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論文

Laser stripping for 1.3 GeV H$$^{-}$$ beam at the SNS

Gorlov, T.*; Aleksandrov, A.*; Cousineau, S.*; Liu, Y.*; Oguz, A. R.*; Kay, M.*; Saha, P. K.

Proceedings of the 2022 North American Particle Accelerator Conference (NAPAC 2022) (Internet), p.702 - 704, 2022/08

The conventional method of H$$^{-}$$ charge-exchange injection by using a solid stripper foil has serious drawbacks such as, a short foil lifetime, unexpected failure and moreover a high residual radiation due to uncontrolled foil scattering beam losses at high-intensity operation. To overcome all those issues, an H$$^{-}$$ stripping by using only lasers or by laser assisted are being extensively studied at J-PARC and the Spallation Neutron Source (SNS) at Oak Ridge, USA, respectively. However, a reduction of the laser power to realize the laser stripping is a common issue at both labs. In this research, different schemes and methods of laser stripping, especially for an effective excitation of the ground state hydrogen atom are considered. Among all methods the most realistic and practical scheme seems to be the sequential excitation scheme by using two types of laser. In this case, a laser power can be reduced to 1/25 as compared to a single step excitation. Due to a lower H$$^{-}$$ energy, a deep UV laser is used at J-PARC. Such a reduction of the laser power is further useful for a realistic implementation.

論文

Preliminary studies of laser-assisted H$$^{-}$$ stripping at 400 MeV

Saha, P. K.; 原田 寛之; 金正 倫計; 丸田 朋史*; 岡部 晃大; 吉本 政弘; 入江 吉郎*; Gorlov, T.*

Proceedings of 6th International Particle Accelerator Conference (IPAC '15) (Internet), p.3795 - 3797, 2015/06

Laser-assisted H$$^{-}$$ stripping at the RCS injection energy of 400 MeV is studied. RCS has a capability to achieve further more than the design beam power of 1 MW but lifetime of the stripper foil may be one of the most concerning issue for operation. The present work has been done in the same framework as in the ongoing project for 1 GeV beam at the Spallation neutron Source (SNS) in Oak Ridge and it gives a set of optimum parameters in order to carry out a proof-of-principle (POP) experiment first at 400 MeV. The simulated transverse and longitudinal beam parameters can be adjusted to fit with laser pulse but a laser of 1 MW peak power with wavelength of around 230 nm is required in order to obtain a stripping efficiency of about 95%. A high power laser system is thus a real challenge at this stage.

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