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LSU Historical Dissertations and Theses Graduate School
1990 Continuous Functions in Pi-Primary Summands of L(2) of Some Compact Solvmanifolds. Carolyn Beth Pfeffer Louisiana State University and Agricultural & Mechanical College
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Recommended Citation Pfeffer, Carolyn Beth, "Continuous Functions in Pi-Primary Summands of L(2) of Some Compact Solvmanifolds." (1990). LSU Historical Dissertations and Theses. 5015. https://digitalcommons.lsu.edu/gradschool_disstheses/5015
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Continuous functions in 7r-primary summands of L2 o f som e compact solvmanifolds
Pfeffer, Carolyn Beth, Ph.D.
The Louisiana State University and Agricultural and Mechanical Col., 1990
UMI 300 N. Zeeb Rd. Ann Arbor, MI 48106
CONTINUOUS FUNCTIONS IN tt-PRIM ARY SUMMANDS SUMMANDS ARY tt-PRIM IN FUNCTIONS CONTINUOUS .A., State University of New York at Bingham ton, 1983 1983 ton, Bingham at York New of University State .A., A, tt Uiest o e Yr a Bnhmtn 1986 ton, Bingham at York New of University State .A., £ w O F F O L2 Subm itted to the G raduate Faculty of the the of Faculty raduate G the to itted Subm F OE O AT SOLVMANIFOLDS PACT COM SOME OF Agricultural and Mechanical College College Mechanical and Agricultural h Deat n o te atics athem M of ent epartm D The Louisiana State University and and University State Louisiana requirem ents for the degree of of degree the for ents requirem in partial fulfillment of the the of fulfillment partial in Doctor of Philosophy of Doctor Carolyn Beth Pfeffer Pfeffer Beth Carolyn Dissertation A uut 1990 August by in ACKNOWLEDGEMENTS
I wish to express my gratitude and admiration to Professor Leonard Richardson for his careful support and guidance.
Thanks are also due to Professors Lawrence Smolinsky and Lawrence Corwin, for their helpful suggestions and support at crucial times.
I wish also to express my gratitude and love to my father Dr. Morris Pfeffer, for his continuing belief in me. TABLE OF CONTENTS
Page
SECTION 0. Preliminaries ...... 1
§0.1. Introduction ...... 1
§0.2. Classification of 3-dimensional compact solvm anifolds ...... 4
§0.3. Preliminaries...... 9
§0.4. 7r-primary summand functions ...... 13
SECTION 1. Theorems on Solvmanifolds ...... 22
§1.1. Fejer theorems on 3-dimensional compact solvmanifolds ...... 22
§1.2. A Sidon theorem for functions in Hn C L2(M n ,k ) ...... 27
SECTION 2. Zeros of Functions on Solvm anifolds ...... 37
§2.1. Zeros of continuous functions in Hn of a compact nilmanifold . . 37
§2.2. Homotopy classes of functions on a solvmanifold ...... 39
§2.3. Zeros of continuous functions in Hn C L2(MRtp ) ...... 43
§2.4. Zeros of continuous functions in H C L2(MH,k) ...... 52
Bibliography ...... 57
i l i ABSTRACT
The compact quotients of three-dimensional solvable non-nilpotent Lie groups by discrete subgroups fall into two categories; those which are quotients of Sr
(semidirect product, R acts on R 2 by rotation), and those which are quotients of
S r = R oc R2 (semidirect product, R acts on R2 via translation along a hyperbolic orbit).
Continuous functions in the primary summands of L2 of each type of solvman- ifold are examined. It is shown that there exists a Fejer theorem on solvmanifolds
M r which are quotients of Sr] if Pi : L2(M r) i— ► L2(Mr) is orthogonal projec tion onto the ith primary summand of such a quotient, there exists a sequence of operators Sn such that each Sn is a finite linear combination of the Pi, and such that for each continuous function / G L2(Mr), Sn(f) —> / uniformly as n —> oo.
It is shown that no such theorem holds for quotients of S r > for which it is known that orthogonal projections do not preserve continuity of functions. It is shown that if / G L2( M r ) is continuous and Pi(f) is essentially bounded, then Pi(f) m ust be continuous. Together with a result of L. Richardson, this result implies that there are continuous / G L2(M r) for which Pi(f) is essentially unbounded.
