Nontrivial Deformation of a Trivial Bundle

The SU(2)-prolongation of the Hopf fibration S³→S² is a trivializable principal SU(2)-bundle. We present a noncommutative deformation of this bundle to a quantum principal SUq(2)-bundle that is not trivializable. On the other hand, we show that the SUq(2)-bundle is piecewise trivializable with respe...

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Автори: Hajac, P.M., Zieliński, B.
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Назва видання:Symmetry, Integrability and Geometry: Methods and Applications
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Цитувати:Nontrivial Deformation of a Trivial Bundle / P.M. Hajac, B. Zieliński // Symmetry, Integrability and Geometry: Methods and Applications. — 2014. — Т. 10. — Бібліогр.: 14 назв. — англ.

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spelling irk-123456789-1468232019-02-12T01:24:50Z Nontrivial Deformation of a Trivial Bundle Hajac, P.M. Zieliński, B. The SU(2)-prolongation of the Hopf fibration S³→S² is a trivializable principal SU(2)-bundle. We present a noncommutative deformation of this bundle to a quantum principal SUq(2)-bundle that is not trivializable. On the other hand, we show that the SUq(2)-bundle is piecewise trivializable with respect to the closed covering of S² by two hemispheres intersecting at the equator. 2014 Article Nontrivial Deformation of a Trivial Bundle / P.M. Hajac, B. Zieliński // Symmetry, Integrability and Geometry: Methods and Applications. — 2014. — Т. 10. — Бібліогр.: 14 назв. — англ. 1815-0659 2010 Mathematics Subject Classification: 58B32 DOI:10.3842/SIGMA.2014.031 http://dspace.nbuv.gov.ua/handle/123456789/146823 en Symmetry, Integrability and Geometry: Methods and Applications Інститут математики НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
description The SU(2)-prolongation of the Hopf fibration S³→S² is a trivializable principal SU(2)-bundle. We present a noncommutative deformation of this bundle to a quantum principal SUq(2)-bundle that is not trivializable. On the other hand, we show that the SUq(2)-bundle is piecewise trivializable with respect to the closed covering of S² by two hemispheres intersecting at the equator.
format Article
author Hajac, P.M.
Zieliński, B.
spellingShingle Hajac, P.M.
Zieliński, B.
Nontrivial Deformation of a Trivial Bundle
Symmetry, Integrability and Geometry: Methods and Applications
author_facet Hajac, P.M.
Zieliński, B.
author_sort Hajac, P.M.
title Nontrivial Deformation of a Trivial Bundle
title_short Nontrivial Deformation of a Trivial Bundle
title_full Nontrivial Deformation of a Trivial Bundle
title_fullStr Nontrivial Deformation of a Trivial Bundle
title_full_unstemmed Nontrivial Deformation of a Trivial Bundle
title_sort nontrivial deformation of a trivial bundle
publisher Інститут математики НАН України
publishDate 2014
url http://dspace.nbuv.gov.ua/handle/123456789/146823
citation_txt Nontrivial Deformation of a Trivial Bundle / P.M. Hajac, B. Zieliński // Symmetry, Integrability and Geometry: Methods and Applications. — 2014. — Т. 10. — Бібліогр.: 14 назв. — англ.
