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Theoretical and Mathematical Physics

Unitary transformations of the group U(N) and diagonalization of multilevel Hamiltonians

Valerii Vladimirovich Val'kov

Published Jul 1, 1988• 28 citations
Publisher
DOI
10.1007/bf01029435

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We investigate the geometric phases and the Bargmann invariants associated with multilevel quantum systems. In particular, we show that a full set of ``gauge-invariant'' objects for an n-level system consists of n geometric phases and $\frac{1}{2}(n\ensuremath{-}1)(n\ensuremath{-}2)$ algebraically independent four-vertex Bargmann invariants. In the process of establishing this result, we develop a canonical form for U(n)\mathrm{U}(n)U(n) matrices that is useful in its own right. We show that the recently discovered ``off-diagonal'' geometric phases [N. Manini and F. Pistolesi, Phys. Rev. Lett. 8, 3067 (2000)] can be completely analyzed in terms of the basic building blocks developed in this work. This result liberates the off-diagonal phases from the assumption of adiabaticity used in arriving at them.
Recent investigations suggest that the discrete linear unitary group U(N)U(N)U(N) can be represented by interlacing a finite sequence of diagonal phase operations with an intervening unitary operator. However, despite rigorous numerical justifications, no formal proof has been provided. Here, we show that elements of U(N)U(N)U(N) can be decomposed into a sequence of NNN-parameter phases alternating with 111-parameter propagators of a lattice Hamiltonian. The proof is based on building a Lie group by alternating these two operators and showing its completeness to represent U(N)U(N)U(N) for a finite number of layers, which is numerically found to be exactly NNN. This architecture can be implemented using elementary optical components and can successfully reconstruct arbitrary unitary matrices. We propose example devices such as optical logic gates, which perform logic gate operations using a single-layer lossless and passive optical circuit design.