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OverviewMethodologyResults &DiscussionsIntroductionObjectiveConclusions# / 1917JAEA2014/3/6, 2013117# / 56

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OverviewMethodologyResults &DiscussionsIntroductionObjectiveConclusions# / 1917JAEA2014/3/6, 2013117# / 56

5 mm*OverviewMethodologyResults &DiscussionsIntroductionObjectiveConclusions# / 1917JAEA2014/3/6, 2013117# / 56

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CO2 Laser@10 J473nm785nmOverviewMethodologyResults &DiscussionsIntroductionObjectiveConclusions# / 1917JAEA2014/3/6, 2013117# / 56

ICCD 473nm785nm

OverviewMethodologyResults &DiscussionsIntroductionObjectiveConclusions# / 1917JAEA2014/3/6, 2013117# / 56

380-600 nmOverviewMethodologyResults &DiscussionsIntroductionObjectiveConclusions# / 1917JAEA2014/3/6, 2013117# / 56

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OverviewMethodologyResults &DiscussionsIntroductionObjectiveConclusions# / 1917JAEA2014/3/6, 2013117# / 56

OverviewResults &DiscussionsIntroductionObjectiveMethodologyConclusions# / 1917JAEA2014/3/6, 2013117# / 5610 mm40 (Mori, 2004)LSD(1/2)

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OverviewResults &DiscussionsIntroductionObjectiveMethodologyConclusions# / 1917JAEA2014/3/6, 2013117# / 56

OverviewResults &DiscussionsIntroductionObjectiveMethodologyConclusions# / 1917JAEA2014/3/6, 2013117# / 561023 m-3

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Laser Propulsion

Space transportation!!

Deep space exploration

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2. LSD, 2013117# / 561024 m-3 eV

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Fig. (left)Time varying of electron density distribution(middle)Image of interferometer and LSD inside.(right) NEW LSD modelK. Shimamura et.al, Internal Structure of Laser Supported Detonation Waves by Two-Wavelength Mach-Zehnder InterferometerJ. appl. Phys. 109 (2011)

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