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{{AFC submission|d|v|u=LaylabDL|ns=118|decliner=ToadetteEdit|declinets=20250526064059|ts=20250304133009}} <!-- Do not remove this line! -->
{{AFC submission|d|reason|Thus article contains major errors of fact. Diffuse scattering is an established technique and very different, as is wide angle scattering (in any form); they are not subsets of this. It is also poorly constructed as a how-to guide for novices. Please read more about the fundamentals of XRD before revising.|u=LaylabDL|ns=118|decliner=Ldm1954|declinets=20250202111112|small=yes|ts=20250129112127}} <!-- Do not remove this line! -->
{{AFC comment|1=The editors have ignored the comments about how-to guides, these are not allowed on Wikipedia. There is still masses of unsourced material and peacock. This is a promo page for the technique, not a proper encyclopedic draft. [[User:Ldm1954|Ldm1954]] ([[User talk:Ldm1954|talk]]) 14:26, 4 March 2025 (UTC)}}
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{{Short description|measurement technique, scattering, X-rays}}
{{Draft topics|chemistry}}
{{AfC topic|stem}}
Time-Resolved X-ray Solution Scattering (TR-XSS), also known as
Hwan Kim, Kyung, et al. "Topical Review: Molecular reaction and solvation visualized by time-resolved X-ray solution scattering: Structure, dynamics, and their solvent dependence." Structural Dynamics 1.1 (2014).
</ref>
Historically, TR-XSS was also called X-ray Diffuse Scattering (XDS)<ref name="source1">Haldrup, Kristoffer, et al. "Observing solvation dynamics with simultaneous femtosecond X-ray emission spectroscopy and X-ray scattering." The journal of physical chemistry B 120.6 (2016): 1158-1168.</ref> to differentiate scattering of an unordered system (e.g. liquid) from solid state scattering. However, due to existing use of the term diffuse scattering from disorder the term is no longer in use.
== Pump-Probe Technique ==
{{Sources needed|Section|date=March 2025}}
TR-XSS is a pump-probe technique, in which the liquid sample is first excited with a short laser pulse and subsequently probed with a short X-ray pulse. The liquid sample contains low concentrations (~1-100 mM) of a solute molecule in solution, which is delivered to the beam interaction region either by a liquid jet or through a capillary. A continuous supply of new sample through the delivery system avoids radiation damage by the X-ray and laser pulses. The intensity I(θ) of the [[X-ray_diffraction|X-rays]] scattered on the sample is recorded as a function of the scattering angle θ with a two dimensional X-ray detector. To capture small structural changes in real space (like sub-angstrom bong elongations in a molecule), large scattering angles (0°-60°) in the reciprocal space are detected. Thus, TR-XSS experiments are recorded in wide-angle X-ray scattering (WAXS) geometry.
The intensity distribution of scattered light contains information on all molecules in the liquid sample, including the target molecule for the investigation (solute) as well as the solvent molecules surrounding it ([[solvation shell]]) and all solvent molecules. To highlight the information gathered on the excited solute molecules, detector images with scattering patterns I(θ) from the sample in the [[ground state]] (I<sub>''laser off''</sub>) are subtracted from scattering pattern after [[Excited_state|exciting]] the solute with a pump laser (I<sub>''laser on''</sub>). The difference intensity
ΔI(θ,Δt) = I<sub>''laser off''</sub> (θ) – I<sub>''laser on''</sub>(θ,Δt)
only contains intensity contributions from the excited solute and solvation shell molecules, which reacted to the chemical reaction triggered by the laser pulse. By changing the delay time Δt between pump and probe pulse, snapshots of different stages of the structural dynamic of the excitation progress can be captured. In the end, those snapshots are combined to construct a [[The_Horse_in_Motion|movie of the observed]] chemical reaction.
== Application ==
{{Prose|date=March 2025|section}}
• [[Dye-sensitized_solar_cell|Dye-sensitised solar cells]]. Fundamental research on structural processes in ruthenium-based and iron-based solar cells
• [[Molecular_switch|Molecular switching]] materials.
• [[Protein_structure|Protein Structural]] Dynamics
• Charge-transfer-to-solvent reactions in solvents.
• Light-induced molecular [[Dissociation_(chemistry)|dissociation reactions]] or complex formations
• [[
== Complementary techniques ==
TR-XSS can deliver real-time information on [[Molecular_geometry|molecular structures]]. Additional information on electronic structure can be obtained by combining the technique with X-ray Absorption Spectroscopy ([[X-ray_absorption_spectroscopy|XAS]]) or X-ray Emission Spectroscopy ([[X-ray_emission_spectroscopy|XES]]) recorded at the same time
== Prerequisites/Limitations ==
{{Sources needed|Section|date=March 2025}}
TR-XSS is a pump-probe technique. It requires a pulsed laser to excite chemical reactions in a solution as well as a pulsed X-ray source of high peak brilliance for the probe. The time-resolution depends on the pulse with of the X-rays and the laser, as well as on the thickness of the probed sample. Examples of experimental setups capable of the technique can be found at [[Synchrotron|synchrotrons]] (ID09 at [[European Synchrotron Radiation Facility|ESRF]], [[Advanced Photon Source|APS]]), laboratory sources
For a solution to be investigated with TR-XSS, the dissolved molecules need to absorb light at the wavelength of the pump laser, while the surrounding solvent ideally does not absorb at the same laser wavelength. Additionally, molecules including heavy atoms (e.g. metals) scatter more X-ray photons than light elements, thus the recorded signals become larger and easier to analyze.
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