Nadine Dörre’s research while affiliated with University of Vienna and other places

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Publications (12)


Phase-Matched Extreme-Ultraviolet Frequency-Comb Generation
  • Conference Paper
  • Full-text available

January 2019

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77 Reads

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6 Citations

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S.B. Schoun

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We achieve phase-matched high-harmonic generation at 77 MHz repetition rate, by using high-temperature gas mixtures to increase gas-jet velocity and reduce plasma accumulation. We generate record power of ~2mW at 97nm and ~0.9mW at 67nm.

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Plasma dynamics in high-repetition-rate high-harmonic generation
a, Overview. A train of femtosecond laser pulses crosses and ionizes a xenon gas jet. The interval between consecutive pulses, τrep = 1/frep, is smaller than the plasma transit time through the ionization volume, resulting in a high steady-state ionization fraction, ηsteady. b, Spatially averaged steady-state ionization fraction, ηsteady (colour scale), as a function of peak laser intensity and the number of laser pulses that cross the gas jet during the gas transit time through the laser beam, ξbeam = τbeam/τrep. The contour lines show the intensity-dependent number of laser pulses ξion = τion/τrep that cross the gas jet during the time it takes an ion to clear the ion-generation volume, as illustrated in the inset. The black diamond (ηsteady = 17%), blue square (ηsteady = 11%), green circle (ηsteady = 1.1%) and purple triangle (ηsteady = 0.2%) indicate experimental conditions of optimal 11th harmonic yield for various gas and laser parameters.
Phase-matching high-repetition-rate high-harmonic generation
a, Phase-matching figure-of-merit, spatially averaged over the beam profile, at the peak of the laser pulse, Labs/Lcoh (colour scale and contour lines), for the 11th harmonic, as a function of peak laser intensity and ξbeam. Phase matching requires Labs/Lcoh ≲ 0.2 (ref. ⁵). The markers correspond to the same experimental conditions as displayed in Fig. 1b. b,c, Measured 11th and 17th harmonic power versus partial xenon backing pressure. d,e, The macroscopic response Smac, which is the measured harmonic power divided by the measured single-atom response. The overturning peaks in the 9:1 He:Xe gas mix curves in d and e indicate phase matching.
Power scaling of high-repetition-rate high-harmonic generation
a, Experimentally generated 11th and 17th harmonic power as a function of ξbeam for experimental conditions with different repetition rates (filled and open markers correspond to 154 and 77 MHz, respectively), He:Xe gas mixes, and gas temperatures. Each point corresponds to the peak of a pressure-curve analogous to Fig. 2b,c. The insets show the intracavity laser power while sweeping over the cavity resonance with gas (black) and without gas (grey) for the smallest and largest ξbeam. b, Overview of experimentally generated power per harmonic above 10 eV at repetition rates above 1 MHz, in the single-pass configuration (circles)29–31 and the intracavity configuration (triangles)10,12,32,33,35. The photon energy is indicated by the marker colour. For the cases where the cavity out-coupling efficiency was not reported, we assume 10% and 5% for the Brewster plate out-coupler¹⁰ and the hole mirror³², respectively.
Phase-matched extreme-ultraviolet frequency-comb generation

July 2018

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502 Reads

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124 Citations

Nature Photonics

Laser-driven high-order harmonic generation (HHG) provides tabletop sources of broadband extreme-ultraviolet (XUV) light with excellent spatial and temporal coherence. These sources are typically operated at low repetition rates, frepf_{rep}\lesssim100 kHz, where phase-matched frequency conversion into the XUV is readily achieved. However, there are many applications that demand the improved counting statistics or frequency-comb precision afforded by operation at high repetition rates, frepf_{rep} > 10 MHz. Unfortunately, at such high frepf_{rep}, phase matching is prevented by the accumulated steady-state plasma in the generation volume, setting stringent limitations on the XUV average power. Here, we use gas mixtures at high temperatures as the generation medium to increase the translational velocity of the gas, thereby reducing the steady-state plasma in the laser focus. This allows phase-matched XUV emission inside a femtosecond enhancement cavity at a repetition rate of 77 MHz, enabling a record generated power of \sim2 mW in a single harmonic order. This power scaling opens up many demanding applications, including XUV frequency-comb spectroscopy of few-electron atoms and ions for precision tests of fundamental physical laws and constants.


