2021
DOI: 10.1002/ctpp.202000097
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Cold electrons acceleration in TNSA laser‐generated plasma using a low‐contrast fs laser

Abstract: The fs laser facility in Bordeaux, delivering an intensity of 10 18 W/cm 2 at normal incidence on thin foils, has been used to induce forward electron and ion acceleration in target-normal-sheath-acceleration (TNSA) regime. Micrometric thin foils with different composition, thickness, and electron density, were prepared to promote the charge particle acceleration in the forward direction. The plasma electron and ion emission monitoring were performed on-line using SiC semiconductor detectors in time-of-flight … Show more

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Cited by 3 publications
(2 citation statements)
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References 31 publications
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“…It shows a net photopeak with an intensity Y(Cu)=17 V, a value between that detected irradiating Al and Au, indicating that the X-ray plasma emission is proportional to the atomic number of the irradiated target, according to the literature. The photopeak is followed by narrow peaks probably due to backscattered photons or fast electrons from the chamber walls [33]. Successively the TOF timescale shows the proton peak with a maximum kinetic energy of about 790 keV and a large carbon ion peak, due to the different contribution of the different ion charge state, which maximum one has an energy of about 4.6 MeV, corresponding to about six times the proton energy, according to the CBS theory of ion acceleration proportional to the charge state [23].…”
Section: Jinst 16 P08026mentioning
confidence: 99%
“…It shows a net photopeak with an intensity Y(Cu)=17 V, a value between that detected irradiating Al and Au, indicating that the X-ray plasma emission is proportional to the atomic number of the irradiated target, according to the literature. The photopeak is followed by narrow peaks probably due to backscattered photons or fast electrons from the chamber walls [33]. Successively the TOF timescale shows the proton peak with a maximum kinetic energy of about 790 keV and a large carbon ion peak, due to the different contribution of the different ion charge state, which maximum one has an energy of about 4.6 MeV, corresponding to about six times the proton energy, according to the CBS theory of ion acceleration proportional to the charge state [23].…”
Section: Jinst 16 P08026mentioning
confidence: 99%
“…In this way, fusion energy using inertial confinement can be studied and innovative neutron sources can be developed to be well controlled in yield and in switching on and off via the laser source. [9,10] In many other fields, the plasma-produced X-rays and protons can be used to induce characteristic fluorescence emission as a probe for elemental recognition or as a beam for X-ray microscopy, as recently demonstrated. [11,12] Hot and dense plasma can be produced in forward and backward directions, especially if the target is not too thin.…”
Section: Introductionmentioning
confidence: 99%