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Photon bunching in high-harmonic emission controlled by quantum light
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Attosecond spectroscopy comprises several techniques to probe matter through electrons and photons. One frontier of attosecond methods is to reveal complex phenomena arising from quantum-mechanical correlations in the matter system, in the photon fields and among them. Recent theories have laid the groundwork for understanding how quantum-optical properties affect high-field photonics, such as strong-field ionization and acceleration of electrons in quantum-optical fields, and how entanglement between the field modes arises during the interaction. Here we demonstrate a new experimental approach that transduces some properties of a quantum-optical state through a strong-field nonlinearity. We perturb high-harmonic emission from a semiconductor with a bright squeezed vacuum field resulting in the emission of sidebands of the high-harmonics with super-Poissonian statistics, indicating that the emitted photons are bunched. Our results suggest that perturbing strong-field dynamics with quantum-optical states is a viable way to coherently control the generation of these states at short wavelengths, such as extreme ultraviolet or soft X-rays. Quantum correlations will be instrumental to advance attosecond spectroscopy and imaging beyond the classical limits.
Forward citations
Cited by 3 Pith papers
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Measuring and controlling the birth of quantum attosecond pulses
A two-color high-harmonic experiment imprints squeezed-vacuum statistics from an infrared beam onto XUV harmonics, enabling the first quantum-state reconstruction of an attosecond pulse.
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Quantum engineering of high harmonic generation
A closed-form quantum theory of sideband high harmonic generation predicts that projecting on one of the entangled light modes creates non-classical states such as single photons, cat states, and photon-added squeezed...
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Theory of quantum optics and optical coherence in high harmonic generation
A Heisenberg-picture quantum optical theory splits the HHG spectrum into coherent and incoherent parts and predicts single-atom photon anti-bunching with g(2)(0) near 0.005.
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