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Jean-Baptiste Lallement (CERN)9/21/26, 2:00 PMInvited
The Linac4 H⁻ ion source is a critical element of CERN’s operations, directly affecting both accelerator performance and its broad user base. As the sole injector particle source, its reliability and efficiency are essential to the stability of the entire proton accelerator chain and the physics programs it enables. This paper presents an overview of the system, drawing on six years of...
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Dr Mark Roberts (Woods Hole Oceanographic Institution)9/21/26, 2:25 PMInvited
Accelerator mass spectrometry (AMS) is a sensitive technique for counting single atoms. The technique was developed in nuclear physics laboratories in the late 1970s for $^{14}$C, and subsequently extended to other isotopes, including $^{10}$Be, $^{36}$Cl, and $^{129}$I. In general, the AMS method employs a positive high-voltage tandem accelerator to accelerate negative ions. Almost...
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Dr Baoxi Han (Oak Ridge National Laboratory)9/21/26, 2:50 PMInvited
The ion source utilized in the SNS accelerator complex is an RF‑driven, multicusp‑confined, Cs‑enhanced H⁻ source. It is presently operated at approximately 50 mA of H⁻ beam current (measured at the LEBT exit) with a 6% duty-factor (1.0 ms, 60 Hz), supporting the SNS proton beam power on target near 2.0 MW. Producing this beam current typically requires about 50 kW of RF power for the ion...
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