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Lie theory · Group

SL(2,C)\mathrm{SL}(2,\mathbb C)Lorentz spin group

As a real Lie group, SL(2,ℂ) is the double cover of the identity component SO⁺(3,1) of the Lorentz group.

Compare this group
Reference coverageLorentzSpinors
Definition

2 × 2 complex matrices of determinant 1

Definition sources
Real dimension
66
Source and assumptions
Center
Z2\mathbb Z_{2}
Source and assumptions
Fundamental group
00
Source and assumptions

Reference properties

PropertyValueEvidence
Real dimension66Sources
CenterZ2\mathbb Z_{2}Sources
Fundamental group00Sources
CompactNoSources
ConnectedYesSources
Real rank11Sources

Representations

Finite-dimensional irreducible complex representations of the real Lie group carry labels (jL,jR). Particle-state representations require the Poincaré group and a different category. [sources]

Topology and global form

Polar decomposition gives SL(2,ℂ) ≃ SU(2) × ℝ³ as a manifold. It is simply connected and noncompact. [sources]

In physics

Weyl and Dirac fields, Lorentz covariance, and the distinction between fields and states. [sources]

The Lorentz algebra is a realification

SL(2,C) is being used as a real six-dimensional Lie group. Its real Lie algebra complexifies to sl(2,C) ⊕ sl(2,C), rather than to a single A₁ factor. Finite-dimensional complex irreducibles consequently carry two nonnegative half-integer labels (jL,jR), with dimension (2jL+1)(2jR+1). [sources]

Names and aliases

Spin+(3,1) · Lorentz spin cover

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Claims and sources

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Definition

2 × 2 complex matrices of determinant 1

group:sl-2-c#definition
Real dimension

6

group:sl-2-c#dimension
Center

ℤ₂

group:sl-2-c#center
Fundamental group

0

group:sl-2-c#pi1
Compact

No

group:sl-2-c#compact
Connected

Yes

group:sl-2-c#connected
Real rank

1

group:sl-2-c#rank
Representations

Finite-dimensional irreducible complex representations of the real Lie group carry labels (jL,jR). Particle-state representations require the Poincaré group and a different category.

group:sl-2-c#representations-1
Topology and global form

Polar decomposition gives SL(2,ℂ) ≃ SU(2) × ℝ³ as a manifold. It is simply connected and noncompact.

group:sl-2-c#topology-1
In physics

Weyl and Dirac fields, Lorentz covariance, and the distinction between fields and states.

group:sl-2-c#physics-1
The Lorentz algebra is a realification

SL(2,C) is being used as a real six-dimensional Lie group. Its real Lie algebra complexifies to sl(2,C) ⊕ sl(2,C), rather than to a single A₁ factor. Finite-dimensional complex irreducibles consequently carry two nonnegative half-integer labels (jL,jR), with dimension (2jL+1)(2jR+1).

Derivation: Complexify the realification, then take tensor products of irreducible modules for the two sl(2,C) factors. The simply connected real group integrates every finite-dimensional module.

Premises: algebra:sl-2-c-as-real · algebra:a-1-plus-a-1-c · SU(2) highest weight 2j has dimension 2j+1 · SL(2,C) is simply connected by polar decomposition

group:sl-2-c#real-algebra-1
Related group

group:su-2

group:sl-2-c#relation-1
Related group

group:spin-4

group:sl-2-c#relation-2
Actual real Lie algebra

algebra:sl-2-c-as-real

group:sl-2-c#relation-3
Real-form context

real-form:sl-2-c-as-real

group:sl-2-c#relation-4
Explicit homomorphism

map:sl-2-c-to-lorentz

group:sl-2-c#relation-5