Abstract
We state and prove a general result establishing that T-duality, or the Connes–Thom isomorphism, simplifies the bulk–boundary correspondence, given by a boundary map in K-theory, in the sense of converting it to a simple geometric restriction map. This settles in the affirmative several earlier conjectures of the authors and provides a clear geometric picture of the correspondence. In particular, our result holds in arbitrary spatial dimension, in both the real and complex cases, and also in the presence of disorder, magnetic fields, and H-flux. These special cases are relevant both to string theory and to the study of the quantum Hall effect and topological insulators with defects in condensed matter physics.
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Notes
Quite often KR-theory groups, in the sense of Atiyah’s Real K-theory, are relevant, and these groups are defined for spaces with involutions. Such spaces are usually called “Real spaces”, which should not be confused with our usage of “real space” as synonymous with “position space”.
Although we concentrate here on the case where the boundary has codimension 1, our notation and arguments have been written to suggest a way to include higher-codimensional boundaries. The main differences lie in the parity of the K-groups linked by Connes–Thom maps and the fact that there can be Mackey obstructions for the boundary.
There may be no such symmetries even if the boundary occupies \(n\ge 1\) dimensions; for instance, it may not be completely straight. Generally speaking, the collection of boundary symmetries determine what topological invariants may be associated with it, and the more symmetries there are, the more boundary invariants are available.
If \(\alpha \) defined a character of L, then the “periodicity” would give Bloch-type functions.
\(A_\Theta \) can be defined as the universal \(C^*\)-algebra generated by d unitaries \(U_1,\ldots ,U_d\) subject to \(U_kU_j={\mathrm{exp}}(2\pi i\Theta _{jk})U_jU_k\), where we regard \(\Theta \) as a skew-symmetric \(d\times d\) matrix.
We have switched convention for induced algebras in this Appendix compared to the main text. This is to make closer contact to Paschke’s original work, and the effect is that \(\alpha ^{-1}\) is replaced by \(\alpha \).
There is no loss of generality in assuming that \({\mathcal {A}}\) is unital and that p is in \(\mathrm {Ind}({\mathcal {A}},\alpha )\) rather than in \(\mathrm {Ind}({\mathcal {A}},\alpha )\otimes M_n\), see [37].
References
Atiyah, M.F., Donnelly, H., Singer, I.M.: Eta invariants, signature defects of cusps, and values of L-functions. Ann. Math. 118, 131–177 (1983)
Bellissard, J., van Elst, A., Schulz-Baldes, H.: The noncommutative geometry of the quantum Hall effect. J. Math. Phys. 35(10), 5373–5451 (1994)
Bellissard, J.: \(K\)-theory of \(C^*\)-algebras in solid state physics. In: Statistical Mechanics and Field Theory: Mathematical Aspects (Groningen, 1985), Lecture Notes in Physics, vol. 257, pp. 99–156. Springer, Berlin (1986)
Bouwknegt, P., Evslin, J., Mathai, V.: T-duality: topology change from \(H\)-flux. Commun. Math. Phys. 249, 383–415 (2004)
Bramwell, S.T., et al.: Measurement of the charge and current of magnetic monopoles in spin ice. Nature 461, 956–959 (2009)
Chang, M.-C., Niu, Q.: Berry phase, hyperorbits, and the Hofstadter spectrum: semiclassical dynamics in magnetic Bloch bands. Phys. Rev. B 53(11), 7010–7023 (1996)
Connes, A.: An analogue of the Thom isomorphism for crossed products of a \(C^*\)-algebra by an action of \({{\mathbb{R}}}\). Adv. Math. 39, 31–55 (1981)
Cuntz, J.: \(K\)-theory and \(C^*\)-algebras. In: Algebraic \(K\)-Theory, Number Theory, Geometry and Analysis, Lecture Notes in Mathematics, vol. 1046, pp. 55–79, Springer, Berlin (1984)
Cuntz, J., Meyer, R., Rosenberg, J.: Topological and bivariant \(K\)-theory. Birkhäuser, Basel (2007)
Echterhoff, S.: A categorical approach to imprimitivity theorems for \(C^*\)-dynamical systems. Mem. Am. Math. Soc. 805 (2006). arXiv:math/0205322
Echterhoff, S., Nest, R., Oyono-Oyono, H.: Principal non-commutative torus bundles. Proc. Lond. Math. Soc. 99(3), 1–31 (2009)
Echterhoff, S., Williams, D.P.: Locally inner actions on \(C_0(X)\)-algebras. J. Oper. Theory 45, 131–160 (2001)
Fack, T., Skandalis, G.: Connes’ analogue of the Thom isomorphism for the Kasparov groups. Invent. Math. 64(1), 7–14 (1981)
