois axis fixed within a triaxial rigid body and distinct from any of its three main axes of inertia. Marvelously, Galois axis rotates uniformly during the critical motion (whether or not such motion is said to be either stable or unstable and whether or not the body "flips"), as shown in [8].

31For example, S. Vladuj (wrongfully) attributes, in his book "Kronecker's Jugendtraum and Modular Functions" (published by Gordon and Breach in 1991), to Hermite showing the equivalence of the general quintic to the modular equation of level 5.

Agnai/i C. <t>.

References

1. S. F. Adlaj, "Iteratsionnyi algoritm vychisleniya ellipticheskogo integrala" [Iterative elliptic integral algorithm], Zadachi issledovaniya ustoichivosti i stabilizatsii dvizheniya, pp. 104-110, 2011, [Online]. Available: http://www.ccas.ru/depart/mechanics/TUMUS/z_SBORNIKI/issues/2011_4Adlaj.pdf (in Russian).

2. S. Adlaj, "Eighth lattice points," arXiv:1110.1743 [math.GM], Oct. 2011.

3. S. Adlaj, "An inverse of the modular invariant," arXiv:1110.3274 [math.GM], Oct. 2011.

4. S. Adlaj, "Mechanical interpretation of negative and imaginary tension of a tether in a linear parallel force field," in Selected works of International Scientific Conference on Mechanics "Sixth Polyakhov Readings," St. Petersburg, Russia, Jan. 31-Feb. 3, 2012, pp. 13-18.

5. S. Adlaj, "Torsion points on elliptic curves and modular polynomial symmetries," presented on at the Joined MSU-CCRAS Computer Algebra Seminar, Moscow, Russia, Sep. 24, 2014 [Online]. Available: http: //www.ccas.ru/sabramov/seminar/lib/exe/fetch.php?media=adlaj140924.pdf.

6. S. Adlaj, "An analytic unifying formula of oscillatory and rotary motion of a simple pendulum," in Special edition dedicated to the 70th birthday of J. J. Slawianowski, Sofia, Bulgaria: Avangard Prima, 2015, pp. 160-171.

7. S. Adlaj, "Dzhanibekov's flipping nut and Feynman's wobbling plate," in Polynomial Computer Algebra International Conference, St. Petersburg, Russia, Apr. 18-23 2016, pp. 10-14 [Online]. Available at http: //pca.pdmi.ras.ru/2016/abstracts_files/PCA2016SA.pdf.

8. S. F. Adlaj, S. A. Berestova, N. E. Misyura, and E. A. Mityushov "Illustrations of rigid body motion along a separatrix in the case of Euler-Poinsot," Computer tools in education, no. 2, 2018, pp. 5-13; doi:10.32603/2071-2340-2-5-13.

9. S. F. Adlaj, Ravnovesie niti v lineinom parallel'nom pole sil: Klassifikatsiya i issledovanie ustoichivosti ravnovesnykh form niti v lineinom parallel'nom pole sil [Thread balance in a linear parallel field of forces: Classification and study of the stability of the equilibrium forms of a thread in a linear parallel field of forces], LAMBERT Academic Publishing, 2018.

10. E. Betti, "Sopra la risolubilità per radicali delle equazioni algebriche irriduttibili di grado primo," DagliAnnali di Scienze matimatiche e fisiche, II (Roma, 1851), pp. 5-19.

11. E. Betti, "Un teorema sulla risoluzione analitica delle equazioni algebriche," Dagli Annali di Scienze matimatiche e fisiche, V (Roma, 1854), pp. 10-17.

12. D. Cox, "The arithmetic-geometric mean of Gauss," L'Enseignement Mathématique, vol. 30,1984, pp. 275-330; doi:10.1007/978-3-319-32377-0_3.

13. É. Galois, "Lettre de Galois a M. Auguste Chevalier," Journal de Mathématiques Pures et Appliquees XI, 1846, pp. 408-415.

14. C. Hermite, "Sur la resolution de l'equation du cinquieme degrÉ," Comptes Rendus de l'Académie des Sciences,, XLVI (I), 1858, pp. 508-515.

