{"id":20485,"date":"2019-05-27T09:52:32","date_gmt":"2019-05-27T07:52:32","guid":{"rendered":"http:\/\/www.eli-beams.eu\/research\/x-ray-sources\/plasma-x-ray-sources-pxs\/"},"modified":"2021-06-17T14:43:06","modified_gmt":"2021-06-17T12:43:06","slug":"plasma-x-ray-sources-pxs","status":"publish","type":"page","link":"https:\/\/www.eli-beams.eu\/research\/x-ray-sources\/plasma-x-ray-sources-pxs\/","title":{"rendered":"Laser-driven Plasma X-ray Source (PXS) Beamline"},"content":{"rendered":"<p>Thus, both line emission radiation of the specific target material and (continuous) Bremsstrahlung forms the energy spectrum of a PXS. ELI\u2019s PXS will offer 8 keV Cu-Ka, 11 keV Bi-La, 24 keV In-Ka, and\/or 77 keV Bi-Ka radiation. The X-ray pulse duration &#8211; inherit from the driving laser pulse duration &#8211; ranges in the hundreds of femtoseconds.<\/p>\n<p>The photons are emitted from the micrometer-sized plasma volume out of the vacuum chamber through an X-ray transparent window (material: Beryllium or Polyimide foil) and are focused by grazing incidence or multilayer optics onto the sample. These Montel-Optics based monochromators will be installed to generate small-focused X-ray pulses for high-spatial resolution spectroscopy and imaging. And poly-capillary optics are deployed to support absorption spectroscopy experiments at the Von-Hamos Installation.\u00a0Both spectroscopy and imaging experiments will be carried out by the PXS endstation T-REX, comprising a high-precision spectrometer with Eulerian cradle and zero-noise EIGER X detector. To enhance furthermore the dynamic spectroscopy capability, continuous X-ray tubes with Cu and Mo targets are available and ready for PXS\/T-REX operation.<\/p>\n<p><img loading=\"lazy\" class=\"alignleft wp-image-29520\" src=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/06\/Picture-1-300x225.jpg\" alt=\"\" width=\"460\" height=\"346\" srcset=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/06\/Picture-1-300x225.jpg 300w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/06\/Picture-1-1024x770.jpg 1024w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/06\/Picture-1-768x577.jpg 768w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/06\/Picture-1-400x300.jpg 400w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/06\/Picture-1.jpg 1360w\" sizes=\"(max-width: 460px) 100vw, 460px\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><em>Figure 1: Laser focus spot in front of Cu tape target (on guiding spools). The high-energetic laser pulse induces an air breakdown generating a plasma spot. Cu-Ka Line emission radiation at 8 keV and Bremsstrahlung (continuum) is not present due to the absence of the Cu target.<\/em><\/p>\n<p>But the salient feature of the incoherent PXS is the fact that X-radiation is emitted in an ultrashort pulse with a typical temporal length of hundreds of femtoseconds (1e-13 s). Such short pulses will allow scientists to resolve the kinetics of chemical reactions on atomic scales via ultrafast hard X-ray diffraction and X-ray absorption spectroscopy techniques.<\/p>\n<p>The inherent synchronization of the X-ray pulse to the driving IR laser will make advanced optical pump-hard X-ray probe methods feasible to study a variety of complex systems such as artificial photosynthetic systems or photoactive biological molecules.<\/p>\n<p><img loading=\"lazy\" class=\"alignleft wp-image-29522\" src=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/06\/Picture-2.png\" alt=\"\" width=\"564\" height=\"305\" srcset=\"https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/06\/Picture-2.png 864w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/06\/Picture-2-300x162.png 300w, https:\/\/www.eli-beams.eu\/wp-content\/uploads\/2021\/06\/Picture-2-768x415.png 768w\" sizes=\"(max-width: 564px) 100vw, 564px\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><em>Figure 2: Concept of PXS Beamline (here Bi\/In target PXS) for operation with T-REX (Time-Resolved Experiments) end station. Montel and poly-capillary optics will focus the plasma spot onto the sample stage of the Eulerian craddle.<\/em><\/p>\n<p>&nbsp;<\/p>\n<p><strong>PXS Team:<\/strong><\/p>\n<p>\u0110\u00f4ng Du Mai<\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Thus, both line emission radiation of the specific target material and (continuous) Bremsstrahlung forms the energy spectrum of a PXS&#8230;.<\/p>\n","protected":false},"author":1,"featured_media":22393,"parent":20480,"menu_order":124,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"_links":{"self":[{"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/pages\/20485"}],"collection":[{"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/comments?post=20485"}],"version-history":[{"count":23,"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/pages\/20485\/revisions"}],"predecessor-version":[{"id":29540,"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/pages\/20485\/revisions\/29540"}],"up":[{"embeddable":true,"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/pages\/20480"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/media\/22393"}],"wp:attachment":[{"href":"https:\/\/www.eli-beams.eu\/wp-json\/wp\/v2\/media?parent=20485"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}