ConceptComplete

Dirichlet's Unit Theorem - Examples and Constructions

Computing fundamental units requires combining continued fractions, lattice reduction, and numerical approximation techniques.

ExamplePell's Equation and Continued Fractions

For K=Q(d)K = \mathbb{Q}(\sqrt{d}) with d>0d > 0 square-free, the fundamental unit is obtained from the continued fraction expansion of d\sqrt{d}.

For d=13d = 13: 13=[3;1,1,1,1,6β€Ύ]\sqrt{13} = [3; \overline{1, 1, 1, 1, 6}] with period 5.

The convergents give solutions to x2βˆ’13y2=Β±1x^2 - 13y^2 = \pm 1:

  • p4/q4=18/5p_4/q_4 = 18/5: gives 182βˆ’13β‹…52=βˆ’118^2 - 13 \cdot 5^2 = -1
  • p9/q9=649/180p_9/q_9 = 649/180: gives 6492βˆ’13β‹…1802=1649^2 - 13 \cdot 180^2 = 1

Therefore Ο΅0=649+18013\epsilon_0 = 649 + 180\sqrt{13} (or Ο΅0=18+513\epsilon_0 = 18 + 5\sqrt{13} if allowing norm βˆ’1-1).

ExampleUnits in Cubic Fields

Consider K=Q(Ξ±)K = \mathbb{Q}(\alpha) where Ξ±3βˆ’Ξ±βˆ’1=0\alpha^3 - \alpha - 1 = 0 (totally real cubic field).

The three real embeddings give r=2r = 2 fundamental units. Using LLL algorithm on the unit lattice: Ο΅1=Ξ±,Ο΅2=Ξ±2βˆ’1\epsilon_1 = \alpha, \quad \epsilon_2 = \alpha^2 - 1

Verification requires checking these are independent under the logarithmic embedding and that they generate OKβˆ—\mathcal{O}_K^* modulo torsion.

ExampleComputing Regulators Numerically

For K=Q(ΞΆ7)K = \mathbb{Q}(\zeta_7) (cyclotomic field of conductor 7):

  • Degree [Q(ΞΆ7):Q]=6[\mathbb{Q}(\zeta_7) : \mathbb{Q}] = 6
  • Signature: r1=0,r2=3r_1 = 0, r_2 = 3, so unit rank r=2r = 2

Fundamental units can be taken as: Ο΅1=1βˆ’ΞΆ721βˆ’ΞΆ7,Ο΅2=1βˆ’ΞΆ731βˆ’ΞΆ7\epsilon_1 = \frac{1 - \zeta_7^2}{1 - \zeta_7}, \quad \epsilon_2 = \frac{1 - \zeta_7^3}{1 - \zeta_7}

Computing embeddings numerically and evaluating the logarithmic map gives regulator RKβ‰ˆ0.5279R_K \approx 0.5279.

Remark

Computational algorithms for units:

  1. LLL reduction: Reduce basis of unit lattice
  2. Enumeration: Search for small-norm elements systematically
  3. Class group computation: Use relation with regulator via class number formula
  4. pp-adic methods: Use pp-adic logarithms for cyclotomic fields

Modern systems (Pari/GP, Magma, SageMath) implement these efficiently.

ExampleStark Units

In abelian extensions of imaginary quadratic fields, Stark units provide explicit generators for unit groups.

For K=Q(i)K = \mathbb{Q}(i) and its ray class field K4=K(1+i)K_4 = K(\sqrt{1+i}), the Stark unit is: Ο΅=1+i\epsilon = \sqrt{1+i}

This unit, predicted by Stark's conjectures, has special properties: its LL-function values encode arithmetic data of the extension.

ExampleS-Units

For a finite set SS of primes, the SS-units are elements invertible outside SS: OK,Sβˆ—={α∈Kβˆ—:vp(Ξ±)=0Β forΒ allΒ pβˆ‰S}\mathcal{O}_{K,S}^* = \{\alpha \in K^* : v_\mathfrak{p}(\alpha) = 0 \text{ for all } \mathfrak{p} \notin S\}

By Dirichlet's SS-unit theorem: OK,Sβˆ—β‰…ΞΌKΓ—Zr+∣Sβˆ£βˆ’1\mathcal{O}_{K,S}^* \cong \mu_K \times \mathbb{Z}^{r + |S| - 1}.

For K=QK = \mathbb{Q} and S={2,3}S = \{2, 3\}: Z(S)βˆ—={Β±2a3b:a,b∈Z}β‰…{Β±1}Γ—Z2\mathbb{Z}_{(S)}^* = \{\pm 2^a 3^b : a, b \in \mathbb{Z}\} \cong \{\pm 1\} \times \mathbb{Z}^2.

SS-units are crucial for solving unit equations and studying integral points on varieties.

ExampleUnits in Compositum Fields

If K1,K2K_1, K_2 are number fields with unit groups OK1βˆ—,OK2βˆ—\mathcal{O}_{K_1}^*, \mathcal{O}_{K_2}^*, the unit group of the compositum K1K2K_1 K_2 relates via: OK1K2βˆ—βŠ‡OK1βˆ—β‹…OK2βˆ—\mathcal{O}_{K_1 K_2}^* \supseteq \mathcal{O}_{K_1}^* \cdot \mathcal{O}_{K_2}^*

The index is bounded and connected to ramification. For linearly disjoint extensions, the regulator satisfies: RK1K2β‰₯RK1[K2:Q]β‹…RK2[K1:Q]R_{K_1 K_2} \geq R_{K_1}^{[K_2:\mathbb{Q}]} \cdot R_{K_2}^{[K_1:\mathbb{Q}]}

with equality when K1,K2K_1, K_2 are linearly disjoint over Q\mathbb{Q}.