It is shown in Section 2 that continuous functions in primary summands of
L2(M r) must vanish on M r , for all compact quotients of M r by discrete sub groups. There are five compact quotients of Sr] one quotient manifold is home- omorphic to the three-dimensional torus, and its continuous primary summand functions need not vanish. For three of the other quotients, it is shown that all continuous primary summand functions must vanish. For the remaining quotient it
iv is known that functions in certain subspaces of the primary summands must vanish, but it is not known whether ail continuous primary summand functions must vanish in this case.
v S E C T IO N O
PRELIMINARIES
§0.1. Introduction
Let G be a solvable, connected and simply connected Lie group, with Lie algebra g and with cocompact discrete subgroup T. By a representation 7r of G we shall mean a strongly continuous, unitary representation of G in some separable
Hilbert space If*.; it will be called irreducible if the space If*. contains no proper closed nontrivial subspace invariant under tt .
Let M be the space of right cosets Tg of T in G, endowed with the quo tient topology. Then G acts on L2(M) by right translation; i.e. g i—> R(g), where [i2(^)/](ra;) = f(Txg) for / 6 L2(M ) (here M has the (7-invariant prob ability measure inherited from Haar measure on G). R is called the quasiregular representation of G on L2{M).
It is well known that L2(M ) decomposes into the direct sum , where the spaces If*, are mutually orthogonal R(G)- invariant subspaces, and R on the space Hn is a finite multiple of the irreducible representation ir. ([GGP], section
1.2). We let (T\(7)A denote the set of irreducible representations appearing in the quasi-regular representation R of G on L2(M). Then the orthogonal projection P* of L2(M ) onto is L2-continuous and preserves C°°(M) ([Aus-Bre 1], theorem
5), and is given by convolution with a bounded Borel measure 1 Now let N be a nilpotent Lie group, connected and simply connected, with Lie
algebra n and cocompact discrete subgroup T.
If the coadjoint orbits of the action of N on the dual n* are linear varieties,
then T\N possesses the property that the orthogonal projections Pn of £2(r\iV) onto Hir preserve continuity ([Ri 1], [Bre 1]). These flat-orbit nilmanifolds share this property with compact quotients of the 3-dimensional solvable group Sr by discrete subgroups. Here Sr denotes the semidirect product R oc R 2, where R acts on R 2 via a one-parameter subgroup of rotations [Ri 1].
The work in chapter 2 was motivated by a theorem of L. Auslander and R.
Tolimieri. Let Hz be the 3-dimensional Heisenberg group, R 3 endowed with the multiplication (x,y, z)(x' ,y' ,zr) = (x + x \y + y' ,z + z' + xy'), and let T be the discrete group of integer points in H z. Let / be a continuous function in H^ C
L2(T\Hz), where n is an irreducible, unitary, infinite dimensional representation in
(r\H 3)A . Then / must have at least one zero on T\Hz ([Aus-Tol], Thm.II.2). This phenomenon arises from a rather surprising interaction between the representation theory of Hz (which determines the primary summand Hn ) and the topology of the manifold T \H z. In chapter 2 of this dissertation, we generalize this theorem to all compact nilmanifolds which are not n-tori. We then examine the question of whether a similar theorem holds for 3-dimensional compact solvmanifolds.
The central covariance of ir-primary summand functions on T\Hz is a key element in Auslander and Tolimieri’s proof that continuous it-primary summand functions have zeros. Since 3-dimensional non-nilpotent solvable Lie groups with cocompact discrete subgroups have trivial centers ([AGH], chapter 3), completely new techniques are needed to show that most 3-dimensional compact solvmani folds do possess the property that their continuous n -primary functions (hereafter referred to as primary functions) must vanish, for infinite-dimensional ir. A note worthy exception is one compact quotient of Sr which is actually homeomorphic to the 3-torus T 3; here one finds plenty of continuous primary functions which do
not vanish, as one would expect. However, for three of four remaining compact
quotients of Sr , it is shown that continuous primary functions must have zeros.
For the fourth compact quotient of Sr , we have shown that continuous functions in
certain subspaces of a primary summand H„ must have zeros. As of this writing,
however, it is conjectured but not known that all continuous primary summand
functions on this manifold must have zeros.
Let Sh be the semidirect product R oc R 2 , where R acts upon R 2 via the A* one-parameter subgroup t in SLi(R), where A + A 1 = k + 1 for
any integer k > 2. It is shown in this dissertation that for all compact quotients
of Sh , continuous primary functions must have zeros. This exhausts the compact
solvmanifolds of dimension three.
