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Debrecen University Symposium Gy˝ory 75 July 10-11, 2015 E↵ective upper bounds for the solutions of a family of Thue equations involving powers of units of the simplest cubic fields.

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July 11, 2015

Debrecen University Symposium Gy˝ory 75

July 10-11, 2015

E↵ective upper bounds for the solutions of a family of Thue equations involving powers of units of the simplest cubic fields.

Michel Waldschmidt Joint work with Claude Levesque.

The pdf file of this talk can be downloaded at URL http://www.imj-prg.fr/~michel.waldschmidt/

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Boldog sz¨ulet´esnapot, K´alm´an !

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Abstract

Emery Thomaswas one of the first to solve an infinite family of Thueequations, when he considered the forms

Fn(X,Y) =X3 (n 1)X2Y (n+ 2)XY2 Y3 and the family of equations Fn(x,y) = ±1,n 2N, x,y 2Z.

This family is associated to the family of the simplest cubic fieldsQ( )of D. Shanks, being a root of Fn(X,1).

We introduce in this family a second parameter by replacing the roots of the minimal polynomial Fn(X,1)of by the a-th powers of the roots and we e↵ectively solve the family ofThue equations that we obtain and which depends now on the two parametersn and a.

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Thue equation

Thue (1908) : there are only finitely many integer solutions of F(x,y) =m,

whenF is homogeneous irreducible form over Qof degree 3.

Baker – Fel’dmanE↵ective upper bounds for the solutions.

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Thue equation

Thue (1908) : there are only finitely many integer solutions of F(x,y) =m,

whenF is homogeneous irreducible form over Qof degree 3.

Baker – Fel’dmanE↵ective upper bounds for the solutions.

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Gel’fond–Baker method

WhileThue’s method was based on the non e↵ective

Thue–Siegel–Roth Theorem,Baker and Fel’dmanfollowed an e↵ective method introduced byA.O. Gel’fond, involving lower bounds for linear combinations of logarithms of algebraic numbers with algebraic coefficients.

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Lower bounds for linear combinations of logarithms

A lower bound for a nonvanishing di↵erence

b11· · ·bnn 1

is essentially the same as a lower bound for a nonvanishing number of the form

b1log1+· · ·+bnlogn, since ez 1z forz !0.

The first nontrivial lower bounds were obtained by

A.O. Gel’fond. His estimates were e↵ective only for n= 2 : for n 3, he needed to use estimates related to the

Thue–Siegel–Roth Theorem.

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Explicit version of Gel’fond’s estimates

A. Schinzel(1968) computed explicitly the constants introduced byA.O. Gel’fond.

in his lower bound for

b112b2 1 .

He deduced explicit Diophantine results using the approach introduced byA.O. Gel’fond.

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Alan Baker

In 1968,A. Baker succeeded to extend to any n 2 the transcendence method used byA.O. Gel’fond forn = 2.

As a consequence, e↵ective upper bounds for the solutions of Thue’s equations have been derived.

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Thue equations and the Siegel unit equation

The main idea behind theGel’fond–Baker approach for solving Thueequations is to exploit Siegel’s unit equation.

Assume1,2,3 are algebraic integers and x, y rational integers such that

(x 1y)(x 2y)(x 3y) = 1.

Then the three numbers

u1 =x 1y, u2 =x 2y, u3 =x 3y, are units. Eliminatingx and y, one deduces Siegel’s unit equation

u1(↵2 3) +u2(↵3 1) +u3(↵1 2) = 0.

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Thue equations and the Siegel unit equation

The main idea behind theGel’fond–Baker approach for solving Thueequations is to exploit Siegel’s unit equation.

Assume1,2,3 are algebraic integers and x, y rational integers such that

(x 1y)(x 2y)(x 3y) = 1.

Then the three numbers

u1 =x 1y, u2 =x 2y, u3 =x 3y, are units.Eliminating x and y, one deduces Siegel’s unit equation

u1(↵2 3) +u2(↵3 1) +u3(↵1 2) = 0.

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Thue equations and the Siegel unit equation

The main idea behind theGel’fond–Baker approach for solving Thueequations is to exploit Siegel’s unit equation.

Assume1,2,3 are algebraic integers and x, y rational integers such that

(x 1y)(x 2y)(x 3y) = 1.

