A collimated beam of fast protons, with energies as high as 1.5 MeV and total number of ≳109, confined in a cone angle of 40°±10° is observed when a high-intensity high-contrast subpicosecond laser pulse is focused onto a thin foil target. The protons, which appear to originate from impurities on the front side of the target, are accelerated over a region extending into the target and exit out the back side in a direction normal to the target surface. Acceleration field gradients ∼10 GeV/cm are inferred. The maximum proton energy can be explained by the charge-separation electrostatic-field acceleration due to “vacuum heating.
The properties of beams of high energy protons accelerated during ultraintense, picosecond laser-irr...
International audienceThe interaction of short and intense laser pulses with plasmas or solids is a ...
Spectrally-peaked proton beams of high charge (E-p approximate to 8 MeV, Delta E approximate to 4 Me...
A collimated beam of fast protons, with energies as high as 1.5 MeV and total number of ≳109, confin...
A collimated beam of fast protons, witlr energies as high as 10 MeV and total number of 109,109, con...
A collimated beam of fast protons, with energies as high as 10 MeV and total number of 109, confined...
We report on the characteristics of an ultrafast-laser driven proton beam from thinfilm targets. The...
We discuss the optimization and control of laser‐driven proton beams. Specifically, we report on the...
We discuss the optimization and control of laser-driven proton beams. Specifically, we report on the...
Ion acceleration resulting from the interaction of ultra-high intensity and ultra-high contrast (∼10...
The properties of beams of high energy protons accelerated during ultraintense, picosecond laser-irr...
International audienceThe interaction of short and intense laser pulses with plasmas or solids is a ...
Spectrally-peaked proton beams of high charge (E-p approximate to 8 MeV, Delta E approximate to 4 Me...
A collimated beam of fast protons, with energies as high as 1.5 MeV and total number of ≳109, confin...
A collimated beam of fast protons, witlr energies as high as 10 MeV and total number of 109,109, con...
A collimated beam of fast protons, with energies as high as 10 MeV and total number of 109, confined...
We report on the characteristics of an ultrafast-laser driven proton beam from thinfilm targets. The...
We discuss the optimization and control of laser‐driven proton beams. Specifically, we report on the...
We discuss the optimization and control of laser-driven proton beams. Specifically, we report on the...
Ion acceleration resulting from the interaction of ultra-high intensity and ultra-high contrast (∼10...
The properties of beams of high energy protons accelerated during ultraintense, picosecond laser-irr...
International audienceThe interaction of short and intense laser pulses with plasmas or solids is a ...
Spectrally-peaked proton beams of high charge (E-p approximate to 8 MeV, Delta E approximate to 4 Me...