2005 Quantum Electronics and Laser Science Conference
DOI: 10.1109/qels.2005.1548925
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Optically induced lattice dynamics probed with ultrafast X-ray diffraction

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Cited by 5 publications
(6 citation statements)
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“…Instead, we find a splitting of the initial Bragg peak into two distinct reflections at intermediate times until the initial peak has disappeared. Similar Bragg peak splittings have been previously observed in photoexcited bulk crystals and thin films 4,43,44 , however, either the signatures were relatively weak compared to the bulk reflection or a thorough description of the underlying structural dynamics is missing. The comparison of the experimental results in Fig.…”
Section: Resultssupporting
confidence: 77%
“…Instead, we find a splitting of the initial Bragg peak into two distinct reflections at intermediate times until the initial peak has disappeared. Similar Bragg peak splittings have been previously observed in photoexcited bulk crystals and thin films 4,43,44 , however, either the signatures were relatively weak compared to the bulk reflection or a thorough description of the underlying structural dynamics is missing. The comparison of the experimental results in Fig.…”
Section: Resultssupporting
confidence: 77%
“…The effective expansion coefficient valid for heating a thin epitaxial layer is based on the lattice constants and strains predicted from equilibrium thermal expansion coefficients, corrected according to the Poisson effect 53 . In cubic materials with (100) surface orientation the ratio of the observed ultrafast (uf) strain and the strain ε eq = α eq ( T )Δ T along the (100) direction calculated from equilibrium value (eq) is ε / ε eq = α uf ( T )/ α eq ( T ) = 1 + 2 C 12 / C 11 = 2.2 for Ni and would be 2.6 for Au.…”
Section: Methodsmentioning
confidence: 99%
“…Light-matter interactions can be utilized to induce ultrafast phenomena in correlated electron materials 1 for realizing functionalities that can neither be observed in bulk equilibrium 2 3 4 5 nor by means of static perturbations to the structure, including chemical substitution, mechanical strain, or digital heterostructures. Inducing nonequilibrium phonon modulations are of particular recent interest owing to their direct 6 and indirect 7 8 9 10 accessibility with high intensity femtosecond laser pulses ranging from the mid-infrared (IR) to terahertz regimes 11 . This athermal light-enabled structure–property control, for example, has been exploited in the superconducting cuprate family, where the electron pairing strength is related to the Cu-O intra-bilayer distance 12 : Mid-IR pulses are able to induce transient high- T C superconductivity from a nominally non-superconducting material 13 or melt charge order in a superconducting cuprate at subpicosecond timescales 14 by direct excitation of IR-active Cu–O bond stretching modes.…”
mentioning
confidence: 99%