series Symmetry, Integrability and Geometry: Methods and Applications
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first_indexed 2025-07-11T00:41:49Z
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fulltext Symmetry, Integrability and Geometry: Methods and Applications SIGMA 10 (2014), 031, 7 pages Nontrivial Deformation of a Trivial Bundle? Piotr M. HAJAC †‡ and Bartosz ZIELIŃSKI § † Instytut Matematyczny, Polska Akademia Nauk, ul. Śniadeckich 8, 00-956 Warszawa, Poland E-mail: pmh@impan.pl URL: http://www.impan.pl/~pmh/ ‡ Katedra Metod Matematycznych Fizyki, Uniwersytet Warszawski, ul. Hoża 74, 00-682 Warszawa, Poland ‡ Department of Computer Science, Faculty of Physics and Applied Informatics, University of Lódź, Pomorska 149/153 90-236 Lódź, Poland E-mail: bzielinski@uni.lodz.pl Received October 29, 2013, in final form March 03, 2014; Published online March 27, 2014 http://dx.doi.org/10.3842/SIGMA.2014.031 Abstract. The SU(2)-prolongation of the Hopf fibration S3 → S2 is a trivializable principal SU(2)-bundle. We present a noncommutative deformation of this bundle to a quantum principal SUq(2)-bundle that is not trivializable. On the other hand, we show that the SUq(2)-bundle is piecewise trivializable with respect to the closed covering of S2 by two hemispheres intersecting at the equator. Key words: quantum prolongations of principal bundles; piecewise trivializable quantum principal bundles 2010 Mathematics Subject Classification: 58B32 Dedicated to Marc A. Rieffel on the occasion of his 75th birthday 1 Introduction and preliminaries The goal of this paper is to show how a noncommutative deformation can turn a trivializable prin- cipal bundle into a nontrivializable quantum principal bundle. This is a peculiar phenomenon because noncommutative deformations usually preserve basic topological features of deformed objects, e.g. K-groups. On the other hand, this paper exemplifies the general theory of piecewise trivial principal comodule algebras developed in [7, 9]. Therefore we follow the notation, conventions and general setup employed therein. To make our exposition self-contained and easy to read, we often recall basic concepts and definitions. Let π : X →M be a principal G-bundle over M , and G′ be a subgroup of G. A G′-reduction of X → M is a subbundle X ′ ⊆ X over M that is a principal G′-bundle over M via the restriction of the G-action on X. Many important structures on manifolds can be formulated as reductions of their frame bundles. For instance, an orientation, a volume form and a metric on a manifold M correspond to reductions of the frame bundle FM to a GL+(n,R), SL(n,R) and O(n,R)-bundle, respectively. See [10] for more details. An operation inverse to a reduction of a principal bundle is a prolongation of a principal bundle. Let π : X → M be a principal G′-bundle over M , and let G′ be a subgroup of G. Define X ×G′ G := (X × G)/∼, where (x, g) ∼ (xh, h−1g), for all x ∈ X, g ∈ G and h ∈ G′. ?This paper is a contribution to the Special Issue on Noncommutative Geometry and Quantum Groups in honor of Marc A. Rieffel. The full collection is available at http://www.emis.de/journals/SIGMA/Rieffel.html mailto:pmh@impan.pl http://www.impan.pl/~pmh/ mailto:bzielinski@uni.lodz.pl http://dx.doi.org/10.3842/SIGMA.2014.031 http://www.emis.de/journals/SIGMA/Rieffel.html 2 P.M. Hajac and B. Zieliński Then π̂ : X ×G′ G −→M, [x, g] 7−→ π(x), is a G-bundle called the G-prolongation of X, with the G-action given by [x, g]h := [x, gh]. The bundle X →M is a G′-reduction of X ×G′ G→M . An interesting special case is when X = G and M = G/G′, that is the homogenous bundle case. It is easy to see that G ×G′ G → G/G′ is always a trivializable bundle. Indeed, the following G-equivariant bundle maps provide an explicit isomorphism and its inverse: f : G×G′ G −→ G/G′ ×G, [g1, g2] 7−→ ([g1], g1g2), f−1 : G/G′ ×G −→ G×G′ G, ([g], h) 7−→ [g, g−1h]. A quantum-group version of the trivializability of G ×G′ G → G/G′ can be easily checked mimicking the classical argument. In particular, the SUq(2)-prolongation SUq(2) × U(1) SUq(2) −→ S2 q of the standard quantum Hopf fibration is trivializable [5, p. 1104]. However, as the main result of this paper, we show that the SUq(2)-prolongation SU(2) × U(1) SUq(2) −→ S2 of the classical Hopf fibration is not trivializable. 