2021
DOI: 10.1140/epjb/s10051-021-00115-w
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Description of zero field steps on the potential energy surface of a Frenkel-Kontorova model for annular Josephson junction arrays

Abstract: We explain the emergence of zero field steps (ZFS) in a Frenkel-Kontorova (FK) model for a 1D annular chain being a model for an annular Josephson junction array. We demonstrate such steps for a case with a chain of 10 phase differences. We necessarily need the periodic boundary conditions. We propose a mechanism for the jump from M fluxons to $$M+1$$ M + 1 in the chain. … Show more

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Cited by 3 publications
(4 citation statements)
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“…The difference between this potential and the exact value (7) does not exceed 1.5%. Potential (8) coincides with Frenkel-Kontorova potential up to the constant and linear transformation of coordinates…”
Section: 𝑈(𝑥′ 𝑧′mentioning
confidence: 70%
See 1 more Smart Citation
“…The difference between this potential and the exact value (7) does not exceed 1.5%. Potential (8) coincides with Frenkel-Kontorova potential up to the constant and linear transformation of coordinates…”
Section: 𝑈(𝑥′ 𝑧′mentioning
confidence: 70%
“…The cosine function specifies the periodic substrate potential. This simple approximation reveals a wide variety of ground states for the system [4][5][6] and different waves in the atoms chain [7][8][9]. Solitons are of the greatest interest.…”
Section: Introductionmentioning
confidence: 95%
“…one can determine an integer M such that the chain of length L o covers up M troughs of the site potential. If λ is set correctly, the FK chain will fit into the M troughs forming a structure of a minimum with an average separation ã, with Equation (7). It holds independently of whether the numbers, L o , a o , ã, and a s , are rational or irrational.…”
Section: The Disappearence Of Incommensurabilitiesmentioning
confidence: 99%
“…The latter acts on the extracted subsystem by a potential. Of special interest may be electronic applications [2][3][4][5][6][7] for Wigner electrons or Josephson junctions. Further models are chargedensity wave conductors [8][9][10], charge transport in solids and on crystal surfaces [11], magnetic or ferro-and antiferromagnetic domain walls [12], magnetic superlattices [13], superconductivity [14,15], and vortex matter [16][17][18], to name a few.…”
Section: Introductionmentioning
confidence: 99%