Thus the interplay of topology and representation theory which produces zeros
of continuous primary functions is seen to be more than a nilpotent phenomenon,
but the extent of this interaction remains obscure. The possibility of a general
ization of this theorem to a larger class of compact solvmanifolds deserves to be
investigated. The study in section 1 of continuous functions in primary summands
of 3-dimensional compact solvmanifolds was motivated by the fact that orthogo
nal projection onto ir-primary summands preserves continuity of functions in L2
of both compact quotients of flat-orbit nilmanifolds and compact quotients of the
group Sr . In [Ri 2], L. Richardson proved a Fejer theorem for flat-orbit nilman ifolds. In chapter 1 of this dissertation, a Fejer theorem is proved for quotients of Sr by compact discrete subgroups T of Sr . Similar questions are examined for compact quotients of the 3-dimensional solvable group Sr- Let T be a co compact discrete subgroup of Sr- It is known that orthogonal projections Pn of
L2(T\Sr) onto H*. do not preserve continuity [Ri 1]. In chapter 1 of this essay, it is demonstrated that no standard Fejer theorem exists for solvmanifolds of this 4 type. However, the series determining the IJ equivalence class of a projected func tion is seen to bear a resemblance to a standard lacunary Fourier series on R\Z
(see [Zyg]). An adaptation of Sidon’s theorem on convergence of lacunary Fourier series ([Zyg], thm. VI.6.1) is used to demonstrate that if the orthogonal projection
P ^f of a continuous function / on Y\S h is an L°° function, then P^f is actually continuous (Thm. 1.2.1). Together with Theorem 3.13 in [Ri 1], this implies that for each Hn there is continuous / G L2(T\Sh ) such that Pnf is discontinuous and essentially unbounded.
This work suggests the possibility of further similarities in the harmonic anal ysis of flat-orbit nilmanifolds and compact quotients of Sr .
§0.2. Classification of 3-dimensional compact solvmanifolds
The following is a convenient exposition of results due to Auslander, Green and
Hahn ([AGH], section 2.2).
Lemma 0.1. If S is a connected, simply connected, 3 -dimensional non-compact, non-nilpotent solvable Lie group with cocompact discrete subgroup T C S , then the dimension of the maximal nilpotent subgroup N is 2.
The remainder of this section is devoted to proving the following.
Theorem 0.2. If S satisfies the conditions of Lemma 1, then S = Sh or Sr , where r ekt X -kt y Sh = : (t,x,y,) G R 3 l t l j for some k such that ek + e G Z, efc -f e ^2, and
c o s 7rt sin TTt X
- s in 7Tt COS TTt y Sr — 1 t 1 J Proof of Theorem 0.2. We know that N is two-dimensional, from Lemma 1,
and hence abelian. Consider the natural map ir : S — ► N\S. Since N is abelian,
N\S acts on N via ( Ns)n = sns~1 , for Ns G N \S, n G N. It follows that
S = R oc R 2 , where R is the additive group of real numbers acting upon R 2 . We give S the coordinates 51 = (<,«,«) : < € R , (u, v) G R 2 where (t,u,v)(t',ur,v') =
(t -(- t',(u,v) + We then have that TniV is a lattice in N generated by two linearly independent basis vectors. If we coordinatize N so that F fl N is generated by (0,1) and (1,0) in N , then 9 acts on R 2 as a linear transformation which preserves the lattice Z2 .
If 9 — N(t,u,v), then 9 acts by
9 • (0,n,m) = (t,u,v)~1(0 ,n ,m )(t,u ,u ) (0-1) and so the action of 7r(r) upon T fl N is well defined.
9 acts as a linear transformation T(9) which preserves Z2 and so has integral entries and a determinant of ± 1.
It remains to be determined how, in light of these facts, R acts upon R 2 . We must find a 1-parameter subgroup such that <^>(1) = T{9).
Since T(9) must lie on a 1-parameter subgroup , det T{9) — 1, so that
T(9) G SL2(Z). Since successive square roots of T(9) must also have determinant
1, must be a 1-parameter subgroup of S L 2(R).
There are three cases to consider.
Case 1. The eigenvalues of T(9) are real and positive.
Case 2. The eigenvalues of T{9) are real and negative.
