Cargando…
Cyclic permutations for qudits in d dimensions
One of the main challenges in quantum technologies is the ability to control individual quantum systems. This task becomes increasingly difficult as the dimension of the system grows. Here we propose a general setup for cyclic permutations X(d) in d dimensions, a major primitive for constructing arb...
Autores principales: | , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2019
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6474885/ https://www.ncbi.nlm.nih.gov/pubmed/31004090 http://dx.doi.org/10.1038/s41598-019-42708-7 |
Sumario: | One of the main challenges in quantum technologies is the ability to control individual quantum systems. This task becomes increasingly difficult as the dimension of the system grows. Here we propose a general setup for cyclic permutations X(d) in d dimensions, a major primitive for constructing arbitrary qudit gates. Using orbital angular momentum states as a qudit, the simplest implementation of the X(d) gate in d dimensions requires a single quantum sorter S(d) and two spiral phase plates. We then extend this construction to a generalised X(d)(p) gate to perform a cyclic permutation of a set of d, equally spaced values {|[Formula: see text] 〉, |[Formula: see text] + p〉, …, |[Formula: see text] + (d − 1)p〉} [Formula: see text] {|[Formula: see text] + p〉, |[Formula: see text] + 2p〉, …, |[Formula: see text] 〉}. We find compact implementations for the generalised X(d)(p) gate in both Michelson (one sorter S(d), two spiral phase plates) and Mach-Zehnder configurations (two sorters S(d), two spiral phase plates). Remarkably, the number of spiral phase plates is independent of the qudit dimension d. Our architecture for X(d) and generalised X(d)(p) gate will enable complex quantum algorithms for qudits, for example quantum protocols using photonic OAM states. |
---|