Physics design of the National Spallation Neutron Source linac
H. Takeda, J.H. Billen, S. Nath
Abstract
H. Takeda, J.H. Billen, S. Nath
Abstract
The National Spallation Neutron Source (NSNS) requires a linac that accelerates a H/sup -/ beam to 1.0 GeV. The NSNS linac starts with a radio-frequency quadrupole (RFQ) accelerator; which is followed by a drift-tube linac (DTL), a coupled-cavity drift-tube linac (CCDTL), and conventional coupled-cavity linac (CCL). In this paper, we focus on the DTL, CCDTL, and CCL parts of the accelerator. We discuss the linac design parameters and beam dynamics issues. The design rationale of no separate matching sections between different accelerating sections maintains the current independence of beam behavior.
OpenAlex reports 1 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
The National Spallation Neutron Source (NSNS) requires a linac that accelerates a H/sup -/ beam to 1.0 GeV. The NSNS linac starts with a radio-frequency quadrupole (RFQ) accelerator; which is followed by a drift-tube linac (DTL), a coupled-cavity drift-tube linac (CCDTL), and conventional coupled-cavity linac (CCL). In this paper, we focus on the DTL, CCDTL, and CCL parts of the accelerator. We discuss the linac design parameters and beam dynamics issues. The design rationale of no separate matching sections between different accelerating sections maintains the current independence of beam behavior.
Key concepts: Linear particle accelerator, Spallation Neutron Source, Radio-frequency quadrupole, Physics, Spallation, Beam (structure), Nuclear physics, Particle accelerator