1.1 Notation We work over the field C of complex numbers. The unadorned tensor product stands for the tensor product over this field. The comultiplication, counit and the antipode of a Hopf algebra H are denoted by ∆, ε and S, respectively. Our standing assumption is that S is invertible. A right H-comodule algebra P is a unital associative algebra equipped with an H-coaction ∆P : P → P ⊗H that is an algebra homomorphism. For a comodule algebra P , we call P coH := {p ∈ P |∆P (p) = p⊗ 1} the subalgebra of coaction-invariant elements in P . A left coaction on V is denoted by V ∆. For comultiplications and coactions, we often employ the Heynemann–Sweedler notation with the summation symbol suppressed: ∆(h) =: h(1) ⊗ h(2), ∆P (p) =: p(0) ⊗ p(1), V ∆(v) =: v(−1) ⊗ v(0). 1.2 Reductions and prolongations of principal comodule algebras Definition 1 ([4]). Let H be a Hopf algebra, P be a right H-comodule algebra and let B := P coH be the coaction-invariant subalgebra. The comodule algebra P is called principal iff: 1) P⊗BP 3 p⊗ q 7→ can(p⊗ q) := pq(0) ⊗ q(1) ∈ P ⊗H is bijective, 2) there exists a left B-linear right H-colinear splitting of the multiplication map B⊗P → P , 3) the antipode of H is bijective. Nontrivial Deformation of a Trivial Bundle 3 Here (1) is the Hopf–Galois (freeness) condition, (2) means equivariant projectivity of P , and (3) ensures a left-right symmetry of the definition (everything can be re-written for left comodule algebras). A particular class of principal comodule algebras is distinguished by the existence of a clea- ving map. A cleaving map is defined as a unital right H-colinear convolution-invertible map j : H → P . Comodule algebras admitting a cleaving map are called cleft. One can show that a cleaving map is automatically injective. However, in general, they are not algebra homomor- phisms. If j : H → P is a right H-colinear algebra homomorphism, then it is automatically convolu- tion-invertible and unital. A cleft comodule algebra admitting a cleaving map that is an algebra homomorphism is called a smash product. All commutative smash products reduce to the tensor algebra P coH ⊗H, so that smash products play the role of trivial bundles. Here a cleaving map is simply given by j(h) := 1 ⊗ h. A cleaving map defines a left action of H on P coH making it a left H-module algebra: h . p := j(h(1))pj −1(h(2)). Conversely, if B is a left H-module algebra, one can construct a smash product B oH by equipping the vector space B ⊗H with the multiplication (a⊗ h)(b⊗ k) := a (h(1) . b)⊗ h(2) k, a, b ∈ B, h, k ∈ H, and coaction ∆BoH := id⊗∆. Then again a cleaving map is simply given by j(h) := 1⊗ h. Definition 2 ([6, 8, 12]). Let P be a principal H-comodule algebra and J be a Hopf ideal of H such that H is a principal left H/J-comodule algebra. We say that an ideal I of P is a J-reduction of P if and only if the following conditions are satisfied: 1) I is an H/J-subcomodule of P , 2) P/I with the induced coaction is a principal H/J-comodule algebra, 3) (P/I)coH/J = P coH . Loosely speaking, J plays the role of the ideal of functions vanishing on a subgroup and I the ideal of functions vanishing on a subbundle. Thus H/J works as the algebra of