2020
DOI: 10.1103/physreva.101.022332
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Majorana representation for mixed states

Abstract: We generalize the Majorana stellar representation of spin-s pure states to mixed states, and in general to any hermitian operator, defining a bijective correspondence between three spaces: the spin density-matrices, a projective space of homogeneous polynomials of four variables, and a set of equivalence classes of points (constellations) on spheres of different radii. The representation behaves well under rotations by construction, and also under partial traces where the reduced density matrices inherit their… Show more

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Cited by 21 publications
(11 citation statements)
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References 55 publications
(107 reference statements)
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“…Over the years much work has been done to elucidate the geometry of the state space of higher level systems, with special focus on the qutrit state space Q 3 [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25]. To develop an intuition for the full high-dimensional geometry of the qutrit state space, subsets, cross sections and projections onto two and three dimensions were extensively studied [6,7,10,12,15,17,18,[20][21][22][23] and multi-parameter representations of qutrit states were developed [14,21,[24][25][26]. While these approaches can reproduce many geometric properties correctly, they do not give a global view of the Bloch body.…”
Section: A Bloch-ball Analog For a Qutritmentioning
confidence: 99%
“…Over the years much work has been done to elucidate the geometry of the state space of higher level systems, with special focus on the qutrit state space Q 3 [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25]. To develop an intuition for the full high-dimensional geometry of the qutrit state space, subsets, cross sections and projections onto two and three dimensions were extensively studied [6,7,10,12,15,17,18,[20][21][22][23] and multi-parameter representations of qutrit states were developed [14,21,[24][25][26]. While these approaches can reproduce many geometric properties correctly, they do not give a global view of the Bloch body.…”
Section: A Bloch-ball Analog For a Qutritmentioning
confidence: 99%
“…The denominator in the l.h.s. of (32) is just the product of the eigenvalues of the matrix − ( ) ( ), i.e., its determinant, so that a generating function for the multiplicities ( , ) , for fixed , , and all values of , may be obtained in the form of an integral formula,…”
Section: Generating Functionsmentioning
confidence: 99%
“…The stellar representation of Majorana, originally designed for pure states of a monopartite system [1], can be also generalized for mixed quantum states [32]. In the case of multipartite systems, the stellar representation is directly applicable to symmetric states of a system composed of several qubits, but a generalization applicable to antisymmetric states has also been established [33].…”
mentioning
confidence: 99%
“…Consequently, ρ nc must commute with F z , and hence share the same eigenvectors |1, m . A useful visual way to infer the rotational symmetries over the quantum states, which allows to simplify the degrees of freedom, is through the stellar Majorana representation for pure [51] and mixed states [52]. The eigenvalues of A (B7) are described by…”
Section: P Phasementioning
confidence: 99%