- Status of the Chinese project CEPC (Circular Electron Positron Collider) - 13 Dicembre 2024 - 15:00 - 16:00
- EIC overview and related studies at LNF - 25 Ottobre 2024 - 15:00 - 16:00
- Search for Electric Dipole Moments of Charged Particles and Axions using Storage Rings - 7 Giugno 2024 - 15:00 - 16:00
- Physics and Applications of Laser Plasma Accelerators - 18 Aprile 2024 - 15:00 - 16:00
- CERN Accelerates sustainability - 2 Febbraio 2024 - 15:00 - 16:00
- Overview on accelerator activities of the INFN Milano LASA SRF Group - 10 Novembre 2023 - 15:00 - 16:00
- PIC modeling proton sources - 13 Ottobre 2023 - 15:00 - 16:00
- Large recoil, symmetric photonic colliders, a way towards ultra-low emittance positron beams and intrinsically mono-chromatic gamma-ray beams - 14 Luglio 2023 - 15:00 - 16:00
- LABEC lab: Accelerators for cultural heritage studies: from big facilities to transportable instrumentation - 16 Giugno 2023 - 15:00 - 16:00
- AM per Acceleratori - 19 Maggio 2023 - 15:00 - 16:00
- Design, test and commissioning of high gradient accelerating structures at LNF - 14 Aprile 2023 - 14:30 - 15:30
- InnovaTron: An innovative compact high-intensity proton cyclotron - 10 Febbraio 2023 - 14:30 - 15:30
- Special Superconducting magnets for HiLumi LHC - 13 Gennaio 2023 - 14:30 - 15:30
- The Drift Tube Linac for ESS and ideas for future applications - 2 Dicembre 2022 - 14:30 - 15:30
- Crystals for Particle Accelerators - 4 Novembre 2022 - 14:30 - 15:30
- Accelerators and PNRR – Italy’s Next Generation Europe - 7 Ottobre 2022 - 14:30 - 15:30
- SPES: technological challenges and prospective for new applications at LNL - 10 Giugno 2022 - 15:30 - 16:30
- Muon Colliders: a challenging opportunity - 13 Maggio 2022 - 15:30 - 16:30
- FLASH - RADIOTHERAPY A NEW PARADIGM FOR TUMOR TREATMENT ? ( SAFEST project, a VHEE Linac for Flash radiotherapy ) - 11 Febbraio 2022 - 15:30 - 16:30
- Ion acceleration by laser-matter interaction: status and perspective with the upcoming I-LUCE facility at INFN-LNS - 12 Gennaio 2022 - 15:30 - 16:30