Freed, D.S., Moore, G.W.: Twisted equivariant matter. Ann. Henri Poincaré 14(8), 1927–2023 (2013)
Gawedzki, K.: Bundle gerbes for topological insulators. Banach Center Publications. arXiv:1512.01028 (in press)
Green, P.: The local structure of twisted covariance algebras. Acta Math. 140, 191–250 (1978)
Hannabuss, K.C.: Representations of nilpotent locally compact groups. J. Funct. Anal. 34, 146–165 (1979)
Hannabuss, K.C., Mathai, V.: Noncommutative principal torus bundles via parametrised strict deformation quantization. AMS Proc. Symp. Pure Math. 81, 133–148 (2010). arXiv:0911.1886
Hannabuss, K.C., Mathai, V.: Parametrised strict deformation quantization of \(C^*\)-bundles and Hilbert \(C^*\)-modules. J. Aust. Math. Soc. 90(1), 25–38 (2011). arXiv:1007.4696
Hannabuss, K.C., Mathai, V., Thiang, G.C.: T-duality simplifies bulk-boundary correspondence: the parametrised case. Adv. Theor. Math. Phys. 20(5), 1193–1226 (2016). arXiv:1510.04785
Kane, C.L., Mele, E.J.: Quantum spin Hall effect in graphene. Phys. Rev. Lett. 95(22), 226801 (2005)
Kane, C.L., Mele, E.J.: \({\mathbb{Z}}_2\) topological order and the quantum spin Hall effect. Phys. Rev. Lett. 95(14), 146802 (2005)
Kellendonk, J., Richter, T., Schulz-Baldes, H.: Edge current channels and Chern numbers in the integer quantum Hall effect. Rev. Math. Phys. 14(1), 87–119 (2002)
Kitaev, A.: Periodic table for topological insulators and superconductors. AIP Conf. Proc. 1134(1), 22–30 (2009)
Kleinert, H.: Gauge Fields in Condensed Matter, vol. 2. World Scientific, Singapore (1989)
Kleppner, A.: Multipliers on abelian groups. Math. Ann. 158, 11–34 (1965)
Lawson, H., Michelsohn, M.-L.: Spin Geometry, Princeton Mathematical Series, vol. 38. Princeton University Press, Princeton (1989)
Lee, S.T., Packer, J.: Twisted group algebras for two-step nilpotent and generalized discrete Heisenberg groups. J. Oper. Theory 33, 91–124 (1995)
Marcolli, M.: Solvmanifolds and noncommutative tori with real multiplication. Commun. Number Theory Phys. 2(2), 421–476 (2008)
Mathai, V., Rosenberg, J.: T-duality for torus bundles via noncommutative topology. Commun. Math. Phys. 253, 705–721 (2005). arXiv:hep-th/0401168
Mathai, V., Rosenberg, J.: T-duality for torus bundles with H-fluxes via noncommutative topology, II. The high-dimensional case and the T-duality group. Adv. Theor. Math. Phys. 10, 123–158 (2006). arXiv:hep-th/0508084
Mathai, V., Thiang, G.C.: T-duality of topological insulators. J. Phys. A Math. Theor. (Fast Track Commun.) 48(42), 42FT02 (2015). arXiv:1503.01206
Mathai, V., Thiang, G.C.: T-duality simplifies bulk-boundary correspondence. Commun. Math. Phys. 345(2), 675–701 (2016). arXiv:1505.05250
Mathai, V., Thiang, G.C.: T-duality simplifies bulk-boundary correspondence: some higher dimensional cases. Ann. Henri Poincaré 17(12), 3399–3424 (2016). arXiv:1506.04492
Mathai, V., Thiang, G.C.: Differential topology of semimetals. Commun. Math. Phys. 355(2), 561–602 (2017)
Packer, J., Raeburn, I.: Twisted crossed products of \(C^*\)-algebras. Math. Proc. Cambridge Philos. Soc. 106, 293–311 (1989)
Paschke, W.: On the mapping torus of an automorphism. Proc. Am. Math. Soc. 88, 481–485 (1983)
Pimsner, M., Voiculescu, D.: Exact sequences for \(K\)-groups and \(EXT\)-groups of certain cross-product \(C^*\)-algebras. J. Oper. Theory 4, 93–118 (1980)
Prodan, E., Schulz-Baldes, H.: Bulk and Boundary Invariants for Complex Topological Insulators: From \(K\)-Theory to Physics. Mathematical Physics Studies. Springer, Cham (2016)
Raeburn, I., Rosenberg, J.: Crossed products of continuous-trace \(C^*\) algebras by smooth actions. Trans. Am. Math. Soc. 305, 1–45 (1988)
Raeburn, I., Williams, D.: Morita Equivalence and Continuous-Trace \(C^*\)-Algebras. Mathematical Surveys and Monographs. American Mathematical Society, Providence (1998)
Ran, Y., Zhang, Y., Vishwanath, A.: One-dimensional topologically protected modes in topological insulators with lattice dislocations. Nat. Phys. 5, 298–303 (2009)
Ray, M.W., Ruokokoski, E., Kandel, S., Möttönen, M., Hall, D.S.: Observation of Dirac monopoles in a synthetic magnetic field. Nature 505, 657–660 (2014)
Rieffel, M.A.: Connes’ analogue for crossed products of the Thom isomorphism. Contemp. Math. 10, 143–154 (1981)
