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ALT Image shows text on a light pink background. The text says: Physics World LIVE In partnership with Reports on Progress in Physics. Physics World Live: Careers. 9th April 2025, 15:00 BST - Register today
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ALT Illustration taken from the open access article showing figure 2. Diagrams describing: (a) radiative corrections to the beta decay; (b) internal bremsstrahlung simultaneous to the beta decay.
ALT Illustration taken from the open access article showing figure 5. The different FPV configurations considered. This figure is only for illustrative purposes and does not portray actual float design or panel arrangement from commercial systems.
ALT Illustration taken from the open access article showing figure 10. (a) The 3D plot of the Wilson ratio R χs w maps out the phase diagram of the 1D Hubbard model at low temperatures, which significantly marks different phases of states. The parameter setting reads: T = 0.005 and u = 1. (b) A plot of the Wilson ratio R χs w at fixed B = 0.4,u = 1. As the chemical potential changes, four phases (I, II, IV and V) can be reached, indicated by sudden enhancements of the Wilson ratio.
![Illustration taken from the open access text showing figure 10. Constraints on axion-nucleon couplings. The laboratory
constraints are from direct searches for axion-nucleon coupling and
indirect searches for spin-dependent forces. Experiments at different
Compton frequencies corresponds to different ALP masses ma.
There are important consequences that the laboratory constraints
from [58–60] exceeds the astrophysical limits. The astrophysical
limits are from the analysis of [18]. Reproduced with permission
from [268].](https://pbs.twimg.com/media/GmfTy2iaUAA2TzJ.png?name=orig)
ALT Illustration taken from the open access text showing figure 10. Constraints on axion-nucleon couplings. The laboratory constraints are from direct searches for axion-nucleon coupling and indirect searches for spin-dependent forces. Experiments at different Compton frequencies corresponds to different ALP masses ma. There are important consequences that the laboratory constraints from [58–60] exceeds the astrophysical limits. The astrophysical limits are from the analysis of [18]. Reproduced with permission from [268].
ALT Illustration taken from the open acces article showing Figure 1. Comparison between conventional-gain-based and dispersive-gain-based wireless power transfer schemes as the coupling coefficient k varies. (a) Conventional saturation-gain and dispersion-gain schemes. (b), (c) Comparison of (b) devices’ gain and (c) steady-state required gain spectrum. Circuit diagrams of the coupled resonator system using (d) parallel–parallel (PP) and (e) parallel–series (PS) topologies
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