2021
DOI: 10.1515/nanoph-2021-0242
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Coherent control at gold needle tips approaching the strong-field regime

Abstract: We demonstrate coherent control in photoemission from a gold needle tip using an ω − 2ω field composed of strong few-cycle laser pulses with a nearfield intensity of ∼4 TW/cm2. We obtain the nearfield intensity from electron energy spectra, showing the tell-tale plateau of field-driven electron rescattering at the metal surface induced by the fundamental field. Changing the relative phase between the fundamental field centered at 1560 nm and its second harmonic modulates the total emitted photocurrent with vis… Show more

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Cited by 9 publications
(10 citation statements)
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“…Taking advantage of the shaper's capability to additionally introduce higher order spectral phase modulation, the trichromatic scheme can be further developed into a powerful tool for coherent control spectroscopy by using sequences of tailored pulses, thus generalizing the concept of 2D spectroscopy. In addition, the tunability of the shaper-generated polarization-controlled multicolor fields makes them attractive for applications in quantum information [222], quantum metrology [109,110,223] and ultrafast nanotechnology [79,178,214,224,225]. In all the experiments reported above, the tailored polarization profile was confined to the (x, y)-plane perpendicular to the propagation direction of the pulse.…”
Section: Discussionmentioning
confidence: 99%
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“…Taking advantage of the shaper's capability to additionally introduce higher order spectral phase modulation, the trichromatic scheme can be further developed into a powerful tool for coherent control spectroscopy by using sequences of tailored pulses, thus generalizing the concept of 2D spectroscopy. In addition, the tunability of the shaper-generated polarization-controlled multicolor fields makes them attractive for applications in quantum information [222], quantum metrology [109,110,223] and ultrafast nanotechnology [79,178,214,224,225]. In all the experiments reported above, the tailored polarization profile was confined to the (x, y)-plane perpendicular to the propagation direction of the pulse.…”
Section: Discussionmentioning
confidence: 99%
“…The applications of polarization-tailored bichromatic fields are as versatile as their shapes. For example, PLP bichromatic fields were applied to control plasmonenhanced photoemission from silver clusters [178] and strongfield photoemission from gold nanotips [79]. OLP bichromatic fields with commensurable frequencies, characterized by Lissajous-type polarization profiles which exhibit a timevarying optical chirality, have been used to investigate subcycle variations in the PECD of chiral molecules [179,180].…”
Section: Bichromatic Pulse Sequencesmentioning
confidence: 99%
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“…The interaction of electrons with intense laser fields of peak optical field strengths larger than 1 GV/m has become a broad, mature research area, , which has opened the exciting fields of attosecond physics and attosecond nanophysics. The underlying mechanism of inelastic and elastic rescattering of laser-driven electrons with the parent gas atoms or parent solid matter is well-explained by the three-step model (TSM) of strong-field physics. High-harmonic generation (HHG) can take place, and high-energy electrons can be produced . In the case of metallic nanoemitters, despite being a complex solid-state system, ultrafast and multiphoton emission, above-threshold photoemission, and strong-field photoemission , have been experimentally demonstrated. Using nanometer sharp needle tips as electron emitters, the existence of local near-field enhancement , allows reaching the strong-field photoemission regime without the need for amplifier laser systems with μJ or even greater pulse energies.…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, we expect this estimation to also hold for atoms, where the extension of the wave function in vacuum dominates the interaction duration ∆t, which can be varied by changing the height of the ionisation potential. Additionally, the field enhancement factors are determined experimentally in another ongoing work [40], where the field enhancement factors are directly evaluated from the scaling of the cut-off energy in strong-field electron energy spectra. The experimentally obtained field enhancement factors ξ 1560nm = 5.5 ± 0.8 and ξ 780nm = 2.8 ± 0.4, together with Γ 780nm = 1.3 × 10 11 W cm −2 from the fit curve in Fig.…”
mentioning
confidence: 99%