research33 min studyLesson 505 in Mathematics

Root systems and Dynkin diagrams

Recover integral reflection data from root geometry while fixing the Cartan-matrix orientation.

On this page

What you’ll understand

  • Calculate coroot pairings and a Cartan matrix with a declared index convention.
  • Translate rank-two angle and length data into a Dynkin diagram.
  • State what the finite complex semisimple classification determines and what it does not.

The roots of a finite-dimensional complex semisimple Lie algebra form a finite reduced crystallographic root system in their real span. This geometric object retains enough information to classify the algebra, yet its diagram is only a compressed encoding of precise numerical rules. Root lengths, coroot pairings, and index conventions matter when multiple edges appear. A calculation that looks like a transposed matrix can reflect a convention change rather than a different algebra.

Reflections and integrality restrict the geometry

Choose a positive-definite invariant inner product on the real root span. Reflection in the hyperplane perpendicular to α sends β to β−2(β,α)α/(α,α) and preserves the root set. Crystallographic integrality requires the coefficient 2(β,α)/(α,α) to be an integer for roots α and β. Reducedness says the only scalar multiples of a root that are roots are itself and its negative. These requirements exclude many otherwise plausible finite arrow configurations. The geometric inner product is not the original complex Killing form treated as a Hermitian norm.

A positive system determines simple roots, which form a basis of the real root span and express each positive root as a nonnegative integral combination. Simple roots have nonpositive mutual pairings. Root strings are compatible with the sl(2) structure: if β−pα through β+qα is a string for nonproportional roots, then p−q equals the coroot pairing of β with α. This integrality is a consequence of finite strings, not an arbitrary lattice decoration added after drawing the roots.

sα(β)=β−⟨β,α∨⟩α,⟨β,α∨⟩=2(β,α)(α,α),aij=⟨αj,αi∨⟩s_\alpha(\beta)=\beta-\langle\beta,\alpha^\vee\rangle\alpha,\qquad \langle\beta,\alpha^\vee\rangle=\frac{2(\beta,\alpha)}{(\alpha,\alpha)},\qquad a_{ij}=\langle\alpha_j,\alpha_i^\vee\rangle
This lesson uses coroot index i in the first Cartan-matrix index. Some sources transpose that convention, so compare definitions before comparing entries.↔ Scroll wide equations horizontally.

A Dynkin edge records an angle and, when needed, a direction

Diagonal Cartan entries are two. Off-diagonal entries are nonpositive integers, and the product aᵢⱼaⱼᵢ is 0,1,2, or 3 for distinct simple roots in a finite root system. These cases correspond to no edge, a single edge, a double edge, or a triple edge. Multiple edges carry an arrow toward the shorter root. The product determines the angle while the ratio determines the squared-length ratio. A double line without its short-root orientation loses information needed to distinguish the two standard coroot conventions.

For example, type B₂ can be represented by long simple root e₁−e₂ and short simple root e₂ in an orthonormal plane. Their inner product is −1, with squared lengths two and one. Under this lesson's convention the Cartan matrix has first row (2,−1) and second row (−2,2). Transposing it exchanges the root and coroot viewpoints. B₂ and C₂ give isomorphic complex Lie algebras, a low-rank coincidence that should not be extrapolated to all higher ranks.

aijaji=4cos⁡2θij,(αi,αi)(αj,αj)=ajiaij(aij≠0)a_{ij}a_{ji}=4\cos^2\theta_{ij},\qquad \frac{(\alpha_i,\alpha_i)}{(\alpha_j,\alpha_j)}=\frac{a_{ji}}{a_{ij}}\quad(a_{ij}\ne0)
The angle is between distinct simple roots and is obtuse when they are connected. The length-ratio identity uses the same coroot-first indexing convention.↔ Scroll wide equations horizontally.

