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Left-invariant CR structures on 3-dimensional Liegroups
Gil Bor and Howard Jacobowitz
June 8, 2020
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 1 / 26
A CR structure on a 3-dimensional manifold M is a rank 2 subbundleD ⊂ TM together with an almost complex structure J on D
J : D → D, J2 = −Id .
Equivalently, a CR structure is a complex line subbundle V ⊂ TM ⊗ Csuch that V ∩ V = {0}.
D = {<V ,=V }
Notation: (M,V ) or (M, L).Usually assume L, L̄, [L, L̄] linearly independent (spc).Note: [L, L̄] ≡ 0 means that M is foliated by complex curves.f : M → C is a CR function if Lf = 0 for each section of V .
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 2 / 26
G a 3 dimensional Lie groupG its Lie algebra
G = TeG = {L : g∗Le = Lg}
(G , L) is a CR manifold provided
L ∩ L̄ = {0}.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 3 / 26
ConjugationΦ : G → Aut(G )
Φ(g)h = ghg−1
induces a mapAd : G → Aut(G)
with derivative at the identity
ad : G→ G
given byad(X )Y = [X ,Y ].
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 4 / 26
Immersions into CP2
A complex line sub-bundle V ⊂ T (G )⊗ C determines a point inP(G⊗ C) = CP2, L→ [L] ∈ P(G⊗ C), and the orbit of L
{X : ∃g ∈ G , AdgL = X}
gives a map of G into CP2
φ : G → CP2
g → [AdgL]
with differential at the identity
φ∗X = [[X , L]].
φ is always a CR mapG → CP2.
φ is an immersion if
[X , L] = 0 for X real ⇒ X = 0.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 5 / 26
Spherical and Aspherical
(M,V ) is spherical near a point if it is locally CR equivalent to thestandard CR structure on S3.
Theorem (Cartan 1932)
The local CR equivalence group of a 3 dimensional aspherical CR manifoldhas dimension at most 3.
Consider two left-invariant aspherical CR structures (Gi ,Vi ) on twoconnected 3-dimensional Lie groups Gi
Corollary
If the two CR structures are locally equivalent, then there exists a groupisomorphism G1 → G2 which extends this local CR equivalence.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 6 / 26
Proof.1 Right-invariant vector fields generate left-translations. SoRGi⊂ AutCR(Gi ,Vi ).
2 Since the dimension are equal these groups coincide near the identity.
3 The local CR equivalence f maps RG1 → RG2 .
4 f preserves the group structure.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 7 / 26
The most interesting examples: SL(2,R) and SU(2)
Basis for sl(2,R) [1 00 −1
],
[0 10 0
],
[0 01 0
]Basis for su(2) [
1 00 −1
],
[0 1−1 0
],
[0 ii 0
]Note
sl(2,C) = su(2)⊗ C.
andP(G⊗ C) = P(sl(2,C)) = CP2.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 8 / 26
Geometry of P(sl(2,C))
Let L ∈ sl(2,C) be given as [a bc −a
].
The Killing form is
K (L, L) = a2 + bc = −detL
andK (L, L) = 0
defines a conic in C = CP1 ⊂ P(sl(2,C)). The polar line with respect to Cof a point [L] ∈ CP2 determines two points in C.
S = {{ζ1, ζ2} : ζi ∈ CP1}.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 9 / 26
L→ [L] ∈ P(sl(2,C))→ S
is SL(2,C) equivariant.
P(sl(2,C))Adg−→ P(sl(2,C)))y y
S −→g
S
Classifying the orbits of [L] under SL(2,R) or SU(2) uses that
SL(2,R) preserves the hyperbolic distance in the upper half-plane.
SU(2) preserves the Euclidean distance in S2.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 10 / 26
So the following are equivalent:
1 [L] and [L̃] are in the same AutG orbit.
2 d(ζ1, ζ2) = d(ζ̃1, ζ̃2).