Rieffel, M.A.: Strong Morita equivalence of certain transformation group \(C^*\)-algebras. Math. Ann. 222(1), 7–22 (1976)
Rørdam, M., Larsen, M., Laustsen, M.: An Introduction to \(K\)-theory for \(C^*\)-algebras. London. Math. Soc. Student Texts 19. Cambridge Univ. Press, Cambridge (2000)
Rosenberg, J.: Some results on cohomology with Borel cochains, with applications to group actions on operator algebras. Oper. Theory Adv. Appl. 17, 301–330 (1986)
Rosenberg, J.: \(C^*\)-algebras, positive scalar curvature, and the Novikov conjecture–III. Topology 25(3), 319–336 (1986)
Schröder, H.: \(K\)-Theory for Real \(C^*\)-Algebra and Applications. Pitman Research Notes in Mathemathical Series. Longman, Harlow (1993)
Scott, P.: The geometries of 3-manifolds. Bull. Lond. Math. Soc. 15(5), 401–487 (1983)
Takai, H.: On a duality for crossed product algebras. J. Funct. Anal. 19, 25–39 (1975)
Thiang, G.C.: On the \(K\)-theoretic classification of topological phases of matter. Ann. Henri Poincaré 17(4), 757–794 (2016)
Wegge-Olsen, N.E.: \(K\)-Theory and \(C^*\)-Algebras. Oxford University Press, Oxford (1993)
Wu, Y.-S., Zee, A.: Cocycles and magnetic monopoles. Phys. Lett. B 152, 98–102 (1985)
Acknowledgements
Varghese Mathai and Guo Chuan Thiang were supported by the Australian Research Council via ARC Discovery Project Grants DP150100008, FL170100020, and DE170100149, respectively. The authors thank the Erwin Schrödinger Institute (ESI), Vienna, for its hospitality during the ESI Program on Higher Structures in String Theory and Quantum Field Theory, when part of this research was completed.
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Appendices
Appendix A: Paschke’s map and the Connes–Thom isomorphism
This appendix explains why Paschke’s map [37] is, up to a sign convention, the Connes–Thom isomorphism [7] composed with an isomorphism from Green’s imprimitivity theorem. This result belongs to a family of ideas which can be found in [7,8,9, 37] and may be known to experts, but we provide a detailed argument for the reader’s reference. The Paschke map is explicitly defined for each \({\mathbb {Z}}\)-algebra \(({\mathcal {A}},\alpha )\), whereas the Connes–Thom map is more abstractly defined. As we will see, there is an analogous abstract characterization of the Paschke map, which determines its formula uniquely.
1.1 Generalities on Connes–Thom isomorphism
Recall from [7] that the Connes–Thom isomorphism is a natural transformation between the functors \(K_\bullet (\cdot )\) and \(K_{\bullet +1}((\cdot )\rtimes {\mathbb {R}})\), \(\bullet \in {\mathbb {Z}}_2\), i.e. it assigns to every \({\mathbb {R}}\)-\(C^*\)-algebra \(({\mathscr {A}},\alpha )\) an isomorphism \(\phi ^\bullet _\alpha : K_\bullet ({\mathscr {A}})\rightarrow K_{\bullet +1}({\mathscr {A}}\rtimes _\alpha {\mathbb {R}})\), such that for any morphism \(\rho :({\mathscr {A}},\alpha )\rightarrow (\mathscr {B},\beta )\), the following diagram commutes:
Here, \(\rho \rtimes {\mathbb {R}}\) is the morphism of crossed products induced by the equivariant map \(\rho \). Furthermore, Connes shows that \(\phi _\alpha ^\bullet \) is an isomorphism, which is determined uniquely by this naturality property together with a normalization condition (for \(({\mathcal {A}},\alpha )=({{\mathbb {C}}},{\mathrm {id}})\)) and compatibility with suspensions.
1.2 The analogous axioms for Paschke’s map
If \(\rho :({\mathcal {A}},\alpha )\rightarrow ({\mathcal {B}},\beta )\) is a morphism of \({\mathbb {Z}}\)-\(C^*\)-algebras (not necessarily unital), the induction functor \(\mathrm {Ind}:=\mathrm {Ind}_{\mathbb {Z}}^{\mathbb {R}}(\cdot )\) gives a morphism of induced algebras \(\tilde{\rho }:\mathrm {Ind}({\mathcal {A}},\alpha )\rightarrow \mathrm {Ind}({\mathcal {B}},\beta )\) which is equivariant for the respective translation actions \(\tau ^\alpha , \tau ^\beta \) of \({\mathbb {R}}\). Elements of \(\mathrm {Ind}({\mathcal {A}},\alpha )\) are viewed either as bounded continuous functions \(f:{\mathbb {R}}\rightarrow {\mathcal {A}}\) satisfying an equivariance conditionFootnote 6, \(f(x+1)=\alpha (f(x)), x\in {\mathbb {R}}\), or alternatively, continuous \(f:[0,1]\rightarrow {\mathcal {A}}\) such that \(f(1)=\alpha (f(0))\) (the mapping torus). The translation action \(\tau ^\alpha \) of \({\mathbb {R}}\) on \(\mathrm {Ind}({\mathcal {A}},\alpha )\) is \((\tau ^\alpha _t f)(s)=f(s+t), s,t\in {\mathbb {R}}\).
