This Article contains typographical errors. In the Results section under subheading ‘Mott insulator phase in the time domain’.
“In order to describe behaviour of the interacting many-body system we may truncate the Hilbert space to a subspace spanned by Fock states |n1, …, ns〉 where the occupied modes correspond to localized wave-packets ψj moving along a s-resonant trajectory. Then, the many-body Floquet Hamiltonian reads
where and are bosonic anihilation and creation operators and . The coefficients describe interactions between particles that ocupy the same mode (for i = j) and between particles in different modes (i ≠ j).”
should read:
“In order to describe behaviour of the interacting many-body system we may truncate the Hilbert space to a subspace spanned by Fock states |n1, …, ns〉 where the occupied modes correspond to localized wave-packets moving along a s-resonant trajectory. Then, the many-body Floquet Hamiltonian reads
where and are bosonic anihilation and creation operators. The coefficients describe interactions between particles that occupy the same mode (for i = j) and between particles in different modes (i ≠ j).”
In the Legend of Figure 2,
“Proper superpositions of the eigenstates allows one to extract 4 individual wave-packets, ψj, that are numbered in (a) and (b).”
should read:
“Proper superpositions of the eigenstates allows one to extract 4 individual wave-packets, , that are numbered in (a) and (b).”
In the Legend of Figure 3,
“The coefficients αn, in H′, are chosen so that the set of 〈〈ϕj|H′|ϕj〉〉 reproduces a chosen set of numbers Ej, where ψj’s are the wave-packets described in Fig. 2.”
should read:
“The coefficients αn, in H′, are chosen so that the set of 〈〈ϕj|H′|ϕj〉〉 reproduces a chosen set of numbers Ej, where ϕj’s are the wave-packets described in Fig. 2.”
and
“The wave-packets ψj arrive at a given position z in equidistant intervals in time, thus, the AL length in time is lt = lT.”
should read:
“The wave-packets arrive at a given position z in equidistant intervals in time, thus, the AL length in time is lt = lT.”
Additional information
The online version of the original article can be found at https://doi.org/10.1038/srep10787
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Sacha, K. Correction: Corrigendum: Anderson localization and Mott insulator phase in the time domain. Sci Rep 8, 46946 (2018). https://doi.org/10.1038/srep46946
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DOI: https://doi.org/10.1038/srep46946
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