ConceptComplete

Dirichlet's Unit Theorem - Key Properties

The logarithmic embedding and regulator provide geometric tools for understanding the unit group structure.

DefinitionLogarithmic Embedding

Let Οƒ1,…,Οƒr1\sigma_1, \ldots, \sigma_{r_1} be the real embeddings and Ο„1,Ο„Λ‰1,…,Ο„r2,Ο„Λ‰r2\tau_1, \bar{\tau}_1, \ldots, \tau_{r_2}, \bar{\tau}_{r_2} be the complex embeddings of KK. The logarithmic embedding is: Ξ»:OKβˆ—β†’Rr1+r2\lambda: \mathcal{O}_K^* \to \mathbb{R}^{r_1 + r_2} Ξ»(Ο΅)=(logβ‘βˆ£Οƒ1(Ο΅)∣,…,logβ‘βˆ£Οƒr1(Ο΅)∣,2logβ‘βˆ£Ο„1(Ο΅)∣,…,2logβ‘βˆ£Ο„r2(Ο΅)∣)\lambda(\epsilon) = (\log|\sigma_1(\epsilon)|, \ldots, \log|\sigma_{r_1}(\epsilon)|, 2\log|\tau_1(\epsilon)|, \ldots, 2\log|\tau_{r_2}(\epsilon)|)

The factor of 2 for complex embeddings accounts for conjugate pairs. This map takes products to sums: λ(ϡη)=λ(ϡ)+λ(η)\lambda(\epsilon\eta) = \lambda(\epsilon) + \lambda(\eta).

The image of Ξ»\lambda lies in the trace-zero hyperplane: H={(x1,…,xr1+r2)∈Rr1+r2:βˆ‘i=1r1xi+βˆ‘j=1r2xj=0}H = \left\{(x_1, \ldots, x_{r_1+r_2}) \in \mathbb{R}^{r_1+r_2} : \sum_{i=1}^{r_1} x_i + \sum_{j=1}^{r_2} x_j = 0\right\}

This follows from NK/Q(Ο΅)=Β±1N_{K/\mathbb{Q}}(\epsilon) = \pm 1, giving βˆ‘ilogβ‘βˆ£Οƒi(Ο΅)∣+2βˆ‘jlogβ‘βˆ£Ο„j(Ο΅)∣=0\sum_i \log|\sigma_i(\epsilon)| + 2\sum_j \log|\tau_j(\epsilon)| = 0.

DefinitionRegulator

Let Ο΅1,…,Ο΅r\epsilon_1, \ldots, \epsilon_r be fundamental units. The regulator RKR_K is the absolute value of the determinant of any (rΓ—r)(r \times r) minor of the (rΓ—(r+1))(r \times (r+1)) matrix with rows Ξ»(Ο΅i)\lambda(\epsilon_i).

Explicitly, for a real quadratic field with fundamental unit ϡ0\epsilon_0: RK=∣log⁑∣ϡ0∣∣R_K = |\log|\epsilon_0||

For general fields, RKR_K measures the "volume" of the fundamental domain of the unit lattice in the trace-zero hyperplane.

ExampleComputing Regulators

For K=Q(2)K = \mathbb{Q}(\sqrt{2}), the fundamental unit is Ο΅0=1+2\epsilon_0 = 1 + \sqrt{2} with norm βˆ’1-1.

The two real embeddings are Οƒ1(Ο΅0)=1+2β‰ˆ2.414\sigma_1(\epsilon_0) = 1 + \sqrt{2} \approx 2.414 and Οƒ2(Ο΅0)=1βˆ’2β‰ˆβˆ’0.414\sigma_2(\epsilon_0) = 1 - \sqrt{2} \approx -0.414.

The regulator is: RK=∣log⁑∣1+2∣∣=log⁑(1+2)β‰ˆ0.881R_K = |\log|1 + \sqrt{2}|| = \log(1 + \sqrt{2}) \approx 0.881

For K=Q(5)K = \mathbb{Q}(\sqrt{5}), fundamental unit Ο΅0=1+52\epsilon_0 = \frac{1+\sqrt{5}}{2} (golden ratio): RK=log⁑(1+52)β‰ˆ0.481R_K = \log\left(\frac{1+\sqrt{5}}{2}\right) \approx 0.481

TheoremUnit Lattice

The image Ξ»(OKβˆ—)\lambda(\mathcal{O}_K^*) is a lattice in the hyperplane Hβ‰…RrH \cong \mathbb{R}^r of rank r=r1+r2βˆ’1r = r_1 + r_2 - 1.

The fundamental units generate this lattice: Ξ»(OKβˆ—)=ZΞ»(Ο΅1)+β‹―+ZΞ»(Ο΅r)\lambda(\mathcal{O}_K^*) = \mathbb{Z}\lambda(\epsilon_1) + \cdots + \mathbb{Z}\lambda(\epsilon_r).

The regulator RKR_K equals the covolume of this lattice in HH.

Remark

The regulator appears in the class number formula: hK=wKβˆ£Ξ”K∣2r1(2Ο€)r2RKlim⁑sβ†’1+(sβˆ’1)ΞΆK(s)h_K = \frac{w_K \sqrt{|\Delta_K|}}{2^{r_1}(2\pi)^{r_2} R_K} \lim_{s \to 1^+} (s-1)\zeta_K(s)

Large regulators correspond to "sparse" unit groups (fundamental units with large norm), while small regulators indicate "dense" units. The product hKRKh_K R_K appears in the Brauer-Siegel theorem.

ExampleCyclotomic Units

For K=Q(ΞΆp)K = \mathbb{Q}(\zeta_p) with pp prime, explicit units are: Ο΅k=1βˆ’ΞΆpk1βˆ’ΞΆp,k=2,…,pβˆ’12\epsilon_k = \frac{1 - \zeta_p^k}{1 - \zeta_p}, \quad k = 2, \ldots, \frac{p-1}{2}

These cyclotomic units have rank (pβˆ’3)/2(p-3)/2, exactly the unit rank. They generate a subgroup of finite index in OKβˆ—\mathcal{O}_K^*, and the index (the unit index) divides the class number.