Let \(S\alpha \) be the suspended \({\mathbb {Z}}\)-action on \(S{\mathcal {A}}\) (acting by \(\alpha \) on \({\mathcal {A}}\) and trivially on the suspension variable). Note that \(S(\mathrm {Ind}({\mathcal {A}},\alpha ))\cong \mathrm {Ind}(S{\mathcal {A}},S\alpha )\) and \(S({\mathcal {A}}\rtimes _\alpha {\mathbb {Z}})\cong S{\mathcal {A}}\rtimes _{S\alpha }{\mathbb {Z}}\), and write \(S^\bullet _{(\cdot )}\) for the natural suspension isomorphisms \(K_\bullet (\cdot )\rightarrow K_{\bullet -1}(S(\cdot ))\).
For \(\bullet \in {\mathbb {Z}}_2\), let \(\gamma ^\bullet \) be a natural transformation of the functors \(({\mathcal {A}},\alpha )\mapsto K_\bullet (\mathrm {Ind}({\mathcal {A}},\alpha ))\) and \(({\mathcal {A}},\alpha )\mapsto K_{\bullet +1}({\mathcal {A}}\rtimes _\alpha {\mathbb {Z}})\) from \({\mathbb {Z}}\)-algebras to abelian groups, satisfying the following three axioms:
Axiom A.1
(Normalization) If \(({\mathcal {A}},\alpha )=({{\mathbb {C}}},{\mathrm {id}})\), then \(\gamma ^0_{{\mathrm {id}}}:K_0(C({\mathbb {R}}/{\mathbb {Z}}))=K_0(C({\mathbb {T}}))\rightarrow K_1(C^*({\mathbb {Z}}))\) takes \([1_{C({\mathbb {T}})}]\) to the (Bott) generator [b] of \(K_1(C^*({\mathbb {Z}}))\) corresponding to \(1\in {\mathbb {Z}}\) regarded as an element of \(C^*({\mathbb {Z}})\).
Axiom A.2
(Naturality) If \(\rho :({\mathcal {A}},\alpha )\rightarrow ({\mathcal {B}},\beta )\) is a morphism of \({\mathbb {Z}}\)-algebras, then the following diagram commutes:
Axiom A.3
(Suspension) \(\gamma \) is compatible with S in the sense that
Proposition A.4
There is a unique \(\gamma \) satisfying Axioms A.1–A.3.
Proof
Outline: We use a modification of Connes’ argument for the uniqueness of \(\phi \). Axiom A.3 and Bott periodicity ensure that we only need to look at \(\gamma ^0\) (which we will simply denote by \(\gamma \) subsequently). We need to show that \(\gamma _\alpha [p]\in K_1({\mathcal {A}}\rtimes _\alpha {\mathbb {Z}})\) is uniquely determined for any projection \(p\equiv \{p_\theta \}_{\theta \in [0,1]}\) in \(\mathrm {Ind}({\mathcal {A}},\alpha )\). The basic idea is to construct a \({\mathbb {Z}}\)-action \(\alpha '\), exterior equivalent to \(\alpha \), which fixes \(p_0\). Furthermore, the new induced algebra \(\mathrm {Ind}({\mathcal {A}},\alpha ')\), with its translation action \(\tau ^{\alpha '}\), is \({\mathbb {R}}\)-equivariantly isomorphic to the original \(\mathrm {Ind}_{\alpha }{\mathcal {A}}\) with a modified action \(\tau '\), where \(\tau '\) is exterior equivalent to the original \(\tau ^\alpha \) and fixes p. Thus, the projection \(p'\in \mathrm {Ind}({\mathcal {A}},\alpha ')\) corresponding to \(p\in \mathrm {Ind}({\mathcal {A}},\alpha )\) under this isomorphism is itself translation invariant under \(\tau ^{\alpha '}\). Then, the Axioms determine what \(\gamma _{\alpha '}[p']\) has to be. Finally, we need to argue that the modification \(\alpha \mapsto \alpha '\) can be assumed because the above exterior equivalences determine unique maps, consistent with the Axioms, which yield the desired \(\gamma _\alpha [p]\) from \(\gamma _{\alpha '}[p']\).
Details: As in [7], we may assume without loss that \({\mathcal {A}}\) is unital and \(p\in \mathrm {Ind}({\mathcal {A}},\alpha )\). By [7] Proposition 4 (c.f. [9] Lemma 10.16, [44]), we may also assume that on \(\mathrm {Ind}({\mathcal {A}},\alpha )\) there is an action \({\mathbb {R}}\)-action \(\tau '\), exterior equivalent to \(\tau ^\alpha \), which fixes p. Let \(U\equiv \{U_t\}_{t\in {\mathbb {R}}}\) be the 1-cocycle on \(\mathrm {Ind}({\mathcal {A}},\alpha )\) which relates \(\tau ^\alpha \) and \(\tau '\) via \(\tau '_t=\mathrm {Ad}(U_t)\circ \tau ^\alpha _t\). Thus, \(\{U_t\}_{t\in {\mathbb {R}}}\) satisfies the cocycle condition and equivariance condition,
Define the modified \({\mathbb {Z}}\)-action \(\alpha '\) on \({\mathcal {A}}\) via
We can verify, from (31), that the assignment \(u:n\mapsto U_n(0)=:u_n,\, n\in {\mathbb {Z}}\) defines a unitary 1-cocycle \(\{u_n\}_{n\in {\mathbb {Z}}}\) on \(({\mathcal {A}},\alpha )\), i.e. \(u_{m+n}=u_m\alpha ^m(u_n)\). Thus, \({\mathcal {A}}\rtimes _{\alpha '}{\mathbb {Z}}\cong {\mathcal {A}}\rtimes _\alpha {\mathbb {Z}}\) (a canonical isomorphism \(\varphi _u\) is given in Lemma A.5 later).
