A   B   C   D   E   F   G   H   I   J   K   L   M   N   O   P   Q   R   S   T   U   V   W   X   Y   Z  

Hanayama, R.

Paper Title Page
THPD054 Inverse Compton Scattering by Laser Accelerated Electrons and its Application to Standoff Detection of Hidden Objects 4404
 
  • Y. Kitagawa, K. Fujita, R. Hanayama, K. Ishii, Y. Mori
    GPI, Hamamatsu
  • T. Kawashima
    Hamamatsu Photonics K.K., Hamamatsu
  • H. Kuwabara
    IHI, Yokohama
 
 

A tech­nique for re­mote de­tec­tion of hid­den ob­jects is an ur­gent issue, but is not yet re­al­ized, be­cause a source and a sen­sor must be lo­cat­ed on the same side of the ob­ject. An ul­tra-in­tense laser can pro­duce ex­treme­ly short and di­rec­tion­al ra­di­a­tions, that is the in­verse Comp­ton scat­ter­ings used for the backscat­ter­ing sys­tem. We here demon­strate that the laser-wake­filed-ac­cel­er­at­ed 10-MeV elec­trons in­verse­ly scat­ter the same laser light to keV X-ray emis­sions. A 10 TW OPCPA Ti:sap­phire laser BEAT ( 1J out­put, wave­length 815 nm, and pulse width 150fs) is di­vid­ed to two beams. A 0. 8-J beam is fo­cused to an en­trance edge of he­li­um gas­jet to ac­cel­er­ate elec­trons via wake­field and the other 0.2-J beam is fo­cused to the exit of the plas­ma chan­nel from the op­po­site di­rec­tion. A sec­ond har­mon­ic probe light mea­sured the chan­nel den­si­ty. To the up­stream di­rec­tion of the lat­ter beam, a CdTe de­tec­tor an­a­lyzed the Comp­ton spec­trum under a pho­ton count­ing mode* in the range of 1 keV to 20 keV, which well agrees with that cal­cu­lat­ed from the ob­tained elec­tron spec­trum up to a few tens MeV. We also have ob­served that the emis­sion is strong into the laser axis di­rec­tion.


*H. Kuwabara, Y. Mori, Y. Kitagawa, 'Coincident Measurement of a Weakly Backscattered X-ray with a CPA Laser-Produced X-ray Pulse', Plasma Fusion Research: 3, 003-004 (2008).