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Well-defined atomic hydrogen target driven by electromagnetic shock wave for stopping power measurement

Published online by Cambridge University Press:  21 September 2015

Kotaro Kondo*
Affiliation:
Research Laboratory for Nuclear Reactors, Tokyo Institute of Technology, 2-12-1 N1-14 Ookayama, Meguro-ku, Tokyo 152-8550, Japan
Tomohiro Yokozuka
Affiliation:
Research Laboratory for Nuclear Reactors, Tokyo Institute of Technology, 2-12-1 N1-14 Ookayama, Meguro-ku, Tokyo 152-8550, Japan
Yoshiyuki Oguri
Affiliation:
Research Laboratory for Nuclear Reactors, Tokyo Institute of Technology, 2-12-1 N1-14 Ookayama, Meguro-ku, Tokyo 152-8550, Japan
*
Address correspondence and reprint requests to: Kotaro Kondo, Research Laboratory for Nuclear Reactors, Tokyo Institute of Technology, 2-12-1 N1-14 Ookayama, Meguro-ku, Tokyo 152-8550, Japan. E-mail: kotaro@nr.titech.ac.jp

Abstract

The precise estimation of stopping power is crucial to predict the beam energy loss in the target for heavy-ion fusion and heavy-ion-driven high-energy density physics experiments. The electromagnetic shock wave has been proposed to generate a well-defined atomic hydrogen target for the stopping power measurement with dissociation effects. We measured the angular distribution profile of the discharge plasma and the plasma velocity in the electromagnetic shock tube by high-speed framing cameras. To improve the uniformity of the discharge plasma and the velocity, an external magnetic field was applied in the electromagnetic shock tube. The plasma velocity was up to approximately 40 km/s for an initial hydrogen gas pressure of 100 Pa and the velocity decreased with the initial pressure and the propagation length. The framing cameras showed that angular distributions of the discharge plasmas were not uniform and the initial angular distributions were important for the development of plasma profiles. The interaction of the plasma with the external magnetic field was estimated using the ratio of the plasma dynamic pressure to the magnetic pressure. The estimations offer more magnetic fields to improve the discharge uniformity due to the interaction.

Type
Research Article
Copyright
Copyright © Cambridge University Press 2015 

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References

REFERENCES

Alfvén, H., Lindberg, L. & Mitlid, P. (1960). Experiments with plasma rings. J. Nucl. Energy C 1, 116120.CrossRefGoogle Scholar
Kondo, K., Moriyama, T., Hasegawa, J., Horioka, K. & Oguri, Y. (2014). Electro-magnetically driven shock and dissociated hydrogen target for stopping power measurement. Nucl. Instrum. Methods Phys. Res. A 733, 13.CrossRefGoogle Scholar
Kondo, K., Nakajima, M., Kawamura, T. & Horioka, K. (2006). Compact pulse power device for generation of one-dimensional strong shock waves. Rev. Sci. Instrum. 77, 036104.CrossRefGoogle Scholar
Kondo, K. & Oguri, Y. (2015). accepted for publication to J. Phys: Conf. Ser.Google Scholar
Grisham, L.R. (2004). Moderate energy ions for high energy density physics experiments. Phys. Plasmas 11, 57275729.CrossRefGoogle Scholar
Hasegawa, J., Ikegawa, H., Nishinomiya, S., Watahiki, T. & Oguri, Y. (2009). Beam-plasma interaction experiments using electromagnetically driven shock waves. Nucl. Instrum. Methods Phys. Res. A 606, 205211.CrossRefGoogle Scholar
Ogawa, M., Neuner, U., Kobayashi, H., Nakajima, Y., Nishigori, K., Takayama, K., Iwase, O., Yoshida, M., Kojima, M., Hasegawa, J., Oguri, Y., Horioka, K., Nakajima, M., Miyamoto, S., Dubenkov, V. & Murakami, T. (2000). Measurement of stopping power of 240 MeV argon ions in partially ionized helium discharge plasma. Laser Part. Beams 18, 647653.CrossRefGoogle Scholar
Paul, H. (2006). A comparison of recent stopping power tables for light and medium-heavy ions with experimental data, and applications to radiotherapy dosimetry. Nucl. Instrum. Methods Phys. Res. B 247, 166172.CrossRefGoogle Scholar
Roth, M., Cowan, T.E., Key, M.H., Hatchett, S.P., Brown, C., Fountain, W., Johnson, J., Pennington, D.M., Snavely, R.A., Wilks, S.C., Yasuike, K., Ruhl, H., Pegoraro, F., Bulanov, S.V., Campbell, E.M., Perry, M.D. & Powell, H. (2001). Fast ignition by intense laser-accelerated proton beams. Phys. Rev. Lett. 86, 436439.CrossRefGoogle ScholarPubMed
Tabak, M., Hammer, J., Glinsky, M.E., Kruer, W.L., Wilks, S.C., Woodworth, J., Campbell, E.M., Perry, M.D. & Mason, R.J. (1994). Ignition and high gain with ultra powerful lasers. Phys. Plasmas 1, 16261634.CrossRefGoogle Scholar
Ziegler, J.F., Ziegler, M.D. & Biersack, J.P. (2008). The Stopping and Range of Ions in Matter (SRIM). http://www.srim.org/Google Scholar
Zwicknagel, G. (1998). Nonlinear heavy-ion stopping in plasmas. Nucl. Instrum. Methods Phys. Res. A 415, 680685.CrossRefGoogle Scholar
Zwicknagel, G. (2009). Theory and simulation of heavy ion stopping in plasma. Laser Part. Beams 27, 399413.CrossRefGoogle Scholar