Since \(\tau '_1=\mathrm {Ad}(U_1)\circ \tau ^\alpha _1\) fixes p, it follows that \(p_0:=p(0)\in {\mathcal {A}}\) fixed by \(\alpha '\). Define the isomorphism \(\Psi _U:\mathrm {Ind}({\mathcal {A}},\alpha )\rightarrow \mathrm {Ind}({\mathcal {A}},\alpha ')\) by
We can verify that \(\Psi _Uf\) does satisfy \(\alpha '\)-equivariance and intertwines \(\tau '\) on \(\mathrm {Ind}({\mathcal {A}},\alpha )\) with the new translation action \(\tau ^{\alpha '}\) on \(\mathrm {Ind}({\mathcal {A}},\alpha ')\), i.e. \((\tau ^{\alpha '}_t(\Psi _U f))= (\Psi _U(\tau '_t f))\).
Observe that \(p'(\theta )=p'_0=p_0\) since \(p'=\Psi _U(p)\) is fixed by \(\tau ^{\alpha '}\). The homomorphism
is \({\mathbb {Z}}\)-equivariant, and we write \(\tilde{\omega }\) for the corresponding inflated map \(\tilde{\omega }:C({\mathbb {T}})\cong \mathrm {Ind}({{\mathbb {C}}},{\mathrm {id}})\rightarrow \mathrm {Ind}({\mathcal {A}},\alpha ')\). Note that
so \(p'=\tilde{\omega }(1_{C({\mathbb {T}})})\). Then naturality and normalization mean that \(\gamma _{\alpha '}[p']\) must be determined by the equation
Corollary A.7 gives the details of how \(\gamma [p]\) is obtained from \(\gamma _{\alpha '}[p']\). \(\square \)
1.2.1 Connes’ \(2\times 2\) matrix trick
Lemma A.5
(c.f. [7] Lemma 2) Let \(\alpha , \alpha '\) be exterior equivalent \({\mathbb {Z}}\)-actions on \({\mathcal {A}}\) related by a unitary 1-cocycle \({\mathbb {Z}}\ni n \mapsto u_n \in U{\mathcal {M}}{\mathcal {A}}\). Then
is a \({\mathbb {Z}}\)-action on \(M_2({\mathcal {A}})\) which restricts to \(\alpha \) in the top-left corner and to \(\alpha '\) in the bottom-right corner. Let \(\iota , \iota '\) be the equivariant inclusions of \({\mathcal {A}}\) into their respective corners in \(M_2({\mathcal {A}})\). There is a unique isomorphism \(\varphi _u:{\mathcal {A}}\rtimes _\alpha {\mathbb {Z}}\rightarrow {\mathcal {A}}\rtimes _{\alpha '}{\mathbb {Z}}\) such that \((\iota '\rtimes {\mathbb {Z}})(\varphi _u(y))=\mathrm {Ad}(\begin{pmatrix} 0 &{}\quad 1 \\ 1 &{}\quad 0\end{pmatrix})[(\iota \rtimes {\mathbb {Z}})(y)]\) for all \(y\in {\mathcal {A}}\rtimes _\alpha {\mathbb {Z}}\).
Similarly, there are inclusions \(\tilde{\iota }, \tilde{\iota '}\) of the induced algebras into the respective corners of \(\mathrm {Ind}_\kappa M_2({\mathcal {A}})\). Let \(\tau ^\alpha , \tau '\) be the exterior equivalent \({\mathbb {R}}\)-actions on \(\mathrm {Ind}({\mathcal {A}},\alpha )\) as in the proof of Proposition A.4, related by the 1-cocycle \(\{U_t\}_{t\in {\mathbb {R}}}\). A straightforward computation shows:
Lemma A.6
Define \(X\in \mathrm {Ind}_{\kappa } M_2({\mathcal {A}})\) by
Then the isomorphism \(\Psi _U\) satisfies \(\tilde{\iota '}(\Psi _U(f))=\mathrm {Ad}(X)[\tilde{\iota }f], f\in \mathrm {Ind}({\mathcal {A}},\alpha )\).
Corollary A.7
Suppose \(\gamma \) satisfies Axioms A.1–A.3, and \(\alpha , \alpha ', U\) are as above. Then \(\gamma ^\bullet _{\alpha '}=(\varphi _u)_*\circ \gamma ^\bullet _\alpha \circ (\Psi _U^{-1})_*\).
