Anthony DiChiara

Imaging ultrafast molecular dynamics with laser-induced electron diffraction

Establishing the structure of molecules and solids has always had an essential role in physics, chemistry and biology. The methods of choice are X-ray and electron diffraction, which are routinely used to determine atomic positions with sub-ångström spatial resolution. Although both methods are currently limited to probing dynamics on timescales longer than a picosecond, the recent development of femtosecond sources of X-ray pulses and electron beams suggests that they might soon be capable of taking ultrafast snapshots of biological molecules and condensed-phase systems undergoing structural changes. The past decade has also witnessed the emergence of an alternative imaging approach based on laser-ionized bursts of coherent electron wave packets that self-interrogate the parent molecular structure. Here we show that this phenomenon can indeed be exploited for laser-induced electron diffraction (LIED), to image molecular structures with sub-ångström precision and exposure times of a few femtoseconds. We apply the method to oxygen and nitrogen molecules, which on strong-field ionization at three mid-infrared wavelengths (1.7, 2.0 and 2.3 μm) emit photoelectrons with a momentum distribution from which we extract diffraction patterns. The long wavelength is essential for achieving atomic-scale spatial resolution, and the wavelength variation is equivalent to taking snapshots at different times. We show that the method has the sensitivity to measure a 0.1 Å displacement in the oxygen bond length occurring in a time interval of ∼5 fs, which establishes LIED as a promising approach for the imaging of gas-phase molecules with unprecedented spatio-temporal resolution.

Strong-field and attosecond physics in solids

We review the status of strong-field and attosecond processes in bulk transparent solids near the Keldysh tunneling limit. For high enough fields and low-frequency excitations, the optical and electronic properties of dielectrics can be transiently and reversibly modified within the applied pulse. In Ghimire et al (2011 Phys. Rev. Lett. 107 167407) non-parabolic band effects were seen in photon-assisted tunneling experiments in ZnO crystals in a strong mid-infrared field. Using the same ZnO crystals, Ghimire et al (2011 Nat. Phys. 7 138–41) reported the first observation of non-pertubative high harmonics, extending well above the bandgap into the vacuum ultraviolet. Recent experiments by Schubert et al (2014 Nat. Photonics 8 119–23) showed a carrier envelope phase dependence in the harmonic spectrum in strong-field 30 THz driven GaSe crystals which is the most direct evidence yet of the role of sub-cycle electron dynamics in solid-state harmonic generation. The harmonic generation mechanism is different from the gas phase owing to the high density and periodicity of the crystal. For example, this results in a linear dependence of the high-energy cutoff with the applied field in contrast to the quadratic dependence in the gas phase. Sub-100 attosecond pulses could become possible if the harmonic spectrum can be extended into the extreme ultraviolet (XUV). Here we report harmonics generated in bulk MgO crystals, extending to ∼26 eV when driven by ∼35 fs, 800 nm pulses focused to a ∼1VA −1 peak field. The fundamental strong-field and attosecond response also leads to Wannier–Stark localization and reversible semimetallization as seen in the sub-optical cycle behavior of XUV absorption and photocurrent experiments on fused silica by Schiffrin et al (2013 Nature 493 70–4) and Schultze et al (2013 Nature 493 75–8). These studies are advancing our understanding of fundamental strong-field and attosecond physics in solids with potential applications for compact coherent short-wavelength sources and ultra-high speed optoelectronics.

An investigation of harmonic generation in liquid media with a mid-infrared laser

We present a harmonic generation experiment using liquid H(2)O and D(2)O interrogated by a mid-infrared, 3.66 mum, laser at a maximum intensity of 8x10(13) W/cm(2). The unique aspects of the experiment include the long wavelength and short (9 cycle-110 fs) pulse duration of the laser as well as the near-resonant excitation of the H(2)O and D(2)O vibrational modes. We observe up to the 13th harmonic order in H(2)O and intensity scaling is consistent with a direct perturbative process up to the 9th harmonic order. Phase matching and resonant absorption are unable to account for the observed differences in harmonic yields between samples.