3 The left-invariant CR structures (G , L) and (G , L̃) are CR equivalentunder a group automorphism.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 11 / 26
Theorem
Let Vt ⊂ TCSL(2,R), t ∈ (−1, 1] be the left-invariant complex line bundlespanned at e by
Lt =
(i 1+t
2 t1 −i 1+t
2
)∈ sl2(C).
Then
1 Vt is a left-invariant CR structure for all t 6= 0.
2 V0 is a foliation by complex curves.
3 Vt is spherical if t = 1 or −3± 2√
2 and aspherical otherwise.
4 Every left-invariant CR structure on SL2(R) is CR equivalent to Vt
for a unique t.
5 The aspherical left-invariant CR structures Vt ,t ∈ (−1, 1) \ {0,−3 + 2
√2}, are pairwise non-equivalent, even locally.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 12 / 26
The immersion results rely on a geometric observation. Recall the nullcone of the Killing form of sl(2,R)
C = {L : a2 + bc = 0}.
A left-invariant CR structure on SL(2,R) is called hyperbolic if the real2-plane spanned by {<L,=L} intersects C in two lines. It is called ellipticif the intersection is the origin.Note: One spherical structure is elliptic, the other is hyperbolic.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 13 / 26
Theorem1 The elliptic left-invariant spherical CR structure on SL(2,R) (t = 1)
is realizable by the map(a bc d
)→(b + iad + ic
).
It is also realizable as the complement of S3 ∩ C1.
2 The hyperbolic spherical structure on SL(2,R) (t = −3 + 2√
2) isrealizable as the complement of S3 ∩R2.
3 The rest of the left-invariant CR structures on SL(2,R) are either4 : 1 covers, in the aspherical elliptic case 0 < t < 1, or 2 : 1 covers,in the aspherical hyperbolic case −1 < t < 0, of the orbits ofSL(2,R) in P(sl(2,C)).
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 14 / 26
Theorem
Let Vt ⊂ TCSU(2), t ≥ 1 be the left-invariant complex line bundlespanned at e ∈ SU(2) by
Lt =
(0 t − 1
t + 1 0
).
1 Vt is a left-invariant CR structure on SU(2) for all t ≥ 1.
2 Vt is spherical if and only if t = 1.
3 Every left-invariant CR structure on SU(2) is CR equivalent to Vt fora unique t.
4 The aspherical left-invariant CR structures Vt , t > 1, are pairwisenon-equivalent, even locally.
5 V1 is realized by the usual CR structure on S3 ⊂ C2. The asphericalstructures are realized as 4 : 1 covers of the adjoint orbits of SU(2) inP(sl(2,C)).
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 15 / 26
The Heisenberg Group
H =
1 a c
0 1 b0 0 1
: a, b, c ∈ R
and
h =
0 x z
0 0 y0 0 0
: a, b, c ∈ R
H is isomorphic to the group on the hyperquadric
{(z ,w) ∈ C2 : =w = |z |2}.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 16 / 26
Theorem1 Every plane in h containing 0 0 1
0 0 00 0 0
gives a foliation of H by complex curves.
2 Every other plane is in the orbit of
L =
0 1 00 0 i0 0 0
under Aut(H).
3 L gives a spherical CR structure equivalent to the usual one on thehyperquadric.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 17 / 26
ObservationLet Vt , t ∈ R be a smooth family of CR structures on some M3, such that
Vt ≡ Vs for s 6= 0, t 6= 0
butV1 6≡ V0.
Then V0 is a foliation of M by complex curves.Example
Lt =
0 i 10 0 t0 0 0
→o i 1
0 0 00 0 0
.
{Lt , L̄t} is not involutive for t 6= 0 but {L0, L̄0} is involutive.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 18 / 26
The Euclidean Group
E =
cos θ sin θ u− sin θ cos θ v
0 0 1
e =
0 x y−x 0 z0 0 0
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 19 / 26
Theorem
Let V ⊂ TCE be the left-invariant line bundle whose value at e ∈ E isspanned by
L =
0 −i 1i 0 00 0 0
.