15. M. B. Kiernan, "The development of Galois theory from Lagrange to Artin. Communicated by M. Kline," Arch. Rational Mech., vol. 8, no 1-2, 1971; doi:10.1007/BF00327219.

16. H. Ruhland, "The Inverse of the Modular Invariant," [Online]. Available: http://www.ccas.ru/depart/ mechanics/TUMUS/Adlaj/TheInverse.pdf.

17. J-P. Serre, A Course in Arithmetic, New York: Springer-Verlag, 1973.

18. G. Shimura, Introduction to the Arithmetic Theory of Automorphic Functions, Princeton, NJ: Princeton University Press, 1981.

19. L. A. Sohnke, "Aequationes modulares pro transformatione Functionum Ellipticarum," Journal fur die reine und angewandte Mathematik, vol. 16,1837, pp. 97-130, [Online]. Available: http://eudml.org/doc/ 146989

Received 19.06.2018, the final version — 26.07.2018.

Компьютерные инструменты в образовании, 2018

№ 4:11-26

УДК: 511.238

http://ipo.spb.ru/journal

doi:10.32603/2071-2340-4-11-26

О ВТОРОМ МЕМУАРЕ ПОСЛЕДНЕГО ПИСЬМА ЭВАРИСТА ГАЛУА

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Адлай С. Ф.

Федеральный научно-исследовательский центр «Информатика и управление» Российской академии наук, Москва, Россия

Аннотация

Последнее письмо Эвариста Галуа, адресованное Огюсту Шевалье, накануне (так называемой) дуэли 30 мая 1832 года (которая, пожалуй, проще и точнее быта охарактеризована как убийство Альфредом, не допустившим на следующий день священника к своему старшему брату Эваристу в его последние мгновения), было написано на семи страницах и разделено на три мемуара. Первый мемуар занимает чуть меньше двух страниц. Впоследствии сей мемуар стал известен как теория Галуа (о которой, в частности, рассказал Мелвин Кирнан). Однако, Галуа продолжил своё письмо потрясающе удивительными конструкциями во втором мемуаре, который занял чуть более двух страниц. Третий (и самый длинный!) мемуар начинается на пятой странице и остаётся загадочным и нерасшифрованным, но он, несомненно, вдохновил Александра Гротендика сформулировать свою гипотезу о периодах. Письмо заканчивается абзацем о последних «главных размышлениях», касающихся «приложений теории неоднозначности к трансцендентному анализу», где Галуа преподносит нам последнюю загадку, говоря, что «мы можем тотчас же рассмотреть большое множество выражений». К сожалению, неумолимость давлеющего времени не позволила ему привести какие-либо конкретные примеры, а смогла лишь дать краткие последние инструкции, о том, что делать с письмом. Несмотря на это, многие «историки» назойливо и примитивно твердят нам (и друг другу), что мы не должны «переоценивать» значение письма, которое (вопреки их советам) красноречиво и правдиво описывалось Германом Вейлем как «самая значимая рукопись во всей истории человечества »!

Ключевые слова: эссенциальная эллиптическая функция, понижение степени модулярного уравнения, проективная специальная линейная группа над простым полем, эллиптические и коэллиптические полиномы, решение общего квинтического уравнения.

Цитирование: Adlaj S. F. On the Second Memoir of Evariste Galois' Last Letter // Компьютерные инструменты в образовании. 2018. № 4. С. 11-26. doi:10.32603/2071-2340-4-11-26

Поступила в редакцию 19.06.2018, окончательный вариант — 26.07.2018.

Адлай Семён Франкович, научный сотрудник, Сектор теории устойчивости и механики управляемых систем, Отделение моделирования сложных физических и технических систем, Вычислительный центр

им А. А. Дородницына ФИЦ ИУ РАН; 119333, Россия, Москва, ул. Вавилова, д. 40, [email protected]

© Our authors, 2018. Наши авторы, 2018.

Semjon F. Adlaj,

Scientific Researcher, Section of Stability Theory and Mechanics of Controlled Systems, Division of Complex Physical and Technical Systems Modeling, Computing Center of the Federal Research Center "Informatics and Control", Russian Academy of Sciences; 119333, Russia, Moscow, Vavilov Street 40, [email protected]

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