Classification concerns a field and a category

Connected finite Dynkin diagrams classify simple complex Lie algebras up to isomorphism. One nonredundant list uses Aₙ for n≥1, Bₙ for n≥2, Cₙ for n≥3, Dₙ for n≥4, and the exceptional E₆,E₇,E₈,F₄,G₂. Semisimple algebras correspond to disjoint unions, or direct sums of simple factors. Small-rank identifications explain the range restrictions. Establishing that each diagram produces an algebra uses generators and Serre relations; the root-system geometry alone is not the full construction proof.

The diagram does not classify real forms or determine the global topology of a Lie group integrating the complex algebra. Simply connected and adjoint groups can share the same Lie algebra while admitting different representation descent conditions. Nor does every generalized Cartan matrix define a finite-dimensional semisimple algebra; dropping the finite positive-definite root-system condition leads into other theories. A diagram is powerful precisely because its scope is controlled: finite reduced crystallographic roots and finite-dimensional complex semisimple structure.

Decode B₂ without guessing the arrow

Use α₁=e₁−e₂ and α₂=e₂. Compute the Cartan matrix, edge type, arrow direction, root count, and Lie-algebra dimension.

  1. The squared lengths are 2 and 1, and the mutual inner product is −1. Therefore a₁₂=2(−1)/2=−1 and a₂₁=2(−1)/1=−2.

  2. The product is 2, so the diagram has a double edge. The arrow points toward α₂ because it is shorter. The Cartan matrix is [[2,−1],[−2,2]].

  3. The complete B₂ system contains ±e₁, ±e₂, and ±e₁±e₂: eight roots. One-dimensional root spaces plus a rank-two Cartan give dimension 8+2=10.

The result

The diagram and dimension follow from checked lengths and root counts. The asymmetric entries encode the short-root direction rather than a failure of the underlying inner product to be symmetric.

Explore the model

Interactive lab

Interactive lab · vectors

Check the A₂ angle numerically

Reset, set angle 0° and magnitude 1 to represent α₁=(1,0). For a fresh comparison, Reset, set angle 120° and magnitude 1 to represent α₂=(−1/2,√3/2). Predict dot product −1/2 and both off-diagonal Cartan entries −1. Their sum has length one and angle 60°. This instrument displays one vector per run, not an entire root system or a Dynkin classification.

Check the A₂ angle numericallyPlayback traces a fixed vector and its projections. Angle and magnitude set the geometry; the moving marker does not change them. Current readings: x component: 1.393; y component: 0.975; Magnitude: 1.7. All parameters are adjustable with the labeled controls below.−7.46−3.7303.737.46−3.5−1.7501.753.5xyvvₓ = 1.39
Vectorx / y projectionsTrace marker
x component
1.393
y component
0.975
Magnitude
1.7
t = 0 s

Playback traces a fixed vector and its projections. Angle and magnitude set the geometry; the moving marker does not change them. Parameter changes pause playback and recompute the model at the current elapsed time. Reset restores both parameters and returns time to zero. Playback starts paused. Adjust either parameter, then choose Play or Step.

Look forSimple-root geometry produces integral Cartan entries through a specified normalization.

Check your understanding

With aᵢⱼ=⟨αⱼ,αᵢ∨⟩, α₁²=2, α₂²=1, and (α₁,α₂)=−1, which pair is correct?

Try it yourself

Take α₁=(1,0) and α₂=(−1/2,√3/2). Compute their Cartan matrix and list the positive A₂ roots for this simple system.

Take a moment to make a prediction or work it out on paper. Open a hint when you need one.

Give me a hint

Both squared lengths are one, and the sum α₁+α₂ has the same length.

Compare with the solution

The mutual inner product is −1/2, so a₁₂=a₂₁=−1 and the matrix is [[2,−1],[−1,2]]. The positive roots are α₁, α₂, and α₁+α₂=(1/2,√3/2). Their negatives give six roots in total. Rescaling all roots together changes lengths but not these Cartan entries or the Dynkin diagram; the chosen unit-length realization is therefore compatible with type A₂.

Take it with you

  • Integral coroot pairings encode root geometry.
  • Cartan indexing and short-root arrows must be declared together.
  • Finite complex Lie-algebra classification does not settle real forms or group topology.

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