OTIMA interferometry with large organic molecules in the presence of gravity. Massive porphyrin derivatives are evaporated from the target translation stage (T) upon absorption of an intense green source laser (SL) beam, which is chopped by either a slotted rotating disk or an acousto-optic modulator (AOM), depending on the experiment. The molecules leave as 100 μs long packets, with an average velocity around 160 m s⁻¹ (TPP). They pass from the source chamber (SC) through a differential pumping stage into the interferometer chamber (MC) which reaches a base pressure of 2 × 10⁻⁸ mbar. Three fluorine lasers deliver the short-pulse VUV laser light that is retro-reflected at the single common CaF2 mirror (M) to form three standing light wave gratings with a period of d = 78.8 nm. The first grating (G1) acts as a spatially selective particle filter, preparing transverse coherence. The second standing light wave (G2) acts as a transmission and phase grating that diffracts the delocalized molecules. The third laser grating (G3) probes the molecular density pattern, i.e. the quantum interferogram. All grating pulses are less than 10 ns long. G2 follows G1 and G3 follows G2 with a pulse separation time that is freely adjustable between ${T}={\rm{50}}\mbox{--}{\rm{150}}\,\mu {\rm{s}}.$ Molecules that are not removed by any of the three lasers are finally ionized by the fourth F2 laser beam (DL) inside the time-of-flight (TOF) mass spectrometer. The mass-dependent transmission through all laser gratings measures the interference fringe visibility (see text and figure 2). For short pulse separation times (green line) molecules will follow essentially a straight flight path. For larger T (red trajectory), the molecular interferogram will shift noticeably with respect to the post-selecting third grating (G3) due to Earth’s gravitational acceleration g. This shift allows measuring the gravitational acceleration.
Isotope-selective interference contrast of TPP: the normalized signal difference is ${S}_{N}=-\,0.293(3)$ for the isotopically pure TPP (614 amu), ${S}_{N}=\,-\,0.289(3)$ for the next fermion (615 amu) and ${S}_{N}=-\,0.290(3)$ for the 616 amu isotopomer. The normalized signal difference is computed from the area associated with each mass, using a Gaussian multi-peak fit (continuous lines). All ${S}_{N}$ values are identical within the error bar of 1%.
Scanning the molecular fringe pattern in real space. (a) 2D view onto OTIMA with the third grating G3 in two alternative positions: on resonance (δT = 0) and off-resonance (δT > 0). The molecular interference pattern, sketched as green ellipses, moves along G3 with a velocity determined by the tilt angle γ of the molecular beam to the mirror surface and the forward velocity ${{v}}_{{\rm{long}}}.$ (b) The interferogram can be scanned across G3 by varying the pulse separation time, δT, between G2 and G3. Delays of the order of δT < 100 ns are sufficient to shift the pattern by one grating period d = 78.8 nm, while keeping the time within the temporal (Talbot–Lau) resonance condition for the formation of an interference pattern. The envelope of this recurrence period is determined by the divergence angle α of the molecular beam.
Scanning across the interferometer orders. The TOF mass spectra of TPP and the normalized signal difference SN are shown for the 7th, 8th, 9th and 11th Talbot order at pulse separation times around (a) ${\rm{\Delta }}T=65.6\,\mu {\rm{s}},$ (b) ${\rm{\Delta }}T=75.5\,\mu {\rm{s}},$ (c) ${\rm{\Delta }}T=85.4\,\mu {\rm{s}},$ and (d) ${\rm{\Delta }}T=104.0\,\mu {\rm{s}},$ respectively. As before, we see the isotopic resolution and dehydrogenation in the source. Notably, the SN value changes sign. This corresponds to a change in the sign of the phase, respectively a relative shift between the molecular density pattern and the probing standing light wave by more than half a grating period. Equation (4) was fitted to the data and is shown as the solid line. The error bars are extracted using Gaussian propagation of the standard deviations derived from the counting noise [11].
Signal of TPPF84 with a pulse separation time of ΔT = 42.32 μs (left) and TPPF8L12 with ΔT = 94.11 μs (right) in the resonant (red) and off-resonant mode (blue). Even up to a mass of 6509 amu the interference contrast is still as high as for the TPP monomer. The isotopic substructure is no longer resolved at high mass and leads to a broadening of the observed mass spectra. For TPPF8L12 (C165H60F212N4S12) the high carbon content causes an isotopic spread over 8 amu. To visualize the area under the peaks, we fit Gaussians to the data.
Isotope-selective high-order interferometry with large organic molecules in free fall

March 2018

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177 Reads

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18 Citations

Interferometry in the time domain has proven valuable for matter-wave based measurements. This concept has recently been generalized to cold molecular clusters using short-pulse standing light waves which realized photo-depletion gratings, arranged in a time-domain Talbot – Lau interferometer ( OTIMA ) . Here we extend this idea further to large organic molecules and demonstrate a new scheme to scan the emerging molecular interferogram in position space. The capability of analyzing different isotopes of the same monomer under identical conditions opens perspectives for studying the interference fringe shift as a function of time in gravitational free fall. The universality of OTIMA interferometry allows one to handle a large variety of particles. In our present work, quasi-continuous laser evaporation allows transferring fragile organic molecules into the gas phase, covering more than an order of magnitude in mass between 614 amu and 6509 amu, i.e. 300% more massive than in previous OTIMA experiments. For all masses, we fi nd about 30% fringe visibility.


New Avenues for Matter-Wave-Enhanced Spectroscopy

January 2018

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61 Reads

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13 Citations

We present matter-wave interferometry as a tool to advance spectroscopy for a wide class of nanoparticles, clusters and molecules. The high sensitivity of de Broglie interference fringes to external perturbations enables measurements in the limit of an individual particle absorbing only a single photon on average, or even no photon at all. The method allows one to extract structural and electronic information from the loss of the interference contrast. It is minimally invasive and works even for dilute ensembles.


