Beam stacking experiment at a fixed field alternating gradient accelerator
A key challenge in particle accelerators is to achieve high peak intensity. Space charge is particularly strong at lower energy such as during injection and typically limits achievable peak intensity. The beam stacking technique can overcome this limitation by accumulating a beam at high energy wher...
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| Main Authors: | , , , , , , , , , , , , |
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| Format: | Article |
| Language: | English |
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American Physical Society
2025-01-01
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| Series: | Physical Review Accelerators and Beams |
| Online Access: | http://doi.org/10.1103/PhysRevAccelBeams.28.012803 |
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| _version_ | 1841526688134987776 |
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| author | T. Uesugi Y. Ishi Y. Kuriyama Y. Mori C. Jolly D. J. Kelliher J.-B. Lagrange A. P. Letchford S. Machida D. W. Posthuma de Boer C. T. Rogers E. Yamakawa M. Topp-Mugglestone |
| author_facet | T. Uesugi Y. Ishi Y. Kuriyama Y. Mori C. Jolly D. J. Kelliher J.-B. Lagrange A. P. Letchford S. Machida D. W. Posthuma de Boer C. T. Rogers E. Yamakawa M. Topp-Mugglestone |
| author_sort | T. Uesugi |
| collection | DOAJ |
| description | A key challenge in particle accelerators is to achieve high peak intensity. Space charge is particularly strong at lower energy such as during injection and typically limits achievable peak intensity. The beam stacking technique can overcome this limitation by accumulating a beam at high energy where space charge is weaker. In beam stacking, a bunch of particles is injected and accelerated to high energy. This bunch continues to circulate, while a second and subsequent bunches are accelerated to merge into the first. It also allows the user cycle and acceleration cycles to be separated which is often valuable. Beam stacking is not possible in a time varying magnetic field, but a fixed field machine such as an fixed field alternating gradient accelerator (FFA) does not sweep the magnetic field. In this paper, we describe experimental demonstration of beam stacking of two beams at KURNS FFA in Kyoto University. The momentum spread and intensity of the beam was analyzed by study of the Schottky signal, demonstrating stacking with only a slight increase of momentum spread of the combined beams. The intensity of the first beam was, however, significantly reduced. rf knockout is the suspected source of the beam loss. |
| format | Article |
| id | doaj-art-e97681ec07fe4745a9047e5cb7a25351 |
| institution | Kabale University |
| issn | 2469-9888 |
| language | English |
| publishDate | 2025-01-01 |
| publisher | American Physical Society |
| record_format | Article |
| series | Physical Review Accelerators and Beams |
| spelling | doaj-art-e97681ec07fe4745a9047e5cb7a253512025-01-16T15:08:39ZengAmerican Physical SocietyPhysical Review Accelerators and Beams2469-98882025-01-0128101280310.1103/PhysRevAccelBeams.28.012803Beam stacking experiment at a fixed field alternating gradient acceleratorT. UesugiY. IshiY. KuriyamaY. MoriC. JollyD. J. KelliherJ.-B. LagrangeA. P. LetchfordS. MachidaD. W. Posthuma de BoerC. T. RogersE. YamakawaM. Topp-MugglestoneA key challenge in particle accelerators is to achieve high peak intensity. Space charge is particularly strong at lower energy such as during injection and typically limits achievable peak intensity. The beam stacking technique can overcome this limitation by accumulating a beam at high energy where space charge is weaker. In beam stacking, a bunch of particles is injected and accelerated to high energy. This bunch continues to circulate, while a second and subsequent bunches are accelerated to merge into the first. It also allows the user cycle and acceleration cycles to be separated which is often valuable. Beam stacking is not possible in a time varying magnetic field, but a fixed field machine such as an fixed field alternating gradient accelerator (FFA) does not sweep the magnetic field. In this paper, we describe experimental demonstration of beam stacking of two beams at KURNS FFA in Kyoto University. The momentum spread and intensity of the beam was analyzed by study of the Schottky signal, demonstrating stacking with only a slight increase of momentum spread of the combined beams. The intensity of the first beam was, however, significantly reduced. rf knockout is the suspected source of the beam loss.http://doi.org/10.1103/PhysRevAccelBeams.28.012803 |
| spellingShingle | T. Uesugi Y. Ishi Y. Kuriyama Y. Mori C. Jolly D. J. Kelliher J.-B. Lagrange A. P. Letchford S. Machida D. W. Posthuma de Boer C. T. Rogers E. Yamakawa M. Topp-Mugglestone Beam stacking experiment at a fixed field alternating gradient accelerator Physical Review Accelerators and Beams |
| title | Beam stacking experiment at a fixed field alternating gradient accelerator |
| title_full | Beam stacking experiment at a fixed field alternating gradient accelerator |
| title_fullStr | Beam stacking experiment at a fixed field alternating gradient accelerator |
| title_full_unstemmed | Beam stacking experiment at a fixed field alternating gradient accelerator |
| title_short | Beam stacking experiment at a fixed field alternating gradient accelerator |
| title_sort | beam stacking experiment at a fixed field alternating gradient accelerator |
| url | http://doi.org/10.1103/PhysRevAccelBeams.28.012803 |
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