Physics Library
 An open source physics library
Encyclopedia | Forums | Docs | Random | Template Test |  
Login
create new user
Username:
Password:
forget your password?
Main Menu
Sections

Talkback

Downloads

Information
weak Hopf C*-algebra (Definition)
Definition 0.1   A weak Hopf $C^*$-algebra is defined as a weak Hopf algebra which admits a faithful $*$–representation on a Hilbert space. The weak C*–Hopf algebra is therefore much more likely to be closely related to a `quantum groupoid' than the weak Hopf algebra. However, one can argue that locally compact groupoids equipped with a Haar measure are even closer to defining quantum groupoids. There are already several, significant examples that motivate the consideration of weak C*-Hopf algebras which also deserve mentioning in the context of `standard' quantum theories. Furthermore, notions such as (proper) weak C*-algebroids can provide the main framework for symmetry breaking and quantum gravity that we are considering here. Thus, one may consider the quasi-group symmetries constructed by means of special transformations of the “coordinate space” $M$.

Remark: Recall that the weak Hopf algebra is defined as the extension of a Hopf algebra by weakening the definining axioms of a Hopf algebra as follows :

(1)  The comultiplication is not necessarily unit-preserving.
(2)  The counit $\varepsilon $ is not necessarily a homomorphism of algebras.
(3)  The axioms for the antipode map $S : A {\longrightarrow}A$ with respect to the counit are as follows. For all $h \in H$,
\begin{equation*}\begin{aligned}m({\rm id}\otimes S) \Delta (h) &= (\varepsilon ... ...lta(1)) \\ S(h) &= S(h_{(1)}) h_{(2)} S(h_{(3)}) ~. \end{aligned}\end{equation*}

These axioms may be appended by the following commutative diagrams

$\displaystyle {\begin{CD}A \otimes A @> S\otimes {\rm id}>> A \otimes A \\ @A \... ...A \otimes A \\ @A \Delta AA @VV m V \\ A @ > u \circ \varepsilon >> A \end{CD}}$ (0.2)
along with the counit axiom:
$\displaystyle \xymatrix@C=3pc@R=3pc{ A \otimes A \ar[d]_{\varepsilon \otimes 1}... ...{\rm id}_A} \ar[d]^{\Delta} \\ A & A \otimes A \ar[l]^{1 \otimes \varepsilon }}$ (0.3)

Some authors substitute the term quantum `groupoid' for a weak Hopf algebra.

Examples of weak Hopf C*-algebra.

(1)  

In Nikshych and Vainerman (2000) quantum groupoids were considered as weak C*–Hopf algebras and were studied in relationship to the noncommutative symmetries of depth 2 von Neumann subfactors. If

$\displaystyle A \subset B \subset B_1 \subset B_2 \subset \ldots$ (0.4)
is the Jones extension induced by a finite index depth $2$ inclusion $A \subset B$ of $II_1$ factors, then $Q= A' \cap B_2$ admits a quantum groupoid structure and acts on $B_1$, so that $B = B_1^{Q}$ and $B_2 = B_1 \rtimes Q$ . Similarly, in Rehren (1997) `paragroups' (derived from weak C*–Hopf algebras) comprise (quantum) groupoids of equivalence classes such as associated with 6j–symmetry groups (relative to a fusion rules algebra). They correspond to type $II$ von Neumann algebras in quantum mechanics, and arise as symmetries where the local subfactors (in the sense of containment of observables within fields) have depth $2$ in the Jones extension. Related is how a von Neumann algebra $N$, such as of finite index depth $2$, sits inside a weak Hopf algebra formed as the crossed product $N \rtimes A$ (Böhm et al. 1999).
(2)  In Mack and Schomerus (1992) using a more general notion of the Drinfeld construction, develop the notion of a quasi triangular quasi–Hopf algebra (QTQHA) is developed with the aim of studying a range of essential symmetries with special properties, such the quantum group algebra ${\rm U}_q (\rm {sl}_2)$ with $\vert q \vert =1$ . If $q^p=1$, then it is shown that a QTQHA is canonically associated with ${\rm U}_q (\rm {sl}_2)$. Such QTQHAs are claimed as the true symmetries of minimal conformal field theories.

