Standard

Bound-state calculations for three atoms without explicit partial wave decomposition. / Roudnev, V. A.; Yakovlev, S. L.; Sofianos, S. A.

In: Few-Body Systems, Vol. 37, No. 4, 01.12.2005, p. 179-196.

Research output: Contribution to journal › Article › peer-review

Harvard

Roudnev, VA, Yakovlev, SL & Sofianos, SA 2005, 'Bound-state calculations for three atoms without explicit partial wave decomposition', Few-Body Systems, vol. 37, no. 4, pp. 179-196. https://doi.org/10.1007/s00601-005-0114-2

APA

Roudnev, V. A., Yakovlev, S. L., & Sofianos, S. A. (2005). Bound-state calculations for three atoms without explicit partial wave decomposition. Few-Body Systems, 37(4), 179-196. https://doi.org/10.1007/s00601-005-0114-2

Vancouver

Roudnev VA, Yakovlev SL, Sofianos SA. Bound-state calculations for three atoms without explicit partial wave decomposition. Few-Body Systems. 2005 Dec 1;37(4):179-196. https://doi.org/10.1007/s00601-005-0114-2

Author

Roudnev, V. A. ; Yakovlev, S. L. ; Sofianos, S. A. / Bound-state calculations for three atoms without explicit partial wave decomposition. In: Few-Body Systems. 2005 ; Vol. 37, No. 4. pp. 179-196.

BibTeX

@article{5c1d07ad0e5a489dbb0173c466c010be,
title = "Bound-state calculations for three atoms without explicit partial wave decomposition",
abstract = "A method to calculate the bound states of three atoms without resorting to an explicit partial wave decomposition is presented. The differential form of the Faddeev equations in the total angular momentum representation is used for this purpose. The method utilizes Cartesian coordinates combined with the tensor trick preconditioning for large linear systems and Arnoldi's algorithm for eigenanalysis. As an example, we consider the He3 system in which the interatomic force has a very strong repulsive core requiring the inclusion of a large number of partial waves to achieve convergence. To improve convergence and stability in the Arnoldi's algorithm, we modify the system of equations by introducing a background potential that removes the large number of unphysical eigenvalues stemming from the hard core. The introduction of such a modifying potential does not affect the physical spectrum of the system. The results obtained by solving the modified, three-dimensional, Faddeev equations compare favorably with other results in the field.",
author = "Roudnev, {V. A.} and Yakovlev, {S. L.} and Sofianos, {S. A.}",
year = "2005",
month = dec,
day = "1",
doi = "10.1007/s00601-005-0114-2",
language = "English",
volume = "37",
pages = "179--196",
journal = "Few-Body Systems",
issn = "0177-7963",
publisher = "Springer Nature",
number = "4",

}

RIS

TY - JOUR

T1 - Bound-state calculations for three atoms without explicit partial wave decomposition

AU - Roudnev, V. A.

AU - Yakovlev, S. L.

AU - Sofianos, S. A.

PY - 2005/12/1

Y1 - 2005/12/1

N2 - A method to calculate the bound states of three atoms without resorting to an explicit partial wave decomposition is presented. The differential form of the Faddeev equations in the total angular momentum representation is used for this purpose. The method utilizes Cartesian coordinates combined with the tensor trick preconditioning for large linear systems and Arnoldi's algorithm for eigenanalysis. As an example, we consider the He3 system in which the interatomic force has a very strong repulsive core requiring the inclusion of a large number of partial waves to achieve convergence. To improve convergence and stability in the Arnoldi's algorithm, we modify the system of equations by introducing a background potential that removes the large number of unphysical eigenvalues stemming from the hard core. The introduction of such a modifying potential does not affect the physical spectrum of the system. The results obtained by solving the modified, three-dimensional, Faddeev equations compare favorably with other results in the field.

AB - A method to calculate the bound states of three atoms without resorting to an explicit partial wave decomposition is presented. The differential form of the Faddeev equations in the total angular momentum representation is used for this purpose. The method utilizes Cartesian coordinates combined with the tensor trick preconditioning for large linear systems and Arnoldi's algorithm for eigenanalysis. As an example, we consider the He3 system in which the interatomic force has a very strong repulsive core requiring the inclusion of a large number of partial waves to achieve convergence. To improve convergence and stability in the Arnoldi's algorithm, we modify the system of equations by introducing a background potential that removes the large number of unphysical eigenvalues stemming from the hard core. The introduction of such a modifying potential does not affect the physical spectrum of the system. The results obtained by solving the modified, three-dimensional, Faddeev equations compare favorably with other results in the field.

UR - http://www.scopus.com/inward/record.url?scp=29144521470&partnerID=8YFLogxK

U2 - 10.1007/s00601-005-0114-2

DO - 10.1007/s00601-005-0114-2

M3 - Article

AN - SCOPUS:29144521470

VL - 37

SP - 179

EP - 196

JO - Few-Body Systems

JF - Few-Body Systems

SN - 0177-7963

IS - 4

ER -

ID: 37233262