C ase 3. The eigenvalues of T{9) are complex conjugates in C R. Lemma 0.3. Let T be a diagonal matrix in SL 2 (R )• If T has a real square root
which is not diagonal, then T = ± 7 .
a b Proof. Suppose there is J11/2 = , b or c nonzero, in SL2 (R). Then c d a2 + be b(a + d) we have P . Since not both b and c are zero, c(a + d) d2 Abe P-1. a + d = 0, and so a2 — d2 . The diagonal terms p,p~1 are thus equal, so that
T = ±1.
Case 1. The eigenvalues of T(9) are real and positive.
Case la. Suppose the eigenvalues of T{9) are positive, real and unequal. The p 0 previous lemma shows that if we write AT(9)A 1 = , then AT(9)A- 1 0 i/p ,1/2 - p i / 2 has 2 square roots, ± The m atrix can ( i / p ),/2 have no further square root. Taking successive square roots we see that A, so th at Case lb. The eigenvalues of T(9) are both 1.
(i) Suppose T(9) = I. Then clearly T(9) lies on a compact, connected, 1- parameter subgroup. Since S is assumed solvable, a cannot be trivial; so cr(t) is a cos 2ir t sin 27rt circle group, isomorphic to — sin 27rt cos 27rt
(ii) Suppose T(9) is not diagonalizable. Then we have, for some A G GL2{R),
1 1 A T { 9 ) A = 0 1
a b Suppose T{9y/2 is a real square root of T{9). Then if T(9)1/2 = we c d a2 + be b(a + d) 1 1 ' have Since (a + d) • b = 1 , we have c = 0; thus c(a + d) d2 + be ° 1 a2 = d? — 1 and so a = d = 1 , since a + d 0. Thus we have 2b = 1 , or 1 1/ 2 ' b — 1/2. The only real square root of T(9) is therefore . Arguing in this 0 way we see that Acr(t)A 1 = q j ’ action of R upon R2 yields the
3-dimensional Heisenberg group H3 .
Case 2. The eigenvalues of T(9) are real and negative.
Case 2a. Suppose the eigenvalues of T(9) are unequal. If so, we may write
AT(0)A~1 = ~P . If T(9)1/2 were a real square root of T{9), then ~P AT{9)XI2 A~l would be a real square root of ~P . However, this matrix
can have no real square root, since by Lemma 0.3 it has no nondiagonal square
root, and it clearly can have no real diagonal square root. Therefore, such a matrix cannot lie on a 1-parameter subgroup of 5'L2(R).
Case 2b. Suppose the eigenvalues of T{9) are —1. If T(9) = —I, then o-(t) is a compact connectedcc subgroup of .S I^R ), and is therefore conjugate to the subgroup cos 7ri sin irt Rot(nt) = — sin irt cos wt a b If T(9) is not diagonalizable, then if is a square root of c d.
AT(9)A- l (for some A € we have 0 -1
a2 + be b(a + d) - 1 1 ' Since b(a + d) = 1 and c(a -f d) = 0 we have c(a + d) d2 + be 0 - 1 0 ; so a 2 d2 ~ 1, a contradiction. Therefore AT(9)A~1 and hence T(9) cannot have a real square root.
Case 3. The eigenvalues of T{9) are complex conjugates in C.
Then oj + uJ = 2Reu> = Tr(T’(^)), the trace of T(9).
If Re(u>) = ±1 we are in cases lb or 2b.
(i) If Tr(T(0)) = 0, the eigenvalues of T(9) are el7r/2 and e~,7r/2; thus T(9) 0 1 is conjugate to the map T , and cr(t) is conjugate to the 1-parameter 1 0 subgroup cos7rt/2 sin7rt/2 -siii7rt/2 cos7rt/2 8
(ii) If Tr(T(0)) = 1, the eigenvalues of T(0) are etir/3 and e t1r/3; thus T(0) 0 - 1 is conjugate to the map T , and cr(t) is conjugate to the 1-parameter cos7t
(iii) If Tr(T(0)) = 1, the eigenvalues of T{9) are e2t7r/ 3 and e 2l,r/ 3 } and connected subgroup of 5,T2(R); hence it is a circle group, isomorphic to the group cos 2irt sin 2 irt — sin 27rt cos 2nt In conclusion, the groups derived in case la are isomorphic to the group Sh-
Pick A G R so that A + A-1 G Z , and A + A-1 > 2. Then if A' is any other positive
number satisfying A' + A'-1 > 2, and A' + A'-1 G Z, then we see that the groups
r A* x ^ y : G R l t l .
and r \ n xi > A'"* y S\i = : (t,x,y) G R 1 t 1 . y are isomorphic via the isomorphism
(t,x,y) G S\ i— ► ((logA, A) • i,x,y) G S\>.