Then the three numbers

u1 =x 1y, u2 =x 2y, u3 =x 3y, are units. Eliminatingx and y, one deduces Siegel’s unit equation

u1(↵2 3) +u2(↵3 1) +u3(↵1 2) = 0.

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Siegel’s unit equation

Write Siegel’s unit equation

u1(↵2 3) +u2(↵3 1) +u3(↵1 2) = 0 in the form

u1(↵2 3)

u2(↵1 3) 1 = u3(↵1 2) u2(↵1 3)· The quotient

u1(↵2 3) u2(↵1 3) is the quantity

b11· · ·bnn in Gel’fond–Baker Diophantine inequality.

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Siegel’s unit equation

Write Siegel’s unit equation

u1(↵2 3) +u2(↵3 1) +u3(↵1 2) = 0 in the form

u1(↵2 3)

u2(↵1 3) 1 = u3(↵1 2) u2(↵1 3)· The quotient

u1(↵2 3) u2(↵1 3) is the quantity

b11· · ·bnn in Gel’fond–Baker Diophantine inequality.

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Work on Baker’s method :

A. Baker (1968),N.I. Fel’dman (1971), V.G. Sprind˘zuk and H.M. Stark(1973), K. Gy˝ory and Z.Z. Papp (1983),

E. Bombieri(1993),Y. Bugeaud and K. Gy˝ory (1996), Y. Bugeaud(1998). . .

SolvingThue equations :

A. Peth˝oand R. Schulenberg(1987), B. de Weger (1987), N. Tzanakisand B. de Weger (1989),Y. Bilu and G. Hanrot (1996), (1999). . .

SolvingThue–Mahler equations :

J.H. Coates (1969),S.V. Kotov and V.G. Sprind˘zuk (1973), A. B´erczes–Yu Kunrui– K. Gy˝ory (2006). . .

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Work on Baker’s method :

A. Baker (1968),N.I. Fel’dman (1971), V.G. Sprind˘zuk and H.M. Stark(1973), K. Gy˝ory and Z.Z. Papp (1983),

E. Bombieri(1993),Y. Bugeaud and K. Gy˝ory (1996), Y. Bugeaud(1998). . .

SolvingThue equations :

A. Peth˝oand R. Schulenberg(1987), B. de Weger (1987), N. Tzanakisand B. de Weger (1989),Y. Bilu and G. Hanrot (1996), (1999). . .

SolvingThue–Mahler equations :

J.H. Coates (1969),S.V. Kotov and V.G. Sprind˘zuk (1973), A. B´erczes–Yu Kunrui– K. Gy˝ory (2006). . .

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Work on Baker’s method :

A. Baker (1968),N.I. Fel’dman (1971), V.G. Sprind˘zuk and H.M. Stark(1973), K. Gy˝ory and Z.Z. Papp (1983),

E. Bombieri(1993),Y. Bugeaud and K. Gy˝ory (1996), Y. Bugeaud(1998). . .

SolvingThue equations :

A. Peth˝oand R. Schulenberg(1987), B. de Weger (1987), N. Tzanakisand B. de Weger (1989),Y. Bilu and G. Hanrot (1996), (1999). . .

SolvingThue–Mahler equations :

J.H. Coates (1969),S.V. Kotov and V.G. Sprind˘zuk (1973), A. B´erczes–Yu Kunrui– K. Gy˝ory (2006). . .

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Diophantine equations

A.O. Gel’fond, A. Baker, V. Sprind˘zuk, R. Tijdeman, C.L. Stewart, M. Mignotte, M. Bennett, P. Voutier, Y. Bugeaud, T.N. Shorey. . .

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Mathematical genealogy of K´alm´an Gy˝ory

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K´alm´an Gy˝ory and his School

K. Gy˝ory A. Peth˝o I. Ga´al,

A. Pint´er´ L. Hajdu A. B´erczes

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Families of Thue equations

The first families of Thue equations having only trivial solutions were introduced byA. Thue himself.

(a+ 1)Xn aYn = 1.

He proved that the only solution in positive integers x,y is x =y = 1 for n prime anda sufficiently large in terms of n.

Forn= 3 this equation has only this solution fora 386.

M. Bennett(2001) proved that this is true for all a and n with n 3and a 1.

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Families of Thue equations

The first families of Thue equations having only trivial solutions were introduced byA. Thue himself.