Von Neumann Algebras (or $W^*$-algebras).

Let $\H$ denote a complex (separable) Hilbert space. A von Neumann algebra $\mathcal A$ acting on $\H$ is a subset of the $*$–algebra of all bounded operators $\mathcal L(\H )$ such that:

(1)   $\mathcal A$ is closed under the adjoint operation (with the adjoint of an element $T$ denoted by $T^*$).
(2)   $\mathcal A$ equals its bicommutant, namely:
$\displaystyle \mathcal A= \{A \in \mathcal L(\H ) : \forall B \in \mathcal L(\H ), \forall C\in \mathcal A,~ (BC=CB)\Rightarrow (AB=BA)\}~.$ (0.5)

If one calls a commutant of a set $\mathcal A$ the special set of bounded operators on $\mathcal L(\H )$ which commute with all elements in $\mathcal A$, then this second condition implies that the commutant of the commutant of $\mathcal A$ is again the set $\mathcal A$.

On the other hand, a von Neumann algebra $\mathcal A$ inherits a unital subalgebra from $\mathcal L(\H )$, and according to the first condition in its definition $\mathcal A$ does indeed inherit a *-subalgebra structure, as further explained in the next section on C*-algebras. Furthermore, we have the notable Bicommutant theorem which states that $\mathcal A$ is a von Neumann algebra if and only if $\mathcal A$ is a *-subalgebra of $\mathcal L(\H )$, closed for the smallest topology defined by continuous maps $(\xi,\eta)\longmapsto (A\xi,\eta)$ for all $<A\xi,\eta)>$ where $<.,.>$ denotes the inner product defined on $\H$ . For further instruction on this subject, see e.g. Aflsen and Schultz (2003), Connes (1994).

Commutative and noncommutative Hopf algebras form the backbone of quantum `groups' and are essential to the generalizations of symmetry. Indeed, in most respects a quantum `group' is identifiable with a Hopf algebra. When such algebras are actually associated with proper groups of matrices there is considerable scope for their representations on both finite and infinite dimensional Hilbert spaces.