Then
1 Every spc left-invariant CR structure on E is CR equivalent to V byAut(E ).
2 V is a aspherical.
3 V is realized in P(e⊗ C) = CP2 by the adjoint orbit of [L]. This isCR equivalent to the real hypersurface [<(z1)]2 + [<(z2)]2 = 1 in C2.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 20 / 26
Lt =
0 −it ait 0 bi0 0 0
is an aspherical CR structure for t 6= 0 but a foliation by complex curvesfor t = 0.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 21 / 26
Cartan’s Moving Frames
H −→ SU(2, 1)yQ
dimSU(2, 1) = 8, dimH = 5.Maurer-Cartan form Θ : TSU(2, 1)→ su(2, 1)
Let M be a three dimensional (spc) CR structure.
H5 −→ B8yM3
Θ : TB ⊗ C→ su(2, 1)⊗ C.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 22 / 26
Theorem
With each spc CR 3-manifold M there is canonically associated a bundleB → M with Cartan connection Θ : TB → su(2, 1), satisfying
1 The eight components of Θ are pointwise linearly independent.
2 (The CR structure equations) There exist functions R,S : B → Csuch that
dθ = iθ1 ∧ θ̄1 − θ ∧ (θ2 + θ̄2),
dθ1 = −θ1 ∧ θ2 − θ ∧ θ3,dθ2 = 2i θ1 ∧ θ̄3 + i θ̄1 ∧ θ3 − θ ∧ θ4,dθ3 = −θ1 ∧ θ4 − θ̄2 ∧ θ3 − R θ ∧ θ̄1,dθ4 = i θ3 ∧ θ̄3 − (θ2 + θ̄2)θ4 + (S θ1 + S̄ θ̄1) ∧ θ.
3 (Spherical structures) M is spherical if and only if R ≡ 0.
4 Any local CR diffeomorphism of CR manifolds f : M → M ′ liftsuniquely to an map f̃ : B → B ′ with f̃ ∗Θ′ = Θ.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 23 / 26
φ, φ1 is an adapted coframe for the CR structure V on M if
1
φ is real.
2
φ(V ) = 0, φ1(V ) = 0.
3
φ ∧ φ1 ∧ φ̄1 6= 0.
4
dφ = i φ1 ∧ φ̄1.
Each adapted coframe has a unique lift to σ : M → B such that σ∗θ = φand σ∗θ1 = φ1.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 24 / 26
Pulling back the other components of Θ we obtain
dφ = iφ1 ∧ φ̄1 − φ ∧ (φ2 + φ̄2),
dφ1 = −φ1 ∧ φ2 − φ ∧ φ3,dφ2 = 2i φ1 ∧ φ̄3 + i φ̄1 ∧ φ3 − φ ∧ φ4,dφ3 = −φ1 ∧ φ4 − φ̄2 ∧ φ3 − r φ ∧ φ̄1,dφ4 = i φ3 ∧ φ̄3 + (s φ1 + s̄ φ̄1) ∧ φ.
M is spherical if and only if the Cartan relative curvature invariant r isidentically 0.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 25 / 26
Lemma
Let M be a manifold with a CR structure given by a coframe φ, φ1satisfying
dφ = iφ1 ∧ φ̄1,dφ1 = aφ1 ∧ φ̄1 + b φ ∧ φ1 + c φ ∧ φ̄1,
(1)
for some complex constants a, b, c . Then
r = ic(|a|2
3+
3ib
2).
If a left-invariant CR structure has a coframe satisfying (1) then a, b, care constants and so the structure is spherical if and only if
c(|a|2
3+
3ib
2) = 0.
Gil Bor and Howard Jacobowitz Left-invariant CR structures on 3-dimensional Lie groups June 8, 2020 26 / 26