(a+ 1)Xn aYn = 1.

He proved that the only solution in positive integers x,y is x =y = 1 for n prime anda sufficiently large in terms of n.

Forn= 3 this equation has only this solution fora 386.

M. Bennett(2001) proved that this is true for all a and n with n 3and a 1.

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E. Thomas’s family of Thue equations

E. Thomasin 1990 studied the families ofThueequations

x3 (n 1)x2y (n+ 2)xy2 y3 = 1 Set

Fn(X,Y) = X3 (n 1)X2Y (n+ 2)XY2 Y3. The cubic fields Q( ) generated by a root of Fn(X,1)are called byD. Shanks the simplest cubic fields. The roots of the polynomialFn(X,1) can be described via homographies of degree 3.

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D. Shanks’s simplest cubic fields Q( ).

Let be one of the three roots of

Fn(X,1) =X3 (n 1)X2 (n+ 2)X 1.

ThenQ( ) is a Galois cubic field.

Write

Fn(X,Y) = (X 0Y)(X 1Y)(X 2Y) with

0 >0> 1 > 1> 2. Then

1 = 1

0+ 1 and 2 = 0+ 1

0 ·

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D. Shanks’s simplest cubic fields Q( ).

Let be one of the three roots of

Fn(X,1) =X3 (n 1)X2 (n+ 2)X 1.

ThenQ( ) is a Galois cubic field.

Write

Fn(X,Y) = (X 0Y)(X 1Y)(X 2Y) with

0 >0> 1 > 1> 2. Then

1 = 1

0+ 1 and 2 = 0+ 1

0 ·

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Simplest fields.

When the following polynomials are irreducible fors,t 2Z, the fieldsQ(!) generated by a root! of respectively 8>

<

>:

sX3 tX2 (t + 3s)X s, sX4 tX3 6sX2+tX +s,

sX6 2tX5 (5t + 15s)X4 20sX3+ 5tX2+ (2t+ 6s)X +s, are cyclic overQ of degree 3, 4and 6respectively.

Fors = 1, they are calledsimplest fields by many authors.

Fors 1, I. Wakabayashi call them simplest fields.

In each of the three cases, the roots of the polynomials can be described via homographies of PSL2(Z) of degree 3,4 and 6 respectively.

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Simplest fields.

When the following polynomials are irreducible fors,t 2Z, the fieldsQ(!) generated by a root! of respectively 8>

<

>:

sX3 tX2 (t + 3s)X s, sX4 tX3 6sX2+tX +s,

sX6 2tX5 (5t + 15s)X4 20sX3+ 5tX2+ (2t+ 6s)X +s, are cyclic overQ of degree 3, 4and 6respectively.

Fors = 1, they are calledsimplest fields by many authors.

Fors 1, I. Wakabayashi call them simplest fields.

In each of the three cases, the roots of the polynomials can be described via homographies of PSL2(Z) of degree 3,4 and 6 respectively.

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E. Thomas’s family of Thue equations

In 1990,E. Thomas proved in some e↵ective way that the set of (n,x,y)2Z3 with

n 0, max{|x|,|y|} 2 and Fn(x,y) = ±1 is finite.

In his paper, he completely solved the equationFn(x,y) = 1 forn 1.365·107 : the only solutions are(0, 1), (1,0)and ( 1,+1).

SinceFn( x, y) = Fn(x,y), the solutions to Fn(x,y) = 1are given by( x, y) where(x,y) are the solutions toFn(x,y) = 1.

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E. Thomas’s family of Thue equations

In 1990,E. Thomas proved in some e↵ective way that the set of (n,x,y)2Z3 with

n 0, max{|x|,|y|} 2 and Fn(x,y) = ±1 is finite.

In his paper, he completely solved the equationFn(x,y) = 1 forn 1.365·107 : the only solutions are(0, 1), (1,0)and ( 1,+1).

SinceFn( x, y) = Fn(x,y), the solutions to Fn(x,y) = 1are given by( x, y) where(x,y) are the solutions toFn(x,y) = 1.

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E. Thomas’s family of Thue equations

In 1990,E. Thomas proved in some e↵ective way that the set of (n,x,y)2Z3 with

n 0, max{|x|,|y|} 2 and Fn(x,y) = ±1 is finite.

