Geometric properties of SIC-POVM tensor square

@article{Ostrovskyi2019GeometricPO,
  title={Geometric properties of SIC-POVM tensor square},
  author={Vasyl Ostrovskyi and Danylo Yakymenko},
  journal={Letters in Mathematical Physics},
  year={2019},
  volume={112},
  pages={1-27}
}
It is known that if $$d^2$$ d 2 vectors in a d -dimensional Hilbert space H form a symmetric, informationally complete, positive operator-valued measure (SIC-POVM), then the tensor squares of these vectors form an equiangular tight frame in the symmetric subspace of $$H\otimes H$$ H ⊗ H . We prove that, for any SIC-POVM of the Weyl–Heisenberg group covariant type (WH-type), this frame can be obtained by projecting a WH-type basis in $$H\otimes H$$ H ⊗ H onto the symmetric subspace. We give a… 

Dimension towers of SICS: II. Some constructions

A SIC is a maximal equiangular tight frame in a finite dimensional Hilbert space. Given a SIC in dimension d, there is good evidence that there always exists an aligned SIC in dimension d(d − 2),

On the continuous Zauner conjecture

In a recent paper by S. Pandey, V. Paulsen, J. Prakash, and M. Rahaman, the authors studied the entanglement breaking quantum channels $\Phi_t:\mbb{C}^{d\times d} \to \mbb{C}^{d \times d}$ for $t \in

The finite Fourier Transform and projective 2-designs

There are several approaches to define an eigenvector decomposition of the finite Fourier Transform (Fourier matrix), which is in some sense unique, and at best resembles the eigenstates of the quantum

SICs: Some Explanations

The aim, so far unfulfilled, is to prove existence of SICs in an infinite sequence of dimensions.

SICs: Some Explanations

The problem of constructing maximal equiangular tight frames or SICs was raised by Zauner in 1998. Four years ago it was realized that the problem is closely connected to a major open problem in

References

SHOWING 1-10 OF 23 REFERENCES

Tight frames, Hadamard matrices and Zauner’s conjecture

We show that naturally associated to a SIC (symmetric informationally complete positive operator valued measure or SIC-POVM) in dimension d there are a number of higher dimensional structures:

SIC-POVMs and the Extended Clifford Group

We describe the structure of the extended Clifford Group (defined to be the group consisting of all operators, unitary and anti-unitary, which normalize the generalized Pauli group (or Weyl-Heisenberg

Symmetric informationally complete–positive operator valued measures and the extended Clifford group

We describe the structure of the extended Clifford group [defined to be the group consisting of all operators, unitary and antiunitary, which normalize the generalized Pauli group (or Weyl–Heisenberg

Symmetric informationally complete quantum measurements

It is conjecture that a particular kind of group-covariant SIC–POVM exists in arbitrary dimensions, providing numerical results up to dimension 45 to bolster this claim.

Symmetric informationally complete positive-operator-valued measures: A new computer study

We report on a new computer study of the existence of d2 equiangular lines in d complex dimensions. Such maximal complex projective codes are conjectured to exist in all finite dimensions and are the

SIC-POVMs: A new computer study

We report on a new computer study into the existence of d2 equiangular lines in d complex dimensions. Such maximal complex projective codes are conjectured to exist in all finite dimensions and are

The SIC Question: History and State of Play

Computer calculations have now furnished solutions in all dimensions up to 151, and in several cases beyond that, as large as dimension 844.

Complex Hadamard matrices and Equiangular Tight Frames

In this paper we give a new construction of parametric families of complex Hadamard matrices of square orders, and connect them to equiangular tight frames. The results presented here generalize some

Tables of the existence of equiangular tight frames

Every known construction of ETFs is surveyed and existence for sufficiently small dimensions is tabulated.