In laser-driven ion acceleration, there are issues,
including repetitive ion source, ion beam
quality, energy efficiency from laser to ion beam,
the total number of ions accelerated, laser efficiency,
particle energy, etc..

Gu, Y. J.

Kawata, S.

Kong, Q.

Li, X. F.

Nakazato, K.

Ootake, Y.

Wang, P. X.

Yu, Q.

English

Nazarbayev University Repository

The 21st International Symposium on Heavy Ion Inertial Fusion | July 18-22, 2016 | Astana, Kazakhstan78 | Control of laser-driven ion acceleration  K. Nakazato1, Y. Ootake1, S. Kawata1, X. F. Li2, Y. J. Gu2, Q. Kong2, P. X. Wang2, Q. Yu2 1 Utsunomiya University, Utsunomiya, 321-8585, Japan 2 Fudan University, Shanghai, 200433, China *Corresponding author: mt166233@cc.utsunomiya-u.ac.jp, kwt@cc.utsunomiya-u.ac.jp       In laser-driven ion acceleration, there are is-sues, including repetitive ion source, ion beam quality, energy efficiency from laser to ion beam, the total number of ions accelerated, laser effi-ciency, particle energy, etc. [1] We have worked on a multi-stage laser ion ac-celeration as shown in Fig. 1 in order to control the ion beam quality and to fulfill the require-ments toward laser-ion cancer therapy.    Figure 1 shows the concept of the future ion acceleration system. An ion beam is generated by an intense laser, and each stage / component has one function to control the ion beam quality by the beam bunching and the collimation. The ions are generated by the interaction of the intense la-ser with a thin film target. The laser-produced ions tend to have a divergence angle as shown in Fig. 2a) by the laser-produced transverse electric field. However, when the target has the hole in Fig. 2b) the focusing transverse electric field is created at the hole wall and a collimated ion beam is successfully generated.   Figure 3 shows an example of a simulation model of the ion-beam collimation. The ion beam transverse divergence is suppressed by the walls behind the target. At the walls behind the target, the transverse electric field is also created to collimate the pre-accelerated ion beam. In Fig. 3 the Al thin foil substrate has another fine struc-ture to absorb the laser energy efficiently.       Figure 4 shows an example simulation for the beam bunching of the pre-accelerated ion beam. The longitudinal electric fields generated at the target surfaces are designed to reduce the veloc-ity tilt as shown in Fig. 4.  In this paper, we will present the latest re-search related to the control of laser-driven ion acceleration.   Acknowledgements:  This work was partly supported by JSPS KAKENHI Grant Number 15K05359, MEXT, the ASHULA project, ILE, Osaka Univ., CORE (Center for Optical Research and Education, Utsunomiya Univ.), Fu-dan University and CDI (Creative Dept. of Innovation, Utsunomiya Univ.).Reference [1]S.Kawata, et al., Laser Therapy, 22, 103(2013).  Fig. 4 The bunching of the pre-accelerated ion beam is re-alized by the multi-foil target. Fig.2 A hole target generates a collimated ion beam. a) b) Fig. 3 The ion beam collimation is realized by the structured target shown here. The transverse electric field at the walls behind the thin foil target reduces the pre-accelerated ion beam transverse divergence.

Control of laser-driven ion acceleration

https://nur.nu.edu.kz/bitstream/123456789/1784/1/Control%20of%20laser-driven%20ion%20acceleration.pdf

Control of laser-driven ion acceleration

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