In his paper, he completely solved the equationFn(x,y) = 1 forn 1.365·107 : the only solutions are(0, 1), (1,0)and ( 1,+1).

SinceFn( x, y) = Fn(x,y), the solutions to Fn(x,y) = 1are given by( x, y) where(x,y) are the solutions toFn(x,y) = 1.

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Exotic solutions found by E. Thomas in 1990

F0(X,Y) =X3 +X2Y 2XY2 Y3 Solutions(x,y) to F0(x,y) = 1 :

( 9,5), ( 1,2),(2, 1), (4, 9), (5,4)

F1(X,Y) =X3 3XY2 Y3

Solutions(x,y) to F1(x,y) = 1 : ( 3,2), (1, 3),(2,1)

F3(X,Y) =X3 2X2Y 5XY2 Y3 Solutions(x,y) to F3(x,y) = 1 :

( 7, 2),( 2,9), (9, 7)

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Exotic solutions found by E. Thomas in 1990

F0(X,Y) =X3 +X2Y 2XY2 Y3 Solutions(x,y) to F0(x,y) = 1 :

( 9,5), ( 1,2),(2, 1), (4, 9), (5,4)

F1(X,Y) =X3 3XY2 Y3

Solutions(x,y) to F1(x,y) = 1 : ( 3,2), (1, 3),(2,1)

F3(X,Y) =X3 2X2Y 5XY2 Y3 Solutions(x,y) to F3(x,y) = 1 :

( 7, 2),( 2,9), (9, 7)

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Exotic solutions found by E. Thomas in 1990

F0(X,Y) =X3 +X2Y 2XY2 Y3 Solutions(x,y) to F0(x,y) = 1 :

( 9,5), ( 1,2),(2, 1), (4, 9), (5,4)

F1(X,Y) =X3 3XY2 Y3

Solutions(x,y) to F1(x,y) = 1 : ( 3,2), (1, 3),(2,1)

F3(X,Y) =X3 2X2Y 5XY2 Y3 Solutions(x,y) to F3(x,y) = 1 :

( 7, 2),( 2,9), (9, 7)

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M. Mignotte’s work on E. Thomas’s family

In 1993,M. Mignotte completed the work of E. Thomas by solving the problem for eachn.

Forn 4 and for n= 2, the only solutions to Fn(x,y) = 1 are(0, 1), (1,0) and

( 1,+1), while for the cases n= 0,1,3, the only nontrivial solutions are the ones found byE. Thomas.

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M. Mignotte’s work on E. Thomas’s family

In 1993,M. Mignotte completed the work of E. Thomas by solving the problem for eachn.

Forn 4 and for n= 2, the only solutions to Fn(x,y) = 1 are(0, 1), (1,0) and

( 1,+1), while for the cases n= 0,1,3, the only nontrivial solutions are the ones found byE. Thomas.

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E. Thomas’s family of Thue equations

For the same family

Fn(X,Y) = X3 (n 1)X2Y (n+ 2)XY2 Y3, givenm6= 0, M. Mignotte, A. Peth˝o and F. Lemmermeyer (1996) studied the family of Diophantine equations

Fn(X,Y) = m.

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M. Mignotte, A. Peth˝o and F. Lemmermeyer (1996)

Forn 2, when x,y are rational integers verifying 0<|Fn(x,y)|m,

then

log|y|c(logn)(logn+ logm) with an e↵ectively computable absolute constant c.

One would like an upper bound formax{|x|,|y|} depending only onm, not on n. This is still open.

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M. Mignotte, A. Peth˝o and F. Lemmermeyer (1996)

Forn 2, when x,y are rational integers verifying 0<|Fn(x,y)|m,

then

log|y|c(logn)(logn+ logm) with an e↵ectively computable absolute constant c.

One would like an upper bound formax{|x|,|y|} depending only onm, not on n. This is still open.

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M. Mignotte, A. Peth˝o and F. Lemmermeyer

Besides,M. Mignotte, A. Peth˝o and F. Lemmermeyer found all solutions of the Thueinequality |Fn(X,Y)|2n+ 1.

As a consequence, when m is a given positive integer, there exists an integern0 depending upon m such that the inequality

|Fn(x,y)|m, with n 0and |y|>p3

m, impliesn n0.

Note that for0<|t|p3

m,( t,t) and(t, t)are solutions.

Therefore, the condition|y|>p3

m cannot be omitted.

