We analyze the characteristics of the \u3b3 radiation produced by Compton back-scattering of a high brightness electron beam produced by a photoinjector and accelerated in a linac up to energies of 360\u2013720 MeV and a laser operated at about 500 nm, by comparing classical and quantum models and codes. The interaction produces \u3b3 rays in the range 4.9\u201318.8 MeV. In view of the application to nuclear resonance fluorescence a relative bandwidth of few 10 123 is needed. The bandwidth is reduced by taking advantage of the frequency\u2013angular correlation typical of the phenomenon and selecting the radiation in an angle of tens of \u3bcrads. The foreseen spectral density is 20\u20136 photons per eV in a single shot, a number that can ...
A new class of tunable, monochromatic {gamma}-ray sources capable of operating at high peak and aver...
Recent progress in accelerator physics and laser technology have enabled the development of a new cl...
No monochromatic (Δω_{x}/ω_{x}<1%), high peak brightness [>10^{20} photons/(mm^{2}×mrad^{2}×s×0.1%...
We analyze the characteristics of the γ radiation produced by Compton back-scattering of a high brig...
A high peak brilliance, laser-based Compton-scattering γ-ray source, capable of producing quasimonoe...
26 pages, 15 figuresGamma sources with high flux and spectral densities are the main requirements fo...
A Compton scattering {gamma}-ray source, capable of producing photons with energies ranging from 0.1...
A new kind of nonresonant optical recirculator, dedicated to the production of $\ensuremath{\gamma}$...
We report and discuss high-flux generation of circularly polarized γ-rays by means of Compton scatte...
In this manuscript we review the challenges of Compton back-scattering sources in advanc...
We employ the λ3 regime where a near-single-cycle laser pulse is tightly focused, thus providing the...
Nuclear photonics is an emerging field of research requiring new tools, including high spectral brig...
An experiment of gamma rays production using Compton collisions between the DAΦNE electron beam and ...
The technological development in the field of high brightness linear accelerators and high energy/hi...
A monoenergetic gamma-ray (MEGa-ray) source based on Compton scattering, targeting nuclear physics a...
A new class of tunable, monochromatic {gamma}-ray sources capable of operating at high peak and aver...
Recent progress in accelerator physics and laser technology have enabled the development of a new cl...
No monochromatic (Δω_{x}/ω_{x}<1%), high peak brightness [>10^{20} photons/(mm^{2}×mrad^{2}×s×0.1%...
We analyze the characteristics of the γ radiation produced by Compton back-scattering of a high brig...
A high peak brilliance, laser-based Compton-scattering γ-ray source, capable of producing quasimonoe...
26 pages, 15 figuresGamma sources with high flux and spectral densities are the main requirements fo...
A Compton scattering {gamma}-ray source, capable of producing photons with energies ranging from 0.1...
A new kind of nonresonant optical recirculator, dedicated to the production of $\ensuremath{\gamma}$...
We report and discuss high-flux generation of circularly polarized γ-rays by means of Compton scatte...
In this manuscript we review the challenges of Compton back-scattering sources in advanc...
We employ the λ3 regime where a near-single-cycle laser pulse is tightly focused, thus providing the...
Nuclear photonics is an emerging field of research requiring new tools, including high spectral brig...
An experiment of gamma rays production using Compton collisions between the DAΦNE electron beam and ...
The technological development in the field of high brightness linear accelerators and high energy/hi...
A monoenergetic gamma-ray (MEGa-ray) source based on Compton scattering, targeting nuclear physics a...
A new class of tunable, monochromatic {gamma}-ray sources capable of operating at high peak and aver...
Recent progress in accelerator physics and laser technology have enabled the development of a new cl...
No monochromatic (Δω_{x}/ω_{x}<1%), high peak brightness [>10^{20} photons/(mm^{2}×mrad^{2}×s×0.1%...