2019
DOI: 10.1038/s41567-018-0385-4
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Leggett mode controlled by light pulses

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Cited by 79 publications
(106 citation statements)
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“…As a consequence, for broadband pulses the spectral components of δE probe (t pp ) are dominated by the characteristic frequency of the mode, ω osc = ω res , while for narrowband pulses δE probe (t pp ) oscillates at twice the pump frequency, ω osc = 2Ω pump , with an amplitude K(2Ω pump ) maximized when 2Ω pump = ω res . These expectations match rather well the observations reported so far in several SC systems [4][5][6][7][8] . From the theoretical point of view, establishing such a general paradigm provides also a scheme for further theoretical investigations aimed at linking the experimental observations to the properties of the underlying microscopic model.…”
supporting
confidence: 92%
See 1 more Smart Citation
“…As a consequence, for broadband pulses the spectral components of δE probe (t pp ) are dominated by the characteristic frequency of the mode, ω osc = ω res , while for narrowband pulses δE probe (t pp ) oscillates at twice the pump frequency, ω osc = 2Ω pump , with an amplitude K(2Ω pump ) maximized when 2Ω pump = ω res . These expectations match rather well the observations reported so far in several SC systems [4][5][6][7][8] . From the theoretical point of view, establishing such a general paradigm provides also a scheme for further theoretical investigations aimed at linking the experimental observations to the properties of the underlying microscopic model.…”
supporting
confidence: 92%
“…The present work aims at filling in part this knowl- * mattia.udina@uniroma1.it † tommaso.cea@imdea.org ‡ lara.benfatto@roma1.infn.it edge gap by providing a general theoretical scheme to understand the origin of time-resolved oscillations observed in typical TH pump-THz/eV probe measurements. This experimental technique has been successfully applied in the last years to investigate the properties of both conventional superconducting (SC) compounds [4][5][6][7][8][9] , whose spectral gap ∆ lies in the THz region, and layered superconductors 10,11 with an interlayer Josephson plasma frequency again in the THz range. The general scheme consists in probing the effects of the intense THz pulse by measuring the pump-induced changes δE probe (t pp ) in the transmitted (for a thin film) or reflected (for a bulk crystal) probe field at a fixed observation time, as a function of the pump-probe delay t pp .…”
mentioning
confidence: 99%
“…An experimental observation of Leggett collective excitations is a challenging problem, because they, in general, have relatively small spectral weights or high decay rates. Leggett modes have been detected in a two-band superconductor MgB 2 using Raman [2] and tunneling [3] spectroscopy, and, recently, using intense terahertz lights pulses [4]. In the experimentally realized two-band 173 Yb cold atomic gases with OFR, Leggett collective excitations can be hardly resolved, because they are strongly damped in the experimentally achieved stable out-of-phase state [13].…”
Section: Discussionmentioning
confidence: 99%
“…Leggett modes were experimentally detected in multiband superconductors [2][3][4]. The two-band superfluidity and Leggett collective modes have been considered theoretically for superconducting MgB 2 [5] and for condensed Fermi gases in the BCS-BEC crossover [6,7].…”
Section: Introductionmentioning
confidence: 99%
“…Finally, in addition to the Higgs mode, unconventional superconductors with reduced dimensionality and multi-band superconductors may host a much richer spectrum of collective excitations [142,157,158]. The first experiments, suggesting the observation of the collective oscillation of the relative phase between the order parameters in a two-band superconductor MgB 2 , the Leggett mode, have just been reported [159].…”
Section: Summary and Perspectivesmentioning
confidence: 99%