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M. Mignotte, A. Peth˝o and F. Lemmermeyer

Besides,M. Mignotte, A. Peth˝o and F. Lemmermeyer found all solutions of the Thueinequality |Fn(X,Y)|2n+ 1.

As a consequence, when m is a given positive integer, there exists an integern0 depending upon m such that the inequality

|Fn(x,y)|m, with n 0and |y|>p3

m, impliesn n0.

Note that for0<|t|p3

m,( t,t) and(t, t)are solutions.

Therefore, the condition|y|>p3

m cannot be omitted.

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M. Mignotte, A. Peth˝o and F. Lemmermeyer

Besides,M. Mignotte, A. Peth˝o and F. Lemmermeyer found all solutions of the Thueinequality |Fn(X,Y)|2n+ 1.

As a consequence, when m is a given positive integer, there exists an integern0 depending upon m such that the inequality

|Fn(x,y)|m, with n 0and |y|>p3

m, impliesn n0.

Note that for0<|t|p3

m,( t,t) and(t, t)are solutions.

Therefore, the condition|y|>p3

m cannot be omitted.

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E. Thomas’s family of Thue inequations

In 1996, for the family ofThue inequations 0<|Fn(x,y)|m,

Chen Jian Hua has given a bound forn by using Pad´e’s approximations. This bound was highly improved in 1999 by G. Lettl, A. Peth˝o and P. Voutier.

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Homogeneous variant of E. Thomas’s family

I. Wakabayashi, using again the approximants ofPad´e, extended these results to the families of forms, depending upon two parameters,

sX3 tX2Y (t + 3s)XY2 sY3,

which includes the family of Thomas for s = 1 (with t =n 1).

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May 2010, Rio de Janeiro What were we doing on the beach of Rio ?

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Suggestion of Claude Levesque

ConsiderThomas’s family of cubic Thueequations Fn(X,Y) = ±1with

Fn(X,Y) = X3 (n 1)X2Y (n+ 2)XY2 Y3. Write

Fn(X,Y) = (X 0nY)(X 1nY)(X 2nY)

where in are units in the totally real cubic field Q( 0n). Twist these equations by introducing a new parameter a2Z :

Fn,a(X,Y) = (X a0nY)(X a1nY)(X a2nY)2Z[X,Y].

Then we get a family of cubic Thueequations depending on two parameters(n,a) :

Fn,a(x,y) =±1.

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Suggestion of Claude Levesque

ConsiderThomas’s family of cubic Thueequations Fn(X,Y) = ±1with

Fn(X,Y) = X3 (n 1)X2Y (n+ 2)XY2 Y3. Write

Fn(X,Y) = (X 0nY)(X 1nY)(X 2nY)

where in are units in the totally real cubic field Q( 0n). Twist these equations by introducing a new parameter a2Z :

Fn,a(X,Y) = (X a0nY)(X a1nY)(X a2nY)2Z[X,Y].

Then we get a family of cubic Thueequations depending on two parameters(n,a) :

Fn,a(x,y) =±1.

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Suggestion of Claude Levesque

ConsiderThomas’s family of cubic Thueequations Fn(X,Y) = ±1with

Fn(X,Y) = X3 (n 1)X2Y (n+ 2)XY2 Y3. Write

Fn(X,Y) = (X 0nY)(X 1nY)(X 2nY)

where in are units in the totally real cubic field Q( 0n). Twist these equations by introducing a new parameter a2Z :

Fn,a(X,Y) = (X a0nY)(X a1nY)(X a2nY)2Z[X,Y].

Then we get a family of cubic Thueequations depending on two parameters(n,a) :

Fn,a(x,y) =±1.

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Suggestion of Claude Levesque

ConsiderThomas’s family of cubic Thueequations Fn(X,Y) = ±1with

Fn(X,Y) = X3 (n 1)X2Y (n+ 2)XY2 Y3. Write

Fn(X,Y) = (X 0nY)(X 1nY)(X 2nY)

where in are units in the totally real cubic field Q( 0n). Twist these equations by introducing a new parameter a2Z :

Fn,a(X,Y) = (X a0nY)(X a1nY)(X a2nY)2Z[X,Y].

Then we get a family of cubic Thueequations depending on two parameters(n,a) :

Fn,a(x,y) =±1.

