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138 DANIEL J. MADDEN<br />

(6l + 7) k + 3l − 1<br />

3<br />

+ 2; 1, 2 (6l + 7)k−1 − 1<br />

,<br />

3<br />

−→<br />

N1, −→<br />

N2, . . . , −→<br />

N k−2,<br />

(6l + 7) k−1 − 1<br />

, 2,<br />

3<br />

(6l + 7)k−2 − 1<br />

+ 2, 2,<br />

3<br />

(6l + 7)k−1 − 1<br />

,<br />

3<br />

←<br />

N k−2, ←<br />

N k−3, . . . , ←<br />

N2, ←<br />

N1, 2 (6l + 7)k−2 − 1<br />

+ 4<br />

3<br />

Since r = 6l + 7 is odd, d is not equivalent to 1 (mod 4); so when d is square<br />

free, we have the fundamental unit of Q( √ d):<br />

β2k 2α2 where α = − (6l+7)k +3l−1<br />

6 + 1<br />

√ (6l+7)<br />

2 d and β = 3 + k +3l−1<br />

6<br />

If we begin with<br />

<br />

u v<br />

N = {a1; a2, . . . , an} = ,<br />

2v w<br />

+ 1<br />

√<br />

2 d.<br />

then all the powers N n will have the same matrix form. We can use the<br />

Chebychev polynomials to express these powers explicitly.<br />

First we recall how Chebychev polynomials can be used to deal with<br />

quadratic units. (See page 355 in [LN].) We begin with the identity<br />

x k + y k =<br />

⌊ k<br />

2 ⌋<br />

<br />

j=0<br />

k<br />

k − j<br />

k<br />

k − j<br />

If we have a quadratic unit β with norm ɛ,<br />

β k + ¯ β k ⌊<br />

=<br />

k<br />

2 ⌋ <br />

k k<br />

k − j k − j<br />

j=0<br />

Therefore if β = s + t √ d has norm 1<br />

β k + ¯ β k ⌊<br />

=<br />

k<br />

2 ⌋ <br />

k k<br />

k − j k − j<br />

j=0<br />

<br />

(−xy) j (x + y) k−2j .<br />

(−ɛ) j (β + ¯ β) k−2j .<br />

(−1) j (2s) k−2j = 2Tk(s)<br />

where Tk(s) is the Chebychev polynomial of the first kind of degree k.<br />

If<br />

<br />

u<br />

N = {a1; a2, . . . , an} =<br />

2v<br />

<br />

v<br />

w<br />

has determinant one, N n can be explicitly given in terms of the rational<br />

part of the eigenvalues of N. Let<br />

β = 1<br />

<br />

u + w +<br />

2<br />

(u + w) 2 <br />

− 4<br />

<br />

.

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