2015
DOI: 10.1103/physrevlett.115.187401
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THz-Frequency Modulation of the HubbardUin an Organic Mott Insulator

Abstract: Abstract:We use midinfrared pulses with stable carrier-envelope phase offset to drive molecular vibrations in the charge transfer salt ET-F2TCNQ, a prototypical one-dimensional Mott insulator. We find that the Mott gap, which is probed resonantly with 10 fs laser pulses, oscillates with the pump field. This observation reveals that molecular excitations can coherently perturb the electronic on-site interactions (Hubbard U) by changing the local orbital wave function. The gap oscillates at twice the frequency o… Show more

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Cited by 84 publications
(87 citation statements)
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“…The amplitude of the modulation of the T 1u mode quoted in Ref. 41 and used in the present work is but an order of magnitude estimate, and a more precise ab-initio determination is desirable (as well as a direct experimental determination of the transient modulation of the structure). The light excitation may also induce other relevant changes in the material besides the interaction imbalance considered here, such as more complex changes in the band-structure, a modulation of the inter-orbital Coulomb matrix element and even a direct modulation of the inverted effective Hund's coupling (due e.g.…”
Section: Discussionmentioning
confidence: 85%
“…The amplitude of the modulation of the T 1u mode quoted in Ref. 41 and used in the present work is but an order of magnitude estimate, and a more precise ab-initio determination is desirable (as well as a direct experimental determination of the transient modulation of the structure). The light excitation may also induce other relevant changes in the material besides the interaction imbalance considered here, such as more complex changes in the band-structure, a modulation of the inter-orbital Coulomb matrix element and even a direct modulation of the inverted effective Hund's coupling (due e.g.…”
Section: Discussionmentioning
confidence: 85%
“…The system Hamiltonian H sys (t) consists of the unperturbed part H sys,0 and the external periodic field H ext (t). Here, we focus on a simple but relevant example of an electron-phonon coupled system, the Holstein model, with the Hamiltonian (2) where c † i is the creation operator for an electron with spin σ at site i, v is the electron hopping, μ is the electron chemical potential, n i = c another phonon mode (Raman mode) that is linearly coupled to the electron sector [11,36] or through a nonlinear-coupling mechanism [8,13,37]. Our present interest is in the former case.…”
Section: Modelmentioning
confidence: 99%
“…The pulse duration of visible radiation, which can be in the range of 4-40 fs, also enables indirect access to resonant modes in the infrared spectral range such as coherent phonons and Raman active modes [64,65]. Additionally, ultra short light pulses can be used for sub-cycle interrogation of processes excited with carrier envelope phase stable mid-IR [66] and THz pulses [55]. We stress that the efficient background suppression afforded by TrpHD with pulsed laser sources may find use in a wide array of spectroscopic measurements in addition to time-resolved control and interrogation of matter at the nanoscale.…”
Section: Outlook and Conclusionmentioning
confidence: 99%