All the other groups derived are isomorphic to Sr , thus proving the main - r theorem of this section.
Therefore we have the following five compact quotients of Sr , with convenient coordinatization.
1- P R,i\S r,\ = M rA ; where Sr = R oc R 2, R acts on R 2 via the one-parameter cos27r< sin27r< subgroup crj (/) , and r flil = {(p ,m ,n ) G SRtl;p,m,n G — sin 27r/ cos 2nt Z}. Here T#,! is isomorphic to the abelian group Z3, and so M r j = T 3 ([Mos],
Theorem A).
2. Tji)2\iS,fl)2 = M r>2; where S r,2 = H. cx R 2, R acts on R 2 via the one-parameter COS TTt sin7T< , _ , / \ r. m subgroup cr2(t) , and r H,2 = UP,™,™) € SRx,P,m,n £ Z}, sin irt cos irt
3- TRf3\S Rt3 = MR>3; where SRf3 = R oc R 2, R acts on R 2 via the one-parameter 0 1 subgroup 4- rj?,4\5’ii,4 = ; where S r^ = R o c R 2, R acts on R 2 via the one-parameter cos7rt/2 sin7rt/2 subgroup 5- r H>6\Sfl,6 = M r$ ; where Sr$ = R a R 2, R acts on R 2 via the one-parameter subgroup We also have the following compact quotients of Sr , with convenient coordi- natizations.
Suppose k £ Z, k > 2. Define Sjj,k = R oc R 2 , where R acts on R 2 via 1 1 the one-parameter subgroup §0.3. Preliminaries
Let G be a connected, simply connected Lie group with Lie algebra g, and let g* be the vector space of linear functionals on g . We define a sequence of ideals 10
of the Lie algebra g by g^0) = g, = [g^fc_1\g ^fc_1^]; this is called the derived
series of g, and g is said to be solvable if g^n) = 0 for some n € N. We define
another sequence of ideals of the Lie algebra g by g ^ = g, g ^ = [g^fc_1^,g]; this is
called the lower central series of g, and g is said to be nilpotent if g ^ = 0 for some
n € N (see [Hum], section 3). Throughout this dissertation, the term “nilmanifold”
(“solvmanifold”) will refer to compact spaces r\G , where G is nilpotent (solvable)
and r is discrete and cocompact.
By a representation tt of G we shall mean an equivalence class of strongly
continuous homomorphisms of G into the set of unitary linear transformations on
some separable Hilbert space H . The representation n will be called irreducible if
H contains no proper closed subspace invariant under ir.
The adjoint representation of the group G in the vector space g, written Ad,
is defined as follows; for each element ifG, Ad(a:) : g — > g is the differential at
the identity of G of the group automorphism I(x), inner conjugation by x £ G.
Ad(x) satisfies
x(exp X )x ~1 = exp[Ad(jc)AT] (0-2)
for each x £ G, X £ g.
The coadjoint representation of G is of central importance in the representa
tion theory of nilpotent and solvable Lie groups. The set of equivalence classes of
irreducible representations of a nilpotent Lie group G is naturally parametrized by
the orbit space g*/Ad*G; this is also true for the (completely) solvable Lie groups
examined in this work. This parametrization, due to A. A. Kirillov, is freely drawn
upon in this work; for details, see [CG], chapter II.
As described in section 0.2, there are two 3-dimensional, solvable, non-nilpotent
Lie groups with cocompact discrete subgroups, the groups Sh and S r . Their Lie
algebras are three- dimensional vector spaces spanned by the vectors T, X, and Y, where exp sT = (s,0,0), exp sX = (0,5,0), and exp sY — (0 ,0 ,s). 11
There are 5 distinct, non-homeomorphic compact quotients of Sr, and in
finitely many distinct compact quotients of Sh■> as seen in section 0 .2 .
It will be convenient to use several different coordinatizations of Sr and Sh •
The coordinatizations of Sr described at the end of section 0.2 will be called
integral coordinatizations of S r }P. Let A € GL2{R) be such that A