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

Theoretical and Mathematical Physics

Virtual levels of n-particle systems

G. M. Zhislin

Published Aug 1, 1986• 5 citations
Publisher
DOI
10.1007/bf01035545

Related papers

The absence of the Efimov effect in systems of one- and two-dimensional particles

Simon Barth, Andreas Bitter, Semjon A. Vugalter

We study virtual levels of N-particle Schrödinger operators and prove that if the particles are one-dimensional and N ≥ 3, then virtual levels at the bottom of the essential spectrum correspond to eigenvalues. The same is true for two-dimensional particles if N ≥ 4. These results are applied to prove the non-existence of the Efimov effect in systems of N ≥ 4 one-dimensional or N ≥ 5 two-dimensional particles.

arXiv:2010.08452•Journal of Mathematical Physics•Dec 1, 2021•4 citations

N-Particle Systems

Jan-Markus Schwindt

Undergraduate lecture notes in physics•Oct 27, 2015•1 citation

Feynman-diagrams approach to the quantum Rabi model for ultrastrong cavity QED: stimulated emission and reabsorption of virtual particles dressing a physical excitation

Omar Di Stefano, Roberto Stassi, Luigi Garziano +3 more

In quantum field theory, bare particles are dressed by a cloud of virtual particles to form physical particles. The virtual particles affect properties such as the mass and charge of the physical particles, and it is only these modified properties that can be measured in experiments, not the properties of the bare particles. The influence of virtual particles is prominent in the ultrastrong-coupling regime of cavity quantum electrodynamics (QED), which has recently been realised in several condensed-matter systems. In some of these systems, the effective interaction between atom-like transitions and the cavity photons can be switched on or off by external control pulses. This offers unprecedented possibilities for exploring quantum vacuum fluctuations and the relation between physical and bare particles. We consider a single three-level quantum system coupled to an optical resonator. Here we show that, by applying external electromagnetic pulses of suitable amplitude and frequency, each virtual photon dressing a physical excitation in cavity-QED systems can be converted into a physical observable photon, and back again. In this way, the hidden relationship between the bare and the physical excitations can be unravelled and becomes experimentally testable. The conversion between virtual and physical photons can be clearly pictured using Feynman diagrams with cut loops.

arXiv:1603.04984•New Journal of Physics•Apr 12, 2017•60 citations

N-particle systems

Springer eBooks•Nov 13, 2005•0 citations

Virtual levels of multi-particle quantum systems and their implications for the Efimov effect

Andreas Bitter

•Jan 1, 2020•0 citations

Many-Particle Systems

Wolfgang Nolting

Springer eBooks•Jan 1, 2017•0 citations
In quantum field theory, bare particles are dressed by a cloud of virtual particles to form physical particles. The virtual particles affect properties such as the mass and charge of the physical particles, and it is only these modified properties that can be measured in experiments, not the properties of the bare particles. The influence of virtual particles is prominent in the ultrastrong-coupling regime of cavity quantum electrodynamics (QED), which has recently been realised in several condensed-matter systems. In some of these systems, the effective interaction between atom-like transitions and the cavity photons can be switched on or off by external control pulses. This offers unprecedented possibilities for exploring quantum vacuum fluctuations and the relation between physical and bare particles. We consider a single three-level quantum system coupled to an optical resonator. Here we show that, by applying external electromagnetic pulses of suitable amplitude and frequency, each virtual photon dressing a physical excitation in cavity-QED systems can be converted into a physical observable photon, and back again. In this way, the hidden relationship between the bare and the physical excitations can be unravelled and becomes experimentally testable. The conversion between virtual and physical photons can be clearly pictured using Feynman diagrams with cut loops.