2019
DOI: 10.1088/1361-6587/aaf613
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Enhancement of laser-driven betatron x-rays by a density-depressed plasma structure

Abstract: We report a significant enhancement of betatron radiation from a laser wakefield accelerator (LWFA) by inserting a density-depressed plasma structure. By using a technique of transverse laser machining, a longitudinally density-depressed plasma structure with tunable length and position has been fabricated to increase the betatron amplitude of the electron beam in the LWFA, leading to an enhanced photon number and critical energy of the betatron x-ray beam. By adjusting the length and position of the plasma de… Show more

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Cited by 7 publications
(7 citation statements)
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References 48 publications
(57 reference statements)
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“…In the experiment, a clear PCI image was obtained within 1 minute at a repetition rate of ∼0.3 Hz (30 s for the butterfly, 60 s for the fish), with a photon number of 1.1 × 10 7 per shot. This data acquisition time can be significantly reduced in future experiments by a factor of 10–300, through single shot photon number enhancement (10 times enhancement under similar conditions has been recently demonstrated 39 ) and repetition rate increasing to 1 Hz 40 to 10 Hz. For comparison with a typical microfocus X-ray tube of constant flux (source size 5 µ m, photon flux ∼2 × 10 4 mrad −2 s −1 ) 41 , a continuous exposure time of 1 minute is needed to get an image with similar quality.…”
Section: Discussionmentioning
confidence: 99%
“…In the experiment, a clear PCI image was obtained within 1 minute at a repetition rate of ∼0.3 Hz (30 s for the butterfly, 60 s for the fish), with a photon number of 1.1 × 10 7 per shot. This data acquisition time can be significantly reduced in future experiments by a factor of 10–300, through single shot photon number enhancement (10 times enhancement under similar conditions has been recently demonstrated 39 ) and repetition rate increasing to 1 Hz 40 to 10 Hz. For comparison with a typical microfocus X-ray tube of constant flux (source size 5 µ m, photon flux ∼2 × 10 4 mrad −2 s −1 ) 41 , a continuous exposure time of 1 minute is needed to get an image with similar quality.…”
Section: Discussionmentioning
confidence: 99%
“…The quasi-constant electron energy and coherent oscillations over a large distance can be seen in example trajectories of 1429 macro particles picked from a region near the front of the electron bunch (Figure 4k). Due to the lower bubble fields during the density depression at the center of the M-jet, the electron beam experiences a transverse expansion and a small increase in the betatron oscillation amplitude around 3.5 -5 mm 20,34 . However, this is not the main cause of the large-amplitude oscillations and enhanced betatron emission.…”
Section: A M-jetmentioning
confidence: 99%
“…An increase in photon flux has been shown by using lasers with a high pulse energy [15][16][17] . A higher conversion efficiency has been demonstrated by using clustered gas targets 18 and the transverse deflection of the injected and accelerated electron beam through transversally offsetting the accelerating plasma structure by laser-electron-beam interactions 19 or a modulated gas density profile 20,21 .…”
Section: Introductionmentioning
confidence: 99%
“…An increase in photon flux has been shown by using lasers with a high pulse energy 15 17 . A higher conversion efficiency has been demonstrated by using clustered gas targets 18 and the transverse deflection of the injected and accelerated electron beam through transversally offsetting the accelerating plasma structure by laser-electron-beam interactions 19 or a modulated gas density profile 20 , 21 .…”
Section: Introductionmentioning
confidence: 99%
“…We were able to significantly enhance the generated number of X-ray photons when compared directly to targets with a flat-top density profile under identical laser conditions. In our concept, the coherent oscillations are initiated close to the gas jet entrance, unlike other methods where increased betatron oscillation amplitudes are achieved by manipulating the already injected and accelerated electron beam well into the gas jet 20 , 21 or near the gas jet exit 19 . This enables the control of multiple degrees of freedom and the potential for additional significant enhancement through emission from many more betatron oscillation periods, further increasing the X-ray brightness and laser-to-X-ray conversion efficiency.…”
Section: Introductionmentioning
confidence: 99%