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Thomas’s family with two parameters

Joint work withClaude Levesque

Main result (2014) : there is an e↵ectively computable absolute constantc >0such that, if (x,y,n,a) are nonzero rational integers withmax{|x|,|y|} 2and

Fn,a(x,y) =±1, then

max{|n|,|a|,|x|,|y|}c.

For all n 0, trivial solutions witha 2: (±1,0),(0,±1)

(±1,±1)for a = 2

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Thomas’s family with two parameters

Joint work withClaude Levesque

Main result (2014) : there is an e↵ectively computable absolute constantc >0such that, if (x,y,n,a) are nonzero rational integers withmax{|x|,|y|} 2and

Fn,a(x,y) =±1, then

max{|n|,|a|,|x|,|y|}c.

For all n 0, trivial solutions witha 2: (±1,0),(0,±1)

(±1,±1)for a = 2

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Exotic solutions to Fn,a(x,y) = 1 with a 2

(n,a) (x,y)

(0,2) ( 14, 9) ( 3, 1) ( 2, 1) (1,5) (3,2) (13,4) (0,3) (2,1)

(0,5) ( 3, 1) (19, 1)

(1,2) ( 7, 2) ( 3, 1) (2,1) (7,3) (2,2) ( 7, 1) ( 2, 1)

(4,2) (3,2)

No further solution in the range

0n 10, 2a 70, 1000x,y 1000.

Open question : are there further solutions ?

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Exotic solutions to Fn,a(x,y) = 1 with a 2

(n,a) (x,y)

(0,2) ( 14, 9) ( 3, 1) ( 2, 1) (1,5) (3,2) (13,4) (0,3) (2,1)

(0,5) ( 3, 1) (19, 1)

(1,2) ( 7, 2) ( 3, 1) (2,1) (7,3) (2,2) ( 7, 1) ( 2, 1)

(4,2) (3,2)

No further solution in the range

0n 10, 2a 70, 1000x,y 1000.

Open question : are there further solutions ?

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Computer search by specialists

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Further Diophantine results on the family Fn,a(x,y)

Letm 1. There exists an absolute e↵ectively computable constant such that, if there exists (n,a,m,x,y)2Z5 with a6= 0 verifying

0<|Fn,a(x,y)|m, then

log max{|x|,|y|}µ with

µ=

( (logm+|a|log|n|)(log|n|)2log log|n| for |n| 3,

logm+|a| for n= 0,±1,±2.

Fora= 1, this follows from the above mentioned result of M. Mignotte,A. Peth˝oandF. Lemmermeyer.

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Further Diophantine results on the family Fn,a(x,y)

Letm 1. There exists an absolute e↵ectively computable constant such that, if there exists (n,a,m,x,y)2Z5 with a6= 0 verifying

0<|Fn,a(x,y)|m, then

log max{|x|,|y|}µ with

µ=

( (logm+|a|log|n|)(log|n|)2log log|n| for |n| 3,

logm+|a| for n= 0,±1,±2.

Fora= 1, this follows from the above mentioned result of M. Mignotte,A. Peth˝oandF. Lemmermeyer.

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Further Diophantine results on the family Fn,a(x,y)

Letm 1. There exists an absolute e↵ectively computable constant such that, if there exists (n,a,m,x,y)2Z5 with a6= 0 verifying

0<|Fn,a(x,y)|m, with n 0, a 1 and |y| 2p3

m, then a µ0 with

µ0 = 8<

:

(logm+ logn)(logn) log logn forn 3,

1 + logm forn = 0,1,2.

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Further Diophantine results on the family Fn,a(x,y)

Letm 1. There exists an absolute e↵ectively computable constant such that, if there exists (n,a,m,x,y)2Z5 with a 1 verifying

0<|Fn,a(x,y)|m, with xy 6= 0, n 0 and a 1, then amax

1, (1 + log|x|) log log(n+ 3), log|y|, logm log(n+ 2) .

(58)

Conjecture on the family Fn,a(x,y)

Assume that there exists(n,a,m,x,y)2Z5 with xy 6= 0 and

|a| 2 verifying

0<|Fn,a(x,y)|m.

We conjecture the upper bound

max{log|n|,|a|,log|x|,log|y|}(1 + logm).

Form>1 we cannot give an upper bound for |n|.

Since the rank of the units of Q( 0) is 2, one may expect a more general result as follows :

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