tunneling phenomena
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2021 ◽  
pp. 172-222
Author(s):  
V.I. Gol’danskii ◽  
L.I. Trakhtenberg ◽  
V.N. Fleurov

2021 ◽  
Author(s):  
V.I. Gol’danskii ◽  
L.I. Trakhtenberg ◽  
V.N. Fleurov

2020 ◽  
Vol 101 (4) ◽  
Author(s):  
Fernando Nieto-Guadarrama ◽  
Jorge Villavicencio

Author(s):  
Vasilis Pagonis ◽  
Shannon Bernier ◽  
Francisco Marques dos Santos Vieira ◽  
Shane Steele

2017 ◽  
Vol 64 (8) ◽  
pp. 3084-3091 ◽  
Author(s):  
Cristina Medina-Bailon ◽  
Jose L. Padilla ◽  
Carlos Sampedro ◽  
Cem Alper ◽  
Francisco Gamiz ◽  
...  

2017 ◽  
Vol 64 (8) ◽  
pp. 3077-3083 ◽  
Author(s):  
Po-Jui Jerry Lin ◽  
Che-An Andy Lee ◽  
Chih-Wei Kira Yao ◽  
Hsin-Jyun Vincent Lin ◽  
Hiroshi Watanabe

2017 ◽  
Vol 72 (7) ◽  
pp. 677-687 ◽  
Author(s):  
Konstantin G. Zloshchastiev

AbstractVarious kinds of Bose-Einstein condensates are considered, which evolve without any geometric constraints or external trap potentials including gravitational. For studies of their collective oscillations and stability, including the metastability and macroscopic tunneling phenomena, both the variational approach and the Vakhitov-Kolokolov (VK) criterion are employed; calculations are done for condensates of an arbitrary spatial dimension. It is determined that that the trapless condensate described by the logarithmic wave equation is essentially stable, regardless of its dimensionality, while the trapless condensates described by wave equations of a polynomial type with respect to the wavefunction, such as the Gross-Pitaevskii (cubic), cubic-quintic, and so on, are at best metastable. This means that trapless “polynomial” condensates are unstable against spontaneous delocalization caused by fluctuations of their width, density and energy, leading to a finite lifetime.


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