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Lie theory · Group

SL(3,R)\mathrm{SL}(3, \mathbb R)Real special linear group in three dimensions

Split real matrix form of A₂. The real 3 × 3 matrices of determinant 1.

Compare this group
Reference coverageNoncompact Lie groupSimple algebraGlobal form
Definition

The real 3 × 3 matrices of determinant 1.

Definition sources
Real dimension
88
Source and assumptions
Fundamental group π₁
C2\mathrm{C}_{2}
Source and assumptions

Reference properties

PropertyValueEvidence
Real dimension88Sources
Real rank22Sources
Center11Sources
Fundamental group π₁C2\mathrm{C}_{2}Sources
CompactNoSources
ConnectedYesSources
AbelianNoSources
Simple real Lie algebraYesSources
Global formSplit real matrix form of A₂Sources
Real Lie algebrasl(3,R)\mathfrak{sl}(3, \mathbb R)Sources
Maximal compact subgroupSO(3)\mathrm{SO}(3)Sources

Global structure and topology

Polar decomposition identifies the manifold with SO(3) × R⁵. Therefore π₁ is C₂ and this centerless matrix group is not simply connected. Real scalar matrices of determinant 1 give only the identity in its center. [sources]

Representation category and descent

The defining real 3 gives a faithful matrix representation. Finite-dimensional complex irreducibles are restrictions of sl(3,C) highest-weight modules; representation data for infinite-dimensional unitary families are outside this record. [sources]

Related objects and maps

Claims and sources

Each assertion has a stable identifier within this record and a source locator or derivation. Cite the dataset edition when referring to a corrected or historical claim.

Definition

The real 3 × 3 matrices of determinant 1.

group:sl-3-r#definition
Real dimension

8

group:sl-3-r#dimension
Real rank

2

group:sl-3-r#real-rank
Center

1

group:sl-3-r#center
Fundamental group π₁

C₂

Derivation: Cartan decomposition is a deformation retraction onto the stated maximal compact subgroup; compute its fundamental group.

Premises: Maximal compact subgroup: SO(3) · π₁(SO(2))=Z, π₁(SO(n))=C₂ for n≥3, π₁(U(2))=Z · For S(U(2)×U(2)), the determinant map has simply connected fiber SU(2)×SU(2), giving π₁=Z

group:sl-3-r#pi1
Compact

No

group:sl-3-r#compact
Connected

Yes

group:sl-3-r#connected
Abelian

No

group:sl-3-r#abelian
Simple real Lie algebra

Yes

group:sl-3-r#simple-algebra
Global form

Split real matrix form of A₂

group:sl-3-r#global-form
Real Lie algebra

sl(3, R)

group:sl-3-r#lie-algebra
Maximal compact subgroup

SO(3)

group:sl-3-r#maximal-compact
Global structure and topology

Polar decomposition identifies the manifold with SO(3) × R⁵. Therefore π₁ is C₂ and this centerless matrix group is not simply connected. Real scalar matrices of determinant 1 give only the identity in its center.

group:sl-3-r#topology-1
Representation category and descent

The defining real 3 gives a faithful matrix representation. Finite-dimensional complex irreducibles are restrictions of sl(3,C) highest-weight modules; representation data for infinite-dimensional unitary families are outside this record.

group:sl-3-r#representations-1
Real Lie algebra

algebra:sl-3-r

group:sl-3-r#relation-1
Real-form context

real-form:sl-3-r

group:sl-3-r#relation-2