the reducing sub- group, and P/I as the algebra of the reduced bundle. The coaction-invariant subalgebra P coH remains intact – the base space of a subbundle coincides with the base space of the bundle. If M is a right comodule over a coalgebra C and N is a left C-comodule, then we define their cotensor product as M2 C N := {t ∈M ⊗N | (∆M ⊗ id)(t) = (id⊗ N∆)(t)}. In particular, for a principal H ′-comodule algebra P and a Hopf algebra epimorphism H π→ H ′ making H a left H ′-comodule in the obvious way, one proves that the cotensor product P2H′H is a principal H-comodule algebra with the H-coaction defined by id⊗∆. We call the principal comodule algebra P2H′H the H-prolongation of P . 1.3 Piecewise triviality Definition 3 (cf. [7, Definition 3.6]). A family of surjective algebra homomorphisms {πi : P → Pi}i∈{1,...,N}, N ∈ N \ {0}, is called a covering iff 1) ⋂ i∈{1,...,N}Kerπi = 0, 2) The family of ideals (Kerπi)i∈{1,...,N} generates a distributive lattice with + and ∩ as meet and join respectively. 4 P.M. Hajac and B. Zieliński We recall now (cf. [7, Definition 3.8]) a quantum version of the notion of piecewise triviality of principal bundles (like local triviality, but with respect to closed subsets). Definition 4. An H-comodule algebra P is called piecewise trivial iff there exists a family {πi : P → Pi}i∈{1,...,N}, N ∈ N \ {0}, of surjective H-colinear maps such that: 1) the restrictions πi|P coH : P coH → P coH i form a covering, 2) the Pi’s are smash products (Pi ∼= P coH i oH as H comodule algebras). Assume also that the antipode of H is bijective. Then, as smash products are principal, it follows from [7, Theorem 3.3] that piecewise trivial comodule algebras are automatically principal. To emphasize this fact and stay in touch with the classical terminology, we frequently use the phrase “piecewise trivial principal comodule algebra”. Note also that the consequence of principality of P is that {πi : P → Pi}i∈{1,...,N} is a covering of P (see [9]). Definition 5 ([9]). Let {πi : P → Pi}i∈{1,...,N}, N ∈ N \ {0}, be a covering by right H-colinear maps of a principal right H-comodule algebra P such that the restrictions πi|P coH : P coH → P coH i also form a covering. A piecewise trivialization of P with respect to the covering {πi : P → Pi}i∈{1,...,N} is a family {ji : H → Pi}i∈{1,...,N} of right H-colinear alge- bra homomorphisms (cleaving maps). It is clear that a principal comodule algebra is piecewise trivial if and only if it admits a piecewise trivialization (see the preceding section). 1.4 The Peter–Weyl comodule algebra The Peter–Weyl comodule algebra (see [1] and references therein) extends the notion of re- gular functions in the C∗-algebra of a compact quantum group (linear combinations of matrix coefficients of the finite-dimensional corepresentations) to unital C∗-algebras equipped with a compact quantum group action. Definition 6 (cf. [11]). For a unital C∗-algebra A and a compact quantum group (H,∆), we say that an injective unital ∗-homomorphism δ : A→ A⊗min H is a coaction if and only if 1) (δ ⊗ id) ◦ δ = (id⊗∆) ◦ δ (coassociativity), 2) {δ(a)(1⊗ h) | a ∈ A, h ∈ H}cls = A ⊗ min H (counitality). Here ⊗min denotes the spatial tensor product of C∗-algebras and {·}cls stands for the closed linear span of a subset of a Banach space. We say that a compact quantum group acts on a unital C∗-algebra if there is a coaction in the aforementioned sense. Next, we denote by O(H) the dense Hopf ∗-subalgebra of H spanned by the matrix coeffi- cients of finite-dimensional corepresentations. We define the Peter–Weyl subalgebra of A [1] as PH(A) := {a ∈ A | δ(a) ∈ A⊗O(H)}. One shows that it is an O(H)-comodule algebra which is a dense ∗-subalgebra of A [11, 13]. The Peter–Weyl comodule algebra of functions on