Abstract:The free-electron laser in Hamburg, FLASH, is the first extreme ultra-violet and soft X-ray free-electron laser (FEL) user facility and has been continuously upgraded since its start in 2005. Further major works are currently underway within the FLASH2020+ project that pioneeringly implements full repetition rate external seeding at a superconducting accelerator facility. With fully tunable undulators providing variable polarization FEL pulses, we expect FLASH to turn into the ideal spectroscopy machine for ul… Show more
“…After sorting out the basic model for the pump-probe dynamics given by Equation (60) with basis functions described in Equation ( 67), we are ready to account for deviations of the dynamics from delta-shaped pump-probe measurements. There are two main reasons why real experimental observations do not exactly follow the trends described in Section 3.2 [41,[48][49][50]]:…”
Section: Accounting For Finite Duration Of the Pulses And Experiments...mentioning
confidence: 99%
“…The last additional function, describing a transient coherent oscillation ("to"), can be taken from Equation (57): 61)-( 66), we can describe any pump-probe observable using expression (60). In the previous discussion, we assumed that the pump pulse only initialized the dynamics and that the probe pulse only changed the species produced with the pump.…”
Ultrafast pump–probe spectroscopic studies allow for deep insights into the mechanisms and timescales of photophysical and photochemical processes. Extracting valuable information from these studies, such as reactive intermediates’ lifetimes and coherent oscillation frequencies, is an example of the inverse problems of chemical kinetics. This article describes a consistent approach for solving this inverse problem that avoids the common obstacles of simple least-squares fitting that can lead to unreliable results. The presented approach is based on the regularized Markov Chain Monte-Carlo sampling for the strongly nonlinear parameters, allowing for a straightforward solution of the ill-posed nonlinear inverse problem. The software to implement the described fitting routine is introduced and the numerical examples of its application are given. We will also touch on critical experimental parameters, such as the temporal overlap of pulses and cross-correlation time and their connection to the minimal reachable time resolution.
“…After sorting out the basic model for the pump-probe dynamics given by Equation (60) with basis functions described in Equation ( 67), we are ready to account for deviations of the dynamics from delta-shaped pump-probe measurements. There are two main reasons why real experimental observations do not exactly follow the trends described in Section 3.2 [41,[48][49][50]]:…”
Section: Accounting For Finite Duration Of the Pulses And Experiments...mentioning
confidence: 99%
“…The last additional function, describing a transient coherent oscillation ("to"), can be taken from Equation (57): 61)-( 66), we can describe any pump-probe observable using expression (60). In the previous discussion, we assumed that the pump pulse only initialized the dynamics and that the probe pulse only changed the species produced with the pump.…”
Ultrafast pump–probe spectroscopic studies allow for deep insights into the mechanisms and timescales of photophysical and photochemical processes. Extracting valuable information from these studies, such as reactive intermediates’ lifetimes and coherent oscillation frequencies, is an example of the inverse problems of chemical kinetics. This article describes a consistent approach for solving this inverse problem that avoids the common obstacles of simple least-squares fitting that can lead to unreliable results. The presented approach is based on the regularized Markov Chain Monte-Carlo sampling for the strongly nonlinear parameters, allowing for a straightforward solution of the ill-posed nonlinear inverse problem. The software to implement the described fitting routine is introduced and the numerical examples of its application are given. We will also touch on critical experimental parameters, such as the temporal overlap of pulses and cross-correlation time and their connection to the minimal reachable time resolution.
“…Alternatively, one could use free-electron laser sources, such as specific IR and THz facilities 93,94 or THz-undulator sources at X-ray free-electron lasers. 95 This could be especially interesting to extend the proposed studies to lower-energy-photon excitations, at the cost of limited accessibility to beamtime at facilities.…”
Section: Ultrashort Mid-ir Pulses For Inducing Thermal-energy Excitat...mentioning
confidence: 99%
“…134,[136][137][138] CDI was also demonstrated for small gas-phase molecules, 9,139,140 based on access to the molecular frame through the imaging of laser-aligned species. 9,[141][142][143] Assuming that analyzable gas-phase diffraction patterns can be captured in hours, if not minutes, 36,144 and the recent drive to develop and integrate THz/mid-IR sources at FEL experimental endstations to deliver thermal-energy-scale pump pulses, 95 coupled with Stark deflectors for separating out specific molecular species, 9 the coherent-diffractive imaging of thermal-energy induced reactions at FELs is closer than ever.…”
Section: B Atomic-resolution Diffractive Imagingmentioning
In this perspective, we discuss how one can initiate, image, and disentangle the ultrafast elementary steps of thermal-energy chemical dynamics, building upon advances in technology and scientific insight. We propose...
“…In the case of CS 2 , the spectral overlap and varying ionization cross sections of different fragments present some challenges for TRXPS in separating their individual contributions. This motivates the use of channel-resolved analysis techniques such as electron–ion covariance to correlate weaker photoelectron spectral signatures to particular ionic fragments in a background-free manner. ,, TRXPS will also benefit greatly from the ongoing developments in seeded and high-repetition rate FELs, allowing large volumes of data to be recorded at high energy resolution in a short acquisition period. This will further increase the applicability of TRXPS, for instance, by enabling one to scan the probe photon energy and thus probe various core sites within a molecule during a single experiment.…”
Recent developments in X-ray free-electron lasers have
enabled
a novel site-selective probe of coupled nuclear and electronic dynamics
in photoexcited molecules, time-resolved X-ray photoelectron spectroscopy
(TRXPS). We present results from a joint experimental and theoretical
TRXPS study of the well-characterized ultraviolet photodissociation
of CS2, a prototypical system for understanding non-adiabatic
dynamics. These results demonstrate that the sulfur 2p binding energy
is sensitive to changes in the nuclear structure following photoexcitation,
which ultimately leads to dissociation into CS and S photoproducts.
We are able to assign the main X-ray spectroscopic features to the
CS and S products via comparison to a first-principles determination
of the TRXPS based on ab initio multiple-spawning
simulations. Our results demonstrate the use of TRXPS as a local probe
of complex ultrafast photodissociation dynamics involving multimodal
vibrational coupling, nonradiative transitions between electronic
states, and multiple final product channels.
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