Inelastic scattering of broadband electron wave packets driven by an intense midinfrared laser field.

Intense, 100 fs laser pulses at 3.2 and 3.6 μm are used to generate, by multiphoton ionization, broadband wave packets with up to 400 eV of kinetic energy and charge states up to Xe(+6). The multiple ionization pathways are well described by a white electron wave packet and field-free inelastic cross sections, averaged over the intensity-dependent energy distribution for (e, ne) electron impact ionization. The analysis also suggests a contribution from a 4d core excitation, or giant resonance, in xenon.

Scaling of High-Order Harmonic Generation in the Long Wavelength Limit of a Strong Laser Field

The development of intense, ultrashort, table-top lasers operating in the mid-infrared spectral region, offers many new avenues for strong-field physics. Atoms submitted to such radiation allow photoelectrons to acquire huge quiver energies well over an order of magnitude larger than the binding energy of the neutral. Consequently, many interesting phenomena arise. First, wavelength offers a convenient experimental knob to tune the ionization regime by controlling the Keldysh parameter. Second, high harmonic generation depends directly on the quiver energy and can, therefore, be pushed to unprecedented limits. Third, wavelength controls the spectral phase of harmonics, and hence the possibility to improve the generation of pulses in the attosecond regime. The use of long wavelength lasers is critical to studying high-order harmonic generation in condensed phase systems, because they facilitate harmonic generation within the transmission window of the material and increase the damage threshold. We review some of the recent discoveries in long wavelength driven high-order harmonic generation in the case of isolated atoms, bulk crystals, and liquid.

High-harmonic generation in strongly driven bulk periodic solid

We report on high-order harmonic generation from bulk zinc-oxide driven by a strong mid-infrared laser pulse. The harmonic spectra extend well above the band-gap and scales non-perturbatively with the laser intensity.

Photoionization by an ultraintense laser field: Response of atomic xenon

We present energy- and angle-resolved photoionization from Xe in an ultrastrong laser field at 10{sup 19} W/cm{sup 2}. The observed yields are consistent with the tunneling ionization of Xe{sup 9+} to Xe{sup 24+}. However, energy and angle-resolved photoelectron spectra show differences for electrons whose final energies are above or below 0.5 MeV, which is approximately the ponderomotive energy at these intensities. Above 0.5 MeV, the observed photoelectron cutoff energy (between 1 and 1.35 MeV), photoelectron energy spectra, and the angle-resolved photoelectron azimuthal distributions agree with a model using tunneling ionization, multiple charge states, a classical relativistic continuum, and nonparaxial three-dimensional (3D) focused laser field. Below 0.5 MeV the yields and angular distributions observed indicate dynamics not included within a classical, single electron model of the interaction.

Strong-Field and Attosecond Physics with Mid-infrared Lasers

This chapter reviews electron energy spectra, multiple ionization, harmonic generation and attophysics as they are modified by scaling the interaction physics to longer driving wavelengths. After a brief outline of the development of mid-infared sources, we discuss findings on Above Threshold Ionization (ATI) and multiple ionization as an (e, ne) process. We then review the properties of high harmonic generation (HHG) in gas phase from the point of view of the highest frequency and the group delay dispersion, both relevant to attophysics. We have explored other generating media and report HHG from crystal and liquid samples. We conclude with a brief outlook of both the laser development and attophysics with MIR sources.

Strong-field effects in solids

We present results of non-perturbative high-order harmonic generation and photon-assisted tunneling driven by intense mid-infrared laser in solids. These strong-field effects are intimately related and occur in a limit where the laser-field competes with crystal bonding.

Strong-field induced optical absorption in ZnO crystal

We report the observation of intensity dependent red shift on the absorption-edge of zinc-oxide driven by a mid-infrared laser pulse. A new regime is identified where the shift is no longer linear to the intensity.