Proof
Recall that inner automorphisms induce the identity map in K-theory. Thus, Lemmas A.5 and A.6 show that \((\iota \rtimes {\mathbb {Z}})_*=(\iota '\rtimes {\mathbb {Z}})_*\circ (\varphi _u)_*\) and \(\tilde{\iota }_*=\tilde{\iota '}_*\circ (\Psi _U)_*\). Using the naturality axiom, and dropping the superscript \({}^\bullet \) for now,
so injectivity of \((\iota '\rtimes {\mathbb {Z}})_*\) (see [7] Proposition 2–3) gives the required result. \(\square \)
1.3 Paschke’s isomorphisms
Paschke’s isomorphisms [37]
are first defined for unital \({\mathcal {A}}\) and \(\bullet =0\) on [p], by exhibiting the existence of a path of unitaries \(\theta \mapsto w_\theta \in {\mathcal {A}}\) such that
In particular, \(p_1=\mathrm {Ad}(w_1)(p_0)\). Then \(\gamma ^{0,\mathrm {Paschke}}_\alpha [p]\) is defined to be
where \(L\in {\mathcal {M}}({\mathcal {A}}\rtimes _\alpha {\mathbb {Z}})\) is the unitary implementing \(\alpha \) (i.e. \(\alpha (a)=LaL^*, a\in {\mathcal {A}}\)), with this map shown to be well-defined in K-theory.Footnote 7
The \(\bullet =1\) case is defined by compatibility with suspensions. Since \(\gamma ^{0,\mathrm {Paschke}}_\alpha \) may be expressed using representative projections and unitaries (rather than their K-theory classes), it is easy to see that the naturality Axiom A.2 is satisfied. It is also clear that normalization Axiom A.1 is satisfied up to a minus sign.
On the other hand, there is a commutative diagram due to the Connes–Thom natural isomorphisms,
Composing \(\phi _{\tau ^\alpha }^\bullet \) with the natural K-theory isomorphisms
given by the Morita equivalence \(\mathrm {Ind}({\mathcal {A}},\alpha )\rtimes _{\tau ^\alpha }{\mathbb {R}}\sim _{\mathrm{M.E.}}{\mathcal {A}}\rtimes _\alpha {\mathbb {Z}}\) (this is a special case of Green’s imprimitivity theorem [16]), we obtain another \(\gamma \) satisfying Axioms A.1–A.3: The normalization axiom follows from the fact that \(\phi _{\tau ^{{\mathrm{id}}}}\) is an isomorphism, so there is only one possibility (apart from a sign choice) for \(M_{\mathrm{id}}^{0,{\mathrm{Green}}}\circ \phi _{\tau ^{\mathrm{id}}}:{\mathbb {Z}}[1_{C({\mathbb {T}})}]\rightarrow {\mathbb {Z}}[b]\). Compatibility with suspensions is inherited from the Connes–Thom map, while naturality follows from naturality of implementing the Morita equivalence (see [10] Chapter 4). By Proposition A.4, we have
Theorem A.8
The map \(\gamma ^{\bullet ,\,{{{\mathrm{Paschke}}}}}_\alpha :K_\bullet (\mathrm {Ind}({\mathcal {A}},\alpha ))\rightarrow K_{\bullet +1}({\mathcal {A}}\rtimes _\alpha {\mathbb {Z}})\) is, up to a sign, the composition \(M_\alpha ^{\bullet +1,\,{\mathrm{Green}}}\circ \phi ^\bullet _{\tau ^\alpha }\).
1.3.1 Paschke’s unitaries and Connes’ cocycle
Given a \(p\in \mathrm {Ind}({\mathcal {A}},\alpha )\), we may start from Connes’ cocycle \(\{U_t\}_{t\in {\mathbb {R}}}\) in (31) above and obtain a path of unitaries \(w_\theta :=U^*_\theta (0), \theta \in [0,1]\) in \({\mathcal {A}}\). Then \(w_0=1\) and
thus \(\{w_\theta \}_{\theta \in [0,1]}\) is precisely a Paschke path whose existence was proved in [37].
Conversely, given a Paschke path \(\{w_\theta \}_{\theta \in [0,1]}\) such that \(w_0=1\) and \(\mathrm {Ad}(w_\theta )(p_0)=p_\theta \), we can reconstruct Connes’ cocycle for the action \(\tau ^\alpha \) on \(\mathrm {Ind}({\mathcal {A}},\alpha )\) as follows. Regard \(p\in \mathrm {Ind}({\mathcal {A}},\alpha )\) as a projection-valued function \({\mathbb {R}}\rightarrow {\mathcal {A}}\) through the equivariance condition \(p(s)\equiv p_s=\alpha (p_{s-1}), s\in {\mathbb {R}}\). Similarly, extend Paschke’s \(w:[1,0]\mapsto {\mathcal {A}}\) to a continuous unitary function \(w:{\mathbb {R}}\ni s\mapsto w_s\in {\mathcal {A}}\) by the recursion relation \(w_s=\alpha (w_{s-1})\cdot w_1\). It is easy to check that \(p_s=\mathrm {Ad}(w_s)(p_0)\) for all \(s\in {\mathbb {R}}\) and that \(n\mapsto w_n\) defines a 1-cocycle for \(({\mathcal {A}},\alpha )\). The projection \(p_0\) is then fixed by \(\alpha '_n=\mathrm {Ad}(w^*_n)\circ \alpha , n\in {\mathbb {Z}}\), since
The assignment \(t\mapsto U_t\in \mathrm {Ind}({\mathcal {A}},\alpha )\) defined by
is the desired Connes 1-cocycle for \((\mathrm {Ind}({\mathcal {A}},\alpha ),\tau ^\alpha )\); we can verify that each \(U_t\) is \(\alpha \)-equivariant and satisfies the cocycle condition. If we define the \({\mathbb {R}}\)-action \(\tau '\) on \(\mathrm {Ind}({\mathcal {A}},\alpha )\) by \(\tau '_t=\mathrm {Ad}(U_t)\circ (\tau ^\alpha _t)\), we find that the projection p is now fixed by \(\tau '\).
