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Entangled Hbars

SIC POVMs and Zauner's Conjecture

 contact:  D. Gross  date:  17 Feb 2005  last progress:    -    solved by:    -  

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Problem   Background   Partial Results and History   Literature  

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Problem

We will give three variants of the problem, each being stronger than its predecessor. The terminology of problems 1 and 2 is taken mainly from [1]. For problem 3 see [2] and [3].


Problem 1: SIC-POVMs

A set of d2 normed vectors {|\phii>}i in a Hilbert space of dimension d constitutes a set of equiangular lines if their mutual inner products

|<\phii|\phij>|2

are independent of the choice of i \neq j. It can be shown [1] that A POVM that arises in this way is called symmetric informationally complete, or a SIC-POVM for short.

The most general form of the problem is: decide if SIC-POVMs exists in any dimension d.


Problem 2: Covariant SIC-POVMs

For a given basis {|q>}q=0... d-1 of the Hilbert space, define the shift operator X and clock operator Z respectively by the relations
X |q> := |q+1>
Z |q> := ei \frac 2 \pi d q |q>,
where arithmetic is modulo d. Further, define the Weyl operators

w(p,q) = Z(p) X(q)      

(label:weyl)

for all p, q in Zd. We will refer to the group generated by (ref:weyl) as the Heisenberg group. It is also known as the Weyl-Heisenberg group or Generalized Pauli group.

A vector |\phi> is called a fiducial vector with respect to the Heisenberg group if the set

{w(p,q) |\phi> <\phi| w(p,q)* }p,q=0... d-1      

(label:cov)

induces a SIC-POVM. Such a SIC-POVM is said to be group covariant. The definition makes sense for any group of order at least d2. However, we will focus on the Heisenberg group in what follows.

The problem: decide if group covariant SIC-POVMs exist in any dimension d.


Problem 3: Zauner's Conjecture

The normalizer of the Heisenberg group within the unitaries U(d) is called the Clifford group. There exists an element z of the Clifford group which is defined via its action on the Weyl operators as

z w(p,q) z* = w(q-p,-p).

Zauner's conjecture, as formulated in [3], runs: in any dimension d, a fiducial vector can be found among the eigenvectors of Z.

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Background

Besides their mathematical appeal, SIC-POVMs have obvious applications to quantum state tomography. The symmetry condition assures that the possible measurement outcomes are in some sense maximally complementary.

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Partial Results and History

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Literature

[1]J. M. Renes, R. Blume-Kohout, A. J. Scott, and C. M. Caves, »Symmetric Informationally Complete Quantum Measurements«, J. Math. Phys. 45, 2171 (2004) and quant-ph/0310075 (2003).
[2]G. Zauner, »Quantendesigns - Grundzüge einer nichtkommutativen Designtheorie«, Doctorial thesis, University of Vienna, 1999 (available online at http://www.mat.univie.ac.at/ neum/papers/physpapers.html).
[3]D. M. Appleby, »SIC-POVMs and the Extended Clifford Group«, quant-ph/0412001 (2004).
[4]A. Klappenecker, and M. Rötteler, »Mutually Unbiased Bases are Complex Projective 2-Designs«, quant-ph/0502031 (2005).
[5]M. Grassl, »On SIC-POVMs and MUBs in dimension 6«, quant-ph/0406175 (2004).
[6]D. Gross, Diploma thesis, University of Potsdam, 2005.
[7]W. K. Wootters, »Quantum measurements and finite geometry«, quant-ph/0406032 (2004).
[8]I. Bengtsson and \AA. Ericsson, »Mutually Unbiased Bases and The Complementarity Polytope«, quant-ph/0410120 (2004).


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