2021
DOI: 10.1038/s41567-021-01366-1
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Engineering crystal structures with light

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Cited by 133 publications
(65 citation statements)
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“…We do note that due to the spectral coverage of commercial optical parametric amplifiers (OPAs), the proposed method does not readily apply to inorganic materials that lack vibrational modes 13 shorter than 16 µm (i.e., 625 cm -1 ), although far-infrared OPAs and intense terahertz source are being actively developed for coherent phonon excitations of solids with vibrational modes in the corresponding spectral ranges. 57,58…”
Section: Discussionmentioning
confidence: 99%
“…We do note that due to the spectral coverage of commercial optical parametric amplifiers (OPAs), the proposed method does not readily apply to inorganic materials that lack vibrational modes 13 shorter than 16 µm (i.e., 625 cm -1 ), although far-infrared OPAs and intense terahertz source are being actively developed for coherent phonon excitations of solids with vibrational modes in the corresponding spectral ranges. 57,58…”
Section: Discussionmentioning
confidence: 99%
“…On the other hand, efficient absorption in the freestanding membranes could stabilize the optically induced transient phases, such as metastable ferroelectricity in paraelectric SrTiO 3 [240] or superconductivity in cuprates [241]. These phases are induced by targeting a specific mid-infrared phonon in TMO [242], yet substrate clamping can increase the phonon decay rates making the suspended samples preferrable to prolong the phase lifetimes. Moreover, the symmetric geometry of the freestanding TMO membranes would allow for the creation of nanocavities for the material's phase control via interaction with the photon vacuum fields that would not require direct optical pumping (figure 8(b)) [243].…”
Section: Light-matter Interactionsmentioning
confidence: 99%
“…Selective excitation of finite momentum X-point phonons requires considerable effort (30)(31)(32), with the experimentally easily accessible phonon excitations being the IR active phonon modes at -point. While the equilibrium EPC is negligible for these phonons, a key finding thus far is that, by itself, this cannot serve as a means to predict the strength of the dynamic coupling between preexcited phonons and demagnetization.…”
Section: Ir Active Phononsmentioning
confidence: 99%