1.4 Paschke’s formula from axioms
Recall that \(\gamma ^0_\alpha [p]\) can be computed by passing to \(\alpha '\), using \(\gamma ^0_\alpha [p]=(\varphi _u^{-1})_*\circ \gamma ^0_{\alpha '}\circ (\Psi _U)_*[p]\). In (34), we saw that \(\gamma ^0_{\alpha '}\circ (\Psi _U)_*[p]=\gamma ^0_{\alpha '}[p']=(\omega \rtimes {\mathbb {Z}})_*[b].\) Note that even if \({\mathcal {A}}\) is unital, the homomorphism \(\omega \) (and thus \(\omega \rtimes {\mathbb {Z}}\)) is nonunital in general, so the induced map \((\omega \rtimes {\mathbb {Z}})_*\) in \(K_1\) is slightly tricky to compute (c.f. Proposition 8.1.6 of [46]). Namely, we have to append a formal unit \(\mathbf{1}\) to \(C({\mathbb {T}})\) and \({\mathcal {A}}\rtimes _{\alpha '}{\mathbb {Z}}\), replace [b] by \([\mathbf{1}-1_{C({\mathbb {T}})}+b]\), then compute \((\omega \rtimes {\mathbb {Z}})_*\) using the unital extension \((\omega \rtimes {\mathbb {Z}})^+:C({\mathbb {T}})^+\rightarrow ({\mathcal {A}}\rtimes _{\alpha '}{\mathbb {Z}})^+\). This gives
and mapping back to unitaries in \(\mathrm {Ind}({\mathcal {A}},\alpha ')\), we obtain
Finally, recall that the isomorphism \(\varphi _u\) implements the isomorphism \({\mathcal {A}}\rtimes _\alpha {\mathbb {Z}}\cong {\mathcal {A}}\rtimes _{\alpha '}{\mathbb {Z}}\) induced by the exterior equivalence \(\alpha '_n=\mathrm {Ad}(w^*_n)\circ \alpha _n\), so it effects \(w_1^*L\mapsto L'\). Thus,
which, up to a sign, concides with \(\gamma ^{0,{{{\mathrm{Paschke}}}}}_\alpha [p]\).
1.5 The real \(C^*\)-algebra case
A general reference for the K-theory of real \(C^*\)-algebras is [49]. The Connes–Thom isomorphisms and Pimsner–Voiculescu exact sequence also hold for real \(C^*\)-algebras \({\mathcal {A}}\) and real crossed products, see [48, 49]. Similarly, Paschke’s map \(\gamma ^{0,{{{{{\mathrm{Paschke}}}}}}}_\alpha \) still makes sense on real \({\mathbb {Z}}\)-algebras \(({\mathcal {A}},\alpha )\). We can then repeat the arguments in this appendix to obtain the real version of Theorem A.8. The only significant change is in the normalization axiom, and in taking \(\bullet \in {\mathbb {Z}}_8\) rather than in \({\mathbb {Z}}_2\).
Recall that \({\mathbb {C}}\rtimes _{\mathrm{id}}{\mathbb {Z}}=C_{\mathbb {R}}^*({\mathbb {Z}})\cong C({\mathbb {T}};\varsigma )\) where \(\varsigma \) is the involution \(\theta \mapsto -k\theta \) on \({\mathbb {T}}=\widehat{{\mathbb {Z}}}\) inherited from complex conjugation of characters (parametrized by \(\theta \in [0,1]\)), and \(C({\mathbb {T}};\varsigma )\) is the real \(C^*\)-algebra of continuous functions \(f\in {\mathbb {T}}\rightarrow {{\mathbb {C}}}\) such that \(\overline{f(\theta )}=f(-\theta )\). These functions are precisely the ones with real Fourier coefficients. It is known (pp. 40 of [49]) that \(K_1(C({\mathbb {T}};\varsigma ))\cong {\mathbb {Z}}[z]\oplus {\mathbb {Z}}_2[-1_{C({\mathbb {T}},\varsigma )}]\), where z denotes the unitary function \(\theta \mapsto e^{2\pi i\theta }\) with winding number 1. Furthermore, [z] is the Bott element implementing (1,1) periodicity in KR-theory (c.f. Theorem 1.5.4 of [49], Theorem 10.3 of [27]), so we also write it as \([b_r]\). We can also identify it with the unitary L implementing the (trivial) automorphism in \({\mathbb {R}}\rtimes _{\mathrm{id}}{\mathbb {Z}}\).
