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

Two-level systems and a low-energy oscillator: Excitation transfer and energy exchange

Peter L. Hagelstein, Irfan U. Chaudhary

Published Mar 5, 2007• 0 citations
OpenAlex

Related papers

Two-level systems coupled to an oscillator: Excitation transfer and energy exchange

Peter L. Hagelstein, Irfan U. Chaudhary

We consider models in which two sets of matched two-level systems are coupled to a common oscillator in the case where the oscillator energy is small relative to the two-level transition energies. Since the two sets of two-level systems are coupled indirectly through the oscillator, excitation transfer from one set of two-level systems to the other is possible. In addition, the excitation energy from the two-level systems may be exchanged with the oscillator coherently, even though the oscillator energy may be orders of magnitude smaller than the two-level system transition energy. In the lossless case, we demonstrate these effects numerically, and also use an approximate diagonalization to show that these effects are expected from the model Hamiltonian. We augment the model to include loss effects, and show that loss enhances the excitation transfer effect by breaking the severe cancelation between different paths that occurs in the lossless case. We describe a simple approximate model wavefunction appropriate when the loss increases rapidly with energy. Within this model approximation, we present numerical and analytical results for excitation transfer and energy transfer rates, showing that they are greatly increased. Our study of these models is motivated in part by claims of excess heat production in electrochemical experiments in heavy water. We examine the question of whether the rates associated with this kind of model are sufficiently large to be relevant to the experimental claims. We find that consistency is possible given recent experimental results showing strong screening effects in low energy deuteron-deuteron fusion experiments in metals.

arXiv:cond-mat/0612306•Dec 12, 2006•4 citations

Non-Markovian excitation transfer dynamics between two level systems

Tomoaki Yazaki, Akira Ishikawa, Kiyoshi Kobayashi

The Japan Society of Applied Physics•Jul 10, 2019•0 citations

Electronic energy transfer in a dense level system

C. Gabbanini, M. Biagini, Silvia Gozzini +3 more

Journal of Quantitative Spectroscopy and Radiative Transfer•Feb 1, 1992•4 citations

Excitation transfer in two two-level systems coupled to an oscillator

Peter L. Hagelstein, Irfan U. Chaudhary

We consider a generalization of the spin-boson model in which two different two-level systems are coupled to an oscillator, under conditions where the oscillator energy is much less than the two-level system energies, and where the oscillator is highly excited. We find that the two-level system transition energy is shifted, producing a Bloch-Siegert shift in each two-level system similar to what would be obtained if the other were absent. At resonances associated with energy exchange between a two-level system and the oscillator, the level splitting is about the same as would be obtained in the spin-boson model at a Bloch-Siegert resonance. However, there occur resonances associated with the transfer of excitation between one two-level system and the other, an effect not present in the spin-boson model. We use a unitary transformation leading to a rotated system in which terms responsible for the shift and splittings can be identified. The level splittings at the anticrossings associated with both energy exchange and excitation transfer resonances are accounted for with simple two-state models and degenerate perturbation theory using operators that appear in the rotated Hamiltonian.

arXiv:0803.1906•Journal of Physics B Atomic Molecular and Optical Physics•Jun 23, 2008•5 citations

Excitation of a two-level system damped by the interaction with bosons

Jan Loos

Czechoslovak Journal of Physics•Jun 1, 1972•1 citation

Coupling between the Center of Mass and Relative Degrees of Freedom in a Relativistic Quantum Composite and Applications

Peter L. Hagelstein, Irfan U. Chaudhary

If we consider the nucleus as a relativistic composite, then we are able to derive from a many-particle Dirac model a coupling between the center of mass motion and internal nuclear degrees of freedom. This interaction can be rotated out in free space, but has the potential to give rise to new physics when two or more nuclei exchange phonons with a common vibrational mode. The simplest example of such a system is a homonuclear diatomic molecule in a frozen matrix, for which we are able to develop an expression for the second-order phonon–nuclear interaction that can result in a splitting of the nuclear energy levels as a result of excitation transfer between the nuclei. The phonon-nuclear coupling is an E1 interaction, so the low energy 6.237 keV E1 transition in 181Ta is special; this motivates an interest in molecular 181Ta2 as a candidate for a Mössbauer experiment where the splitting might be observable. We also consider excitation transfer in the case of a macroscopic a Ta plate.

Journal of Condensed Matter Nuclear Science•Oct 1, 2017•5 citations
We consider models in which two sets of matched two-level systems are coupled to a common oscillator in the case where the oscillator energy is small relative to the two-level transition energies. Since the two sets of two-level systems are coupled indirectly through the oscillator, excitation transfer from one set of two-level systems to the other is possible. In addition, the excitation energy from the two-level systems may be exchanged with the oscillator coherently, even though the oscillator energy may be orders of magnitude smaller than the two-level system transition energy. In the lossless case, we demonstrate these effects numerically, and also use an approximate diagonalization to show that these effects are expected from the model Hamiltonian. We augment the model to include loss effects, and show that loss enhances the excitation transfer effect by breaking the severe cancelation between different paths that occurs in the lossless case. We describe a simple approximate model wavefunction appropriate when the loss increases rapidly with energy. Within this model approximation, we present numerical and analytical results for excitation transfer and energy transfer rates, showing that they are greatly increased. Our study of these models is motivated in part by claims of excess heat production in electrochemical experiments in heavy water. We examine the question of whether the rates associated with this kind of model are sufficiently large to be relevant to the experimental claims. We find that consistency is possible given recent experimental results showing strong screening effects in low energy deuteron-deuteron fusion experiments in metals.
We consider a generalization of the spin-boson model in which two different two-level systems are coupled to an oscillator, under conditions where the oscillator energy is much less than the two-level system energies, and where the oscillator is highly excited. We find that the two-level system transition energy is shifted, producing a Bloch-Siegert shift in each two-level system similar to what would be obtained if the other were absent. At resonances associated with energy exchange between a two-level system and the oscillator, the level splitting is about the same as would be obtained in the spin-boson model at a Bloch-Siegert resonance. However, there occur resonances associated with the transfer of excitation between one two-level system and the other, an effect not present in the spin-boson model. We use a unitary transformation leading to a rotated system in which terms responsible for the shift and splittings can be identified. The level splittings at the anticrossings associated with both energy exchange and excitation transfer resonances are accounted for with simple two-state models and degenerate perturbation theory using operators that appear in the rotated Hamiltonian.
If we consider the nucleus as a relativistic composite, then we are able to derive from a many-particle Dirac model a coupling between the center of mass motion and internal nuclear degrees of freedom. This interaction can be rotated out in free space, but has the potential to give rise to new physics when two or more nuclei exchange phonons with a common vibrational mode. The simplest example of such a system is a homonuclear diatomic molecule in a frozen matrix, for which we are able to develop an expression for the second-order phonon–nuclear interaction that can result in a splitting of the nuclear energy levels as a result of excitation transfer between the nuclei. The phonon-nuclear coupling is an E1 interaction, so the low energy 6.237 keV E1 transition in 181Ta is special; this motivates an interest in molecular 181Ta2 as a candidate for a Mössbauer experiment where the splitting might be observable. We also consider excitation transfer in the case of a macroscopic a Ta plate.