Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Bulletin of the American Physical Society

Bogoliubov Excitations and Superfluidity in a Kronig-Penney Potential

Ippei Danshita, Susumu Kurihara, Shunji Tsuchiya

Published Mar 15, 2006• 1 citation
OpenAlex

Related papers

Landau and Dynamical Instabilities of Bose-Einstein Condensates in a Kronig-Penney Potential

Ippei Danshita, Shunji Tsuchiya

arXiv:cond-mat/0607195•Journal of Low Temperature Physics•May 29, 2007•1 citation

The Bogoliubov equations for an unconventional superfluid

John B. Ketterson, Shenian N. Song

Cambridge University Press eBooks•Jan 12, 1999•0 citations

Stability of Bose-Einstein condensates in a Kronig-Penney potential

Ippei Danshita, Shunji Tsuchiya

We study the stability of Bose-Einstein condensates with superfluid currents in a one-dimensional periodic potential. By using the Kronig-Penney model, the condensate and Bogoliubov bands are analytically calculated and the stability of condensates in a periodic potential is discussed. The Landau and dynamical instabilities occur in a Kronig-Penney potential when the quasimomentum of the condensate exceeds certain critical values as in a sinusoidal potential. It is found that the onsets of the Landau and dynamical instabilities coincide with the point where the perfect transmission of low energy excitations through each potential barrier is forbidden. The Landau instability is caused by the excitations with small $q$ and the dynamical instability is caused by the excitations with $q=\ensuremath{\pi}∕a$ at their onsets, where $q$ is the quasimomentum of excitation and $a$ is the lattice constant. A swallow-tail energy loop appears at the edge of the first condensate band when the mean-field energy is sufficiently larger than the strength of the periodic potential. We find that the upper portion of the swallow-tail is always dynamically unstable, but the second Bogoliubov band has a phonon spectrum reflecting the positive effective mass.

arXiv:cond-mat/0610582•Physical Review A•Mar 22, 2007•38 citations

Interferences between Bogoliubov excitations in superfluids of light

Iacopo Carusotto

•Jan 1, 2020•0 citations

Bogoliubov excitations in a Kronig-Penney potential

Ippei Danshita, Susumu Kurihara, Shunji Tsuchiya

With use of the Kronig-Penney model, we study the excitation spectrum of a Bose-Einstein condensate in a one-dimensional periodic potential. We solve the Bogoliubov equations analytically and obtain the band structure of the excitation spectrum for arbitrary values of the lattice depth. We find that the excitation spectrum is gapless and linear at low energies, and that it is due to the anomalous tunneling of low-energy excitations, predicted by Kagan et al.

arXiv:cond-mat/0506266•Physical Review A•Nov 10, 2005•16 citations

Elementary Excitations of Condensates in a Kronig-Penney Potential

Ippei Danshita, Shinichiro Kurihara, S. Tsuchiya

We investigate the excitation spectrum of a Bose‐Einstein condensate in a Kronig‐Penney potential. We solve the Bogoliubov equations analytically and obtain the band structure of the excitation spectrum. We find that the excitation spectrum is gapless and linear at low energies. This property is found to be attributed to the anomalous tunneling behavior of low energy excitations, which has been predicted by Kagan et al.

AIP conference proceedings•Jan 1, 2006•0 citations
We study the stability of Bose-Einstein condensates with superfluid currents in a one-dimensional periodic potential. By using the Kronig-Penney model, the condensate and Bogoliubov bands are analytically calculated and the stability of condensates in a periodic potential is discussed. The Landau and dynamical instabilities occur in a Kronig-Penney potential when the quasimomentum of the condensate exceeds certain critical values as in a sinusoidal potential. It is found that the onsets of the Landau and dynamical instabilities coincide with the point where the perfect transmission of low energy excitations through each potential barrier is forbidden. The Landau instability is caused by the excitations with small qqq and the dynamical instability is caused by the excitations with $q=\ensuremath{\pi}∕a$ at their onsets, where qqq is the quasimomentum of excitation and aaa is the lattice constant. A swallow-tail energy loop appears at the edge of the first condensate band when the mean-field energy is sufficiently larger than the strength of the periodic potential. We find that the upper portion of the swallow-tail is always dynamically unstable, but the second Bogoliubov band has a phonon spectrum reflecting the positive effective mass.