001     596416
005     20231115211045.0
024 7 _ |a urn:nbn:de:gbv:18-ediss-112508
|2 URN
024 7 _ |a 10.3204/PUBDB-2023-06144
|2 datacite_doi
037 _ _ |a PUBDB-2023-06144
041 _ _ |a English
100 1 _ |a Trost, Fabian
|0 P:(DE-H253)PIP1082226
|b 0
|e Corresponding author
|g male
245 _ _ |a Imaging via photon-photon correlation of X-ray fluorescence
|f 2017-10-01 - 2023-09-18
260 _ _ |c 2023
300 _ _ |a 146
336 7 _ |a Output Types/Dissertation
|2 DataCite
336 7 _ |a DISSERTATION
|2 ORCID
336 7 _ |a PHDTHESIS
|2 BibTeX
336 7 _ |a Thesis
|0 2
|2 EndNote
336 7 _ |a Dissertation / PhD Thesis
|b phd
|m phd
|0 PUB:(DE-HGF)11
|s 1700050380_16735
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336 7 _ |a doctoralThesis
|2 DRIVER
502 _ _ |a Dissertation, University of Hamburg, 2023
|c University of Hamburg
|b Dissertation
|d 2023
|o 2023-09-18
520 _ _ |a This work discusses and demonstrates the imaging method ‘photon-photon correlation of X-ray fluorescence’, also called ‘Incoherent Diffraction Imaging (IDI)’. This method corresponds to the ‘intensity interferometry’, known from astronomy. However, this method requires measurement or exposure times that are on the order of the coherence time of the measured radiation; for Kα fluorescence of light transition metals, this is on the order of a femtosecond – a temporal length that can be achieved by modern X-ray free electron lasers (XFELs).In addition to the exposure time requirement, this work discusses other influencing factors that can cause a reduction in the useful correlation signal. These are the temporal shape of the excitation pulse, the sample size, the (non) polarization of the detected photons, and others. These factors, collectively called ‘visibility factor’, also manifest as ‘speckle contrast’ and can be measured without the need to perform intensity correlation. A weighting method is presented to determine the speckle contrast from a data set consisting of images with very low photon counts that fluctuate significantly from image to image. This method is applied to compare the speckle contrast of iron Kα fluorescence excited by 3 fs and 15 fs XFEL pulses. An increase in speckle contrast was found for the short pulses compared to the longer ones – a fundamental requirement for the IDI method.Furthermore, inherent noise sources affecting the IDI are discussed. A model is derived to estimate the dependence of the signal-to-noise ratio (SNR) on the photon number per pixel, temporal coherence (or visibility factor), and the shape of the imaged object. In addition, simulations in two and three dimensions were performed to validate the model’s predictions. Unlike coherent imaging methods, more detected photons do not always result in higher SNR. Moreover, larger and more complex objects generally yield poorer SNR, even when the number of measured photons is proportional to the object size or complexity.Finally, an experiment that uses the photon-photon correlation of X-ray fluorescence photons for the first time to reconstruct a nontrivial (noncontinuous) fluorescence emitter distribution is presented. In the course of this experiment, the application of IDI to determine XFEL beam parameters such as focus and temporal pulse length is demonstrated.
536 _ _ |a 633 - Life Sciences – Building Blocks of Life: Structure and Function (POF4-633)
|0 G:(DE-HGF)POF4-633
|c POF4-633
|f POF IV
|x 0
536 _ _ |a DFG project 390715994 - EXC 2056: CUI: Advanced Imaging of Matter (390715994)
|0 G:(GEPRIS)390715994
|c 390715994
|x 1
693 _ _ |0 EXP:(DE-H253)CFEL-Exp-20150101
|5 EXP:(DE-H253)CFEL-Exp-20150101
|e Experiments at CFEL
|x 0
693 _ _ |a XFEL
|e MID: Materials Imaging and Dynamics
|f SASE2
|1 EXP:(DE-H253)XFEL-20150101
|0 EXP:(DE-H253)XFEL-MID-20150101
|5 EXP:(DE-H253)XFEL-MID-20150101
|6 EXP:(DE-H253)XFEL-SASE2-20150101
|x 1
693 _ _ |0 EXP:(DE-MLZ)External-20140101
|5 EXP:(DE-MLZ)External-20140101
|e Measurement at external facility
|x 2
700 1 _ |a Chapman, Henry N.
|0 P:(DE-H253)PIP1006324
|b 1
|e Thesis advisor
700 1 _ |a Roehlsberger, Ralf
|0 P:(DE-H253)PIP1000401
|b 2
|e Thesis advisor
856 4 _ |u https://ediss.sub.uni-hamburg.de/handle/ediss/10509
856 4 _ |u https://bib-pubdb1.desy.de/record/596416/files/Thesis_Fabian.pdf
|y OpenAccess
856 4 _ |u https://bib-pubdb1.desy.de/record/596416/files/Thesis_Fabian.pdf?subformat=pdfa
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|y OpenAccess
909 C O |o oai:bib-pubdb1.desy.de:596416
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910 1 _ |a Centre for Free-Electron Laser Science
|0 I:(DE-H253)_CFEL-20120731
|k CFEL
|b 0
|6 P:(DE-H253)PIP1082226
910 1 _ |a Deutsches Elektronen-Synchrotron
|0 I:(DE-588b)2008985-5
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910 1 _ |a Centre for Free-Electron Laser Science
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910 1 _ |a European XFEL
|0 I:(DE-588)1043621512
|k XFEL.EU
|b 1
|6 P:(DE-H253)PIP1006324
910 1 _ |a Deutsches Elektronen-Synchrotron
|0 I:(DE-588b)2008985-5
|k DESY
|b 2
|6 P:(DE-H253)PIP1000401
910 1 _ |a European XFEL
|0 I:(DE-588)1043621512
|k XFEL.EU
|b 2
|6 P:(DE-H253)PIP1000401
913 1 _ |a DE-HGF
|b Forschungsbereich Materie
|l Von Materie zu Materialien und Leben
|1 G:(DE-HGF)POF4-630
|0 G:(DE-HGF)POF4-633
|3 G:(DE-HGF)POF4
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|v Life Sciences – Building Blocks of Life: Structure and Function
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914 1 _ |y 2023
915 _ _ |a OpenAccess
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915 _ _ |a Creative Commons Attribution CC BY 4.0
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920 _ _ |l yes
920 1 _ |0 I:(DE-H253)FS-CFEL-1-20120731
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980 _ _ |a phd
980 _ _ |a VDB
980 _ _ |a UNRESTRICTED
980 _ _ |a I:(DE-H253)FS-CFEL-1-20120731
980 1 _ |a FullTexts


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