a compact Hausdorff space with an action of a compact group is principal if and only if the action is free [1, 2]. In other words, the Galois condition of Hopf–Galois theory holds if and only if we have a compact principal bundle. Nontrivial Deformation of a Trivial Bundle 5 2 The SUq(2)-prolongation of the classical Hopf fibration To fix the notation, let us recall definitions of the Hopf algebras O(U(1)) and O(SUq(2)), and the Peter–Weyl comodule algebra PC(U(1))(C(S3)) of functions on the classical sphere S3. For details on the latter algebra we refer the reader to [3]. Recall that the ∗-algebra O(U(1)) of polynomial functions on U(1) is generated by the unitary element u : U(1) 3 x 7→ x ∈ C, and can be equivalently defined as the algebra of Laurent polynomials in u subject to the relation u−1 = u∗. The Hopf algebra structure is given by ∆(u) := u⊗ u, ε(u) := 1 and S(u) := u−1. The algebra of polynomial functions on SUq(2) [14] is generated as a ∗-algebra by α and γ satisfying relations αγ = qγα, αγ∗ = qγ∗α, γγ∗ = γ∗γ, α∗α+ γ∗γ = 1, αα∗ + q2γγ∗ = 1, (1) where 0 < q ≤ 1. The Hopf algebra structure comes from the matrix U := ( α −qγ∗ γ α∗ ) , i.e. ∆(Uij) := ∑ k Uik ⊗ Ukj , S(Uij) := U∗ji, ε(Uij) := δij . The Hopf ∗-algebra epimorphism π : O(SUq(2)) −→ O(U(1)), π(α) := u, π(γ) := 0, (2) makes O(SUq(2)) into a left and right O(U(1))-comodule algebra via the left and right coactions (π⊗ id)◦∆ and (id⊗π)◦∆ respectively. For q = 1 the Hopf algebra O(SUq(2)) is commutative, and we denote its generators by a and c rather then α and γ. The Peter–Weyl comodule algebra PC(U(1))(C(S3)) is the subalgebra of C(SU(2)) that is the algebraic direct sum of the modules of continuous sections of the complex line bundles Ln, n ∈ Z, associated to the Hopf fibration: PC(U(1))(C(S3)) = ⊕ n∈Z Γ(Ln). We have the following proper inclusions of function algebras: O(SU(2)) ( PC(U(1))(C(S3)) ( C(S3). Next, recall that a, c : S3 → C are coordinate functions on S3 satisfying |a|2 + |c|2 = 1. The diagonal action of U(1) on S3 yielding the Hopf fibration dualizes to the O(U(1))-comodule algebra structure on PC(U(1))(C(S3)) given by a 7→ a⊗ u, c 7→ c⊗ u. Now we will describe the piecewise trivial structure of PC(U(1))(C(S3)). For brevity, we define ω := √ 2 1 + ||a|2 − |c|2| . Note that ω is an element of the coaction-invariant subalgebra PC(U(1))(C(S3))coO(U(1)) = Γ(L0), which we identify with C(S2). Let us also define the following ideals Ia, Ic ⊆ C(S2): Ia := { f ∈ C(S2) ∣∣ f(x) = 0 for all x ∈ S2 such that |a|2(x) ≤ 1/2 } , Ic := { f ∈ C(S2) ∣∣ f(x) = 0 for all x ∈ S2 such that |a|2(x) ≥ 1/2 } . It is well known (cf. [3]) that the canonical surjections C(S2) → C(S2)/Ii ∼= C(D), i = a, c, where D is the unit disk, form a covering, and that (1− ω2|a|2) ∈ Ia, (1− ω2|c|2) ∈ Ic. We also know [3, equation (3.4.57)] that( 1− ω2|a|2 )( 1− ω2|c|2 ) = 0. 6 P.M. Hajac and B. Zieliński The covering of PC(U(1))(C(S3)) can now be given by the canonical surjections in terms of Ia and Ic (cf. [3]): πa : PC(U(1))(C(S3)) −→ PC(U(1))(C(S3))/(IaPC(U(1))(C(S3))), πc : PC(U(1))(C(S3)) −→ PC(U(1))(C(S3))/(IcPC(U(1))(C(S3))). Indeed, since PC(U(1))(C(S3)) is a principal O(U(1))-comodule algebra with the coaction-inva- riant subalgebra C(S2), it follows from [7, Proposition 3.4] that the maps πi form a covering. A trivialization associated with the above covering is given by the following cleaving maps, which are clearly algebra homomorphisms: ja : O(U(1)) −→ PC(U(1))(C(S3))/(IaPC(U(1))(C(S3))), un 7−→ πa(ωa)n, jc : O(U(1)) −→ PC(U(1))(C(S3))/(IcPC(U(1))(C(S3))), un 7−→ πc(ωc) n. One can argue (cf. [3]) that fa : PC(U(1))(C(S3))/(IaPC(U(1))(C(S3))) ∼=−→ C(D)⊗O(U(1)), fc : PC(U(1))(C(S3))/(IcPC(U(1))(C(S3))) ∼=−→ C(D)⊗O(U(1)), (3) fi : x 7−→ πi(x(0))ji(Sx(1))⊗ x(2), i = a, c. To see this, first note that πa(C(S2)) ∼= C(D) ∼= πc(C(S2)). Then, for any n ∈ Z, fi(πi(Γ(Ln))) = πi(C(S2))⊗ un = C(D)⊗ un, i = a, c, whence fi(PC(U(1))(C(S3))) = C(D)⊗O(U(1)). Indeed, fi(πi(Γ(Ln))) ⊆ πi(C(S2))⊗un. On the other hand, consider an arbitrary element y ∈ C(D). Then there exist elements ya, yc ∈ C(S2) such that y = πa(ya) = πc(yc). Hence y ⊗ un = fz(πz(yzz nωn)), z = a, c. Here we adopt the convention that z−|n| := (z∗)|n|. Summarizing, PC(U(1))(C(S3)) is a piecewise trivial principal comodule algebra [3]. SinceO(SUq(2)) is a left principalO(U(1))-comodule algebra, by [9, Lemma 1.13] the cotensor product PC(U(1))(C(S3))�O(U(1))O(SUq(2)) is a piecewise trivial principal comodule algebra. Explicitly, the covering and trivializations inherited from PC(U(1))(C(S3)) make it piecewise trivial via the formulas: π̂i := πi ⊗ id, ĵi := (ji ◦ π ⊗ id) ◦∆O(SUq(2)), i = a, c. Using these formulas and the isomorphisms (3), one can check that the trivializable pieces of the comodule algebra PC(U(1))(C(S3))�O(U(1))O(SUq(2)) are isomorphic to C(D)⊗O(SUq(2)) (cf. [9, equation (1.8)]). Furthermore, as the comodule algebra PC(U(1))(C(S3))�O(U(1))O(SUq(2)) is a cotensor pro- duct, combining [9, Lemma 1.13] with [9, Theorem 1.5] yields that PC(U(1))(C(S3)) is a piecewise trivial (Kerπ)-reduction (see (2)) of PC(U(1))(C(S3))�O(U(1))O(SUq(2)). Theorem 1 (main result). The comodule algebra PC(U(1))(C(S3))�O(U(1))O(SUq(2)) is not iso- morphic to any smash product C(S2) oO(SUq(2)) comodule algebra. Nontrivial Deformation of a Trivial Bundle 7 Proof. Suppose that there exists a cleaving map O(SUq(2)) −→ PC(U(1))(C(S3))�O(U(1))O(SUq(2)) that is an algebra homomorphism. It is tantamount to the existence of a U(1)-equivariant algebra homomorphism f : O(SUq(2)) → PC(U(1))(C(S3)) [5, Proposition 4.1]. Let α and γ denote generators of O(SUq(2)), and a, c their classical counterparts. Since f([α, α∗]) = 0, it follows from (1) that f(γ) = 0 and f(α)f(α)∗ = 1. On the other hand, by the U(1)-equivariance, f(α) = f1a + f2c, for some f1, f2 ∈ C(S2). Furthermore, any continuous section of the Hopf line bundle L1 can be written as g1a + g2c for some g1, g2 ∈ C(S2). We can rewrite it as (g1a + g2c)f(α)∗f(α). Since (g1a + g2c)f(α)∗ ∈ C(S2), we conclude that f(α) spans Γ(L1) as a left C(S2)-module. Also, if gf(α) = 0 for some g ∈ C(S2), then g = gf(α)f(α∗) = 0. Hence f(α) is a basis of Γ(L1) contradicting its nonfreeness. � Acknowledgements The authors are grateful to Tomasz Brzeziński for discussions, and to the referees for care- ful proofreading of the manuscript. This work was partially supported by the NCN-grant 2011/01/B/ST1/06474. References [1] Baum P.F., De Commer K., Hajac P.M., Free actions of compact quantum groups of unital C∗-algebras, arXiv:1304.2812. 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Sci. 23 (1987), 117–181. http://arxiv.org/abs/1304.2812 http://arxiv.org/abs/1402.3024 http://arxiv.org/abs/math.DG/0701033 http://dx.doi.org/10.1016/j.crma.2003.11.009 http://arxiv.org/abs/math.KT/0306436 http://dx.doi.org/10.1016/j.geomphys.2011.12.008 http://arxiv.org/abs/1105.5897 http://dx.doi.org/10.1080/00927879908826704 http://dx.doi.org/10.4171/JNCG/88 http://dx.doi.org/10.4171/JNCG/88 http://arxiv.org/abs/0707.1344 http://arxiv.org/abs/1101.0201 http://dx.doi.org/10.1007/BF02099436 http://arxiv.org/abs/hep-th/9402069 http://dx.doi.org/10.1006/jabr.1998.7814 http://arxiv.org/abs/1003.5526 http://dx.doi.org/10.2977/prims/1195176848 http://dx.doi.org/10.2977/prims/1195176848 1 Introduction and preliminaries 1.1 Notation 1.2 Reductions and prolongations of principal comodule algebras 1.3 Piecewise triviality 1.4 The Peter–Weyl comodule algebra 2 The SUq(2)-prolongation of the classical Hopf fibration References