Bibliography

1
E. M. Alfsen and F. W. Schultz: Geometry of State Spaces of Operator Algebras, Birkhäuser, Boston–Basel–Berlin (2003).
2
I. Baianu : Categories, Functors and Automata Theory: A Novel Approach to Quantum Automata through Algebraic–Topological Quantum Computations., Proceed. 4th Intl. Congress LMPS, (August-Sept. 1971).
3
I. C. Baianu, J. F. Glazebrook and R. Brown.: A Non–Abelian, Categorical Ontology of Spacetimes and Quantum Gravity., Axiomathes 17,(3-4): 353-408(2007).
4
I.C.Baianu, R. Brown J.F. Glazebrook, and G. Georgescu, Towards Quantum Non–Abelian Algebraic Topology. in preparation, (2008).
5
F.A. Bais, B. J. Schroers and J. K. Slingerland: Broken quantum symmetry and confinement phases in planar physics, Phys. Rev. Lett. 89 No. 18 (1–4): 181–201 (2002).
6
M. R. Buneci.: Groupoid Representations, Ed. Mirton: Timishoara (2003).
7
M. Chaician and A. Demichev: Introduction to Quantum Groups, World Scientific (1996).
8
L. Crane and I.B. Frenkel. Four-dimensional topological quantum field theory, Hopf categories, and the canonical bases. Topology and physics. J. Math. Phys. 35 (no. 10): 5136–5154 (1994).
9
V. G. Drinfel'd: Quantum groups, In Proc. Intl. Congress of Mathematicians, Berkeley 1986, (ed. A. Gleason), Berkeley, 798-820 (1987).
10
G. J. Ellis: Higher dimensional crossed modules of algebras, J. of Pure Appl. Algebra 52 (1988), 277-282.
11
P.. I. Etingof and A. N. Varchenko, Solutions of the Quantum Dynamical Yang-Baxter Equation and Dynamical Quantum Groups, Comm.Math.Phys., 196: 591-640 (1998).
12
P. I. Etingof and A. N. Varchenko: Exchange dynamical quantum groups, Commun. Math. Phys. 205 (1): 19-52 (1999)
13
P. I. Etingof and O. Schiffmann: Lectures on the dynamical Yang–Baxter equations, in Quantum Groups and Lie Theory (Durham, 1999), pp. 89-129, Cambridge University Press, Cambridge, 2001.
14
B. Fauser: A treatise on quantum Clifford Algebras. Konstanz, Habilitationsschrift.
arXiv.math.QA/0202059 (2002).
15
B. Fauser: Grade Free product Formulae from Grassman–Hopf Gebras. Ch. 18 in R. Ablamowicz, Ed., Clifford Algebras: Applications to Mathematics, Physics and Engineering, Birkhäuser: Boston, Basel and Berlin, (2004).
16
J. M. G. Fell.: The Dual Spaces of C*–Algebras., Transactions of the American Mathematical Society, 94: 365–403 (1960).
17
F.M. Fernandez and E. A. Castro.: (Lie) Algebraic Methods in Quantum Chemistry and Physics., Boca Raton: CRC Press, Inc (1996).
18
R. P. Feynman: Space–Time Approach to Non–Relativistic Quantum Mechanics, Reviews of Modern Physics, 20: 367–387 (1948). [It is also reprinted in (Schwinger 1958).]
19
A. Fröhlich: Non–Abelian Homological Algebra. I. Derived functors and satellites., Proc. London Math. Soc., 11(3): 239–252 (1961).
20
R. Gilmore: Lie Groups, Lie Algebras and Some of Their Applications., Dover Publs., Inc.: Mineola and New York, 2005.
21
P. Hahn: Haar measure for measure groupoids., Trans. Amer. Math. Soc. 242: 1–33(1978).
22
P. Hahn: The regular representations of measure groupoids., Trans. Amer. Math. Soc. 242:34–72(1978).
23
R. Heynman and S. Lifschitz. 1958. Lie Groups and Lie Algebras., New York and London: Nelson Press.
24
Leonid Vainerman. 2003. Locally Compact Quantum Groups and Groupoids: Proceedings of the Meeting of Theoretical Physicists and Mathematicians., Strasbourg, February 21-23, 2002., Walter de Gruyter Gmbh & Co: Berlin.



"weak Hopf C*-algebra" is owned by bci1.

View style:

Other names:  quantum groupoid dual
Also defines:  commutant, von Neumann algebra, $*$--representation on a Hilbert space, weak C*-algebroid, coordinate space, unital subalgebra, bicommutant
Keywords:  commutant, von Neumann algebra, C*-algebra, Haar measure associated with a groupoid, bicommutant theorem

Cross-references: representations, matrices, inner product, theorem, C*-algebras, section, commute, operation, operators, quantum group, fields, observables, quantum mechanics, type, groups, groupoids, paragroups, noncommutative, commutative diagrams, homomorphism, Hopf algebra, quantum gravity, quantum theories, Haar measure, locally compact groupoids, quantum groupoid, Hilbert space
There are 6 references to this object.

This is version 2 of weak Hopf C*-algebra, born on 2009-05-12, modified 2009-06-22.
Object id is 752, canonical name is WeakHopfCAlgebra2.
Accessed 1865 times total.

Classification:
Physics Classification: 00. (GENERAL)
 02. (Mathematical methods in physics)
 03. (Quantum mechanics, field theories, and special relativity )
 03.65.Fd (Algebraic methods )
Pending Errata and Addenda
None.
Discussion
Style: Expand: Order:

No messages.

Testing some escape charachters for html category with a generator has an injective cogenerator" now escape ” with "