General Theory of Constructing Potential with Bound States in the Continuum

We present a general theory of potentials that support bound states at positive energies (bound states in the continuum). On the theoretical side, we prove that, for systems described by nonlocal potentials of the form $V(r,r^{\prime })$, bound states at positive energies are as common as those at n...

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Published inProgress of theoretical and experimental physics Vol. 2024; no. 7
Main Authors Kurino, Mao, Takayanagi, Kazuo
Format Journal Article
LanguageEnglish
Published Oxford Oxford University Press 01.07.2024
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Abstract We present a general theory of potentials that support bound states at positive energies (bound states in the continuum). On the theoretical side, we prove that, for systems described by nonlocal potentials of the form $V(r,r^{\prime })$, bound states at positive energies are as common as those at negative energies. At the same time, we show that a local potential of the form $V(r)$ rarely supports a positive-energy bound state. On the practical side, we show how to construct a (naturally nonlocal) potential that supports an arbitrary normalizable state at an arbitrary positive energy. We demonstrate our theory with numerical examples both in momentum and coordinate spaces with emphasis on the important role played by nonlocal potentials. Finally, we discuss how to observe bound states at positive energies, and where to search for nonlocal potentials that may support them.
AbstractList We present a general theory of potentials that support bound states at positive energies (bound states in the continuum). On the theoretical side, we prove that, for systems described by nonlocal potentials of the form $V(r,r^{\prime })$, bound states at positive energies are as common as those at negative energies. At the same time, we show that a local potential of the form $V(r)$ rarely supports a positive-energy bound state. On the practical side, we show how to construct a (naturally nonlocal) potential that supports an arbitrary normalizable state at an arbitrary positive energy. We demonstrate our theory with numerical examples both in momentum and coordinate spaces with emphasis on the important role played by nonlocal potentials. Finally, we discuss how to observe bound states at positive energies, and where to search for nonlocal potentials that may support them.
Author Kurino, Mao
Takayanagi, Kazuo
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  surname: Takayanagi
  fullname: Takayanagi, Kazuo
  email: k-takaya@sophia.ac.jp
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Cites_doi 10.1103/PhysRevLett.107.183901
10.1103/PhysRevA.77.062714
10.1007/978-3-642-83317-5
10.1016/j.ppnp.2011.07.002
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10.1103/PhysRevA.57.3534
10.1103/PhysRevC.24.874
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10.1093/ptep/ptad076
10.1103/RevModPhys.88.035004
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Copyright The Author(s) 2024. Published by Oxford University Press on behalf of the Physical Society of Japan. 2024
The Author(s) 2024. Published by Oxford University Press on behalf of the Physical Society of Japan. This work is published under https://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.
Copyright_xml – notice: The Author(s) 2024. Published by Oxford University Press on behalf of the Physical Society of Japan. 2024
– notice: The Author(s) 2024. Published by Oxford University Press on behalf of the Physical Society of Japan. This work is published under https://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.
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Snippet We present a general theory of potentials that support bound states at positive energies (bound states in the continuum). On the theoretical side, we prove...
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SubjectTerms Decomposition
Energy
Fourier transforms
Physics
Title General Theory of Constructing Potential with Bound States in the Continuum
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