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X-ray sources with high photon fluxes and small source sizes have been widely pursued in the last decades. With synchrotron and XFEL facilities being complex, scarce and not easily accessible, laser-driven x-ray sources have emerged as a promising option because of their compactness, high photon yield and micrometric source size. In this work, we present the optimisation of an x-ray source driven by means of 0.8 mJ, 35 fs laser pulses focused on a solid Cu target in air. A detailed characterisation of the main x-ray beam parameters is included. A Cu K flux of 2.3·10 photons/s has been measured in 2 sr. Despite the simplicity of our setup, this flux is competitive with respect to that achieved with vacuum-based sources. A clear non-isotropic distribution of the x-ray continuum has been recorded, differing from the isotropic emission reported in dedicated studies. The beam is emitted within a cone with a semiangle of ≈14°, directed primarily along the target normal. Given the achieved flux, this source stands as a competitive alternative to more complex laser-driven x-ray sources operating in vacuum or in a He environment.
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http://dx.doi.org/10.1364/OE.544027 | DOI Listing |
Ultra-intense laser and plasma interactions with their ability to accelerate particles reaching relativistic speed are exciting from a fundamental high-field physics perspective. Such relativistic laser-plasma interaction (RLPI) offers a plethora of critical applications for energy, space, and defense enterprise. At AFIT's Extreme Light Laboratory (ELL), we have demonstrated such RLPI employing a table-top ∼10, 40 fs laser pulses at a kHz repetition rate that produce different types of secondary radiations via target normal sheath acceleration (TNSA).
View Article and Find Full Text PDFRev Sci Instrum
July 2025
National Key Laboratory of Plasma Physics, Laser Fusion Research Center (LFRC), Academy of Engineering Physics (CAEP), Mianyang 621900, China.
Laser-driven plasma diagnostics commonly rely on high-resolution monochromatic x-ray imaging using α-quartz (211) spherical crystals at an 88.7° Bragg angle for the Cu Kα characteristic line. However, the performance of this imaging approach is constrained by astigmatism-induced resolution limits (<10 μm) and background noise interference.
View Article and Find Full Text PDFSci Rep
July 2025
Center for Free-Electron Laser Science CFEL, Deutsches Elektronen-Synchrotron DESY, Notkestr. 85, 22607, Hamburg, Germany.
Here, we present a fiber-optic dispersive wave generator for highly-efficient, wavelength-tunable ultrashort pulse generation, enabling multicolor deep-tissue two-photon imaging of neuronal and vascular structures in fixed, labeled mouse brain. Guided by comprehensive numerical simulations, a compact Yb: fiber laser-driven system is constructed that utilizes precisely parameter- and phase-matching-controlled dispersive wave generation in a photonic crystal fiber. The system delivers sub-100 fs pulses with over ~ 6.
View Article and Find Full Text PDFWith its ability to efficiently probe low-Z materials, X-ray phase imaging methods have recently raised high interest in multiple fields from biology and medical applications to high energy density (HED) physics. Initially developed with synchrotron light and X-ray tubes, we present a novel grating based Talbot X-ray deflectometer (TXD) diagnostic that was coupled with laser-generated K-α X-ray sources. The multi-terawatt laser (I > 1 × 10 W cm) was used as a testbed for diagnostic development.
View Article and Find Full Text PDFSci Adv
April 2025
Center for High-Pressure Science and Technology Advanced Research, Beijing 100094, China.
The phase transitions in minerals under shock are crucial for understanding meteorite impact history. Recent time-resolved x-ray diffraction (XRD) studies on silica shocked to 65 GPa proposed the formation of different high-pressure phases between fused silica and quartz. Furthermore, the dynamics of silica behavior under higher pressure need to be investigated, particularly during nonequilibrium superheating before melting.
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