On the other hand, the induced algebra for \(({\mathbb {R}},{\mathrm{id}})\) is just the continuous real-valued functions on the circle \(C({\mathbb {T}};{\mathbb {R}})\). It is also known that
where \(P_{\mathrm{Mob}}\) is the Möbius projection in \(M_2(C({\mathbb {T}};{\mathbb {R}}))\) given by
It is straightforward to compute the real Paschke map on \(KO_0(C({\mathbb {T}};{\mathbb {R}}))\). For the constant projection 1, the Paschke path of unitaries is trivial, so we have \(\gamma ^{0,{{{\mathrm{Paschke}}}}}_{\mathrm{id}}[1]=[L+1-1]=[L]=[b_r]\). For the Möbius projection, the Paschke path of unitaries is \(w_\theta =R(\theta )\), so \(w_1\) is minus the identity. Then
so \(\gamma ^{0,{{{\mathrm{Paschke}}}}}_{\mathrm{id}}([P_{\mathrm{Mob}}]-[1_{C({\mathbb {T}};{\mathbb {R}})}])=[-1_{C({\mathbb {T}},\varsigma )}]\), i.e. the torsion generators are correctly mapped to each other.
The normalization axiom in the real \(C^*\)-algebra case needs to be replaced by
Axiom A.9
(Normalization) If \(({\mathcal {A}},\alpha )=({\mathbb {R}},{\mathrm {id}})\), then \(\gamma ^0_{{\mathrm {id}}}:KO_0(C({\mathbb {T}};{\mathbb {R}}))\cong KO^0({\mathbb {T}})\rightarrow KO_1(C_{\mathbb {R}}^*({\mathbb {Z}}))\cong KO_1(C({\mathbb {T}};\varsigma ))\) takes \([1_{C({\mathbb {T}};{\mathbb {R}})}]\) to the (Bott) generator \([b_r]\) and \(([P_{\mathrm{Mob}}]-[1_{C({\mathbb {T}};{\mathbb {R}})}])\) to \([-1_{C({\mathbb {T}},\varsigma )}]\).
Theorem A.10
There is a unique natural transformation \(\gamma \) of the functors \(({\mathcal {A}},\alpha )\mapsto KO_\bullet (\mathrm {Ind}({\mathcal {A}},\alpha ))\) and \(({\mathcal {A}},\alpha )\mapsto KO_{\bullet +1}({\mathcal {A}}\rtimes _\alpha {\mathbb {Z}})\), \(\bullet \in {\mathbb {Z}}_8\) , from the category of real \({\mathbb {Z}}\)-algebras to abelian groups, which satisfy Axiom A.9 and Axioms A.2–A.3 with K replaced by KO. Thus, the real version of Corollary A.8 holds: \(\gamma ^{\bullet ,\,{{{{{\mathrm{Paschke}}}}}}}_\alpha =M_\alpha ^{\bullet +1,\,{\mathrm{Green}}}\circ \phi ^\bullet _{\tau ^\alpha }\) up to a sign convention.
Appendix B: Multipliers for lattice groups
Let \(N={\mathbb {Z}}^d\) and for a multiplier \(\sigma \), let \(\widetilde{\sigma }(n,n^\prime ) = \sigma (n,n^\prime )/ \sigma (n^\prime ,n)\) be the antisymmetric bicharacter labelling its class in \(H^2(N,{\mathbb {T}})\). We reconstruct a canonical representative multiplier in this class starting from \(\widetilde{\sigma }\). Choose generators \(\{e_j\}_{j\in J}\), where J is a totally ordered set, and, expanding \(n = \sum _j n_je_j \in N\), and \(n^\prime \) similarly, we define the multiplier
which is also a bicharacter (but not antisymmetric). Then we see that
Thus, we see that \(\widetilde{\sigma }_J = \widetilde{\sigma }\), and consequently, \(\sigma _J\) is cohomologous to \(\sigma \), and so also to any \(\sigma _{J^\prime }\) for any other totally ordered set \(J^\prime \). We note that when \(N = {\mathbb Z}^{2}\) and \(J = \{1,2\}\) indexes the usual generators with the natural ordering, the antisymmetric bicharacter \(\widetilde{\sigma }(n,n^\prime ) = \exp (i(n_1n_2^\prime - n_2n_1^\prime ))\) produces \(\sigma _J(n,n^\prime ) = \exp (i(n_1n_2^\prime ))\).
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Hannabuss, K.C., Mathai, V. & Thiang, G.C. T-duality simplifies bulk–boundary correspondence: the noncommutative case. Lett Math Phys 108, 1163–1201 (2018). https://doi.org/10.1007/s11005-017-1028-x
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DOI: https://doi.org/10.1007/s11005-017-1028-x
Keywords
- T-duality
- Topological insulators
- Quantum Hall effect
- Defects
- Bulk–boundary correspondence
- Disorder
- Magnetic fields
- H-flux