Phase-matched extreme-ultraviolet frequency-comb generation

October 2017

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2 Reads

Laser-driven high-order harmonic generation (HHG) provides tabletop sources of broadband extreme-ultraviolet (XUV) light with excellent spatial and temporal coherence. These sources are typically operated at low repetition rates, frepf_{rep}\lesssim100 kHz, where phase-matched frequency conversion into the XUV is readily achieved. However, there are many applications that demand the improved counting statistics or frequency-comb precision afforded by operation at high repetition rates, frepf_{rep} > 10 MHz. Unfortunately, at such high frepf_{rep}, phase matching is prevented by the accumulated steady-state plasma in the generation volume, setting stringent limitations on the XUV average power. Here, we use gas mixtures at high temperatures as the generation medium to increase the translational velocity of the gas, thereby reducing the steady-state plasma in the laser focus. This allows phase-matched XUV emission inside a femtosecond enhancement cavity at a repetition rate of 77 MHz, enabling a record generated power of \sim2 mW in a single harmonic order. This power scaling opens up many demanding applications, including XUV frequency-comb spectroscopy of few-electron atoms and ions for precision tests of fundamental physical laws and constants.


a UV–VIS spectroscopy in OTIMA: absorption of a single photon from a running laser wave imparts a recoil to the absorbing cluster or molecule. If the wavelength of the light is comparable to the semiclassical path separation of the delocalized particle, the interference fringe pattern experiences a measurable dephasing (Sect. 3) [19, 20]. Because of the small grating period (79 nm), single-color visible or infrared (VIS/IR) spectroscopy requires the collective momentum transfer of several photons or operation of the matter-wave interferometer in higher Talbot orders. b VIS/IR spectroscopy: can also be realized by combining a single (VIS/IR) photon of laser beam L1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${L}_1$$\end{document} (red arrow) with a single UV photon from beam L2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${L}_2$$\end{document} (green arrow) which provides the required momentum transfer (Sects. 6 and 7). c Polarizability spectroscopy: is the least invasive of all three techniques. The off-resonant dipole interaction with the intense laser field G4\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${G}_4$$\end{document} deforms the matter-wave front—leading to a loss of fringe contrast even without any photo-absorption. This method may be particularly useful for weakly bound van der Waals clusters (Sect. 8)
a The absorption of multiple photons from a monochromatic source is suppressed due to the anharmonicity bottleneck. b Internal vibrational relaxation (IVR) to other modes dissipates the energy and enables the repeated excitation of the same IR transition until sufficient momentum recoil has been accumulated to shift the fringe pattern measurably
a In IR–UV-recoil dip spectroscopy the matter-wave dephasing action of a UV photon is suppressed by emptying the ground state in a resonant IR transition. b In double resonant IR–UV-recoil spectroscopy the kick of the UV photon is conditioned on the prior absorption of the IR or VIS photon
New avenues for matter-wave-enhanced spectroscopy

December 2016

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152 Reads

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35 Citations

Applied Physics B

We present matter-wave interferometry as a tool to advance spectroscopy for a wide class of nanoparticles, clusters and molecules. The high sensitivity of de Broglie interference fringes to external perturbations enables measurements in the limit of an individual particle absorbing only a single photon on average, or even no photon at all. The method allows one to extract structural and electronic information from the loss of the interference contrast. It is minimally invasive and works even for dilute ensembles.


Prospects for quantum interference-assisted molecule metrology. (A) The Kapitza–Dirac–Talbot–Lau interferometer [43] consists of three gratings with a fixed mutual distance L. It has been successfully applied to numerous organic molecules, also in quantum-assisted metrology [68, 79]. (B) OTIMA interferometry [44] uses three retro-reflected nanosecond pulsed photo-depletion gratings to realize three absorptive masks that remove molecules from the antinodes of the grating. The pulsed nature of the grating structure allows suppressing various dispersive phase shifts and opens a window to time-resolved metrology. In both cases, metrology relies on the fact that matter-wave physics leads to the formation of molecular density patterns on the nanoscale. Interaction of the delocalized molecules with electric, magnetic and optical fields or collisions with directed atoms and molecules will shift these fringes. This is depicted in (A) by a deflector electrode and by a running light wave in (B). The high sensitivity of these instruments derives from the fact that even minuscule perturbations—as for instance imparted by single photons interacting with single molecules—shift the matter-wave fringes by an amount that is readily resolved.
Proposed beam splitter based on the dissociation of biomolecular water clusters. Clusters which pass by the antinodes of the standing light wave can be electronically excited by a single UV photon (1) while those which move through a node remain in their electronic ground state (2). An intense running wave IR laser beam can selectively induce the dissociation of excited state molecules when it is sufficiently far-detuned with respect to the vibrational frequencies of the electronic ground state.
Molecular beam sources. (A) Small biomolecules can be evaporated thermally and co-expanded in a supersonic noble gas jet. This leads to well-directed beams with high forward velocities and temperatures low enough for efficient clustering of biomolecules and water adsorbates. (B) For less volatile particles, such as polypeptides or proteins the interaction with the heating source needs to be kept short. Nanosecond laser desorption into the supersonic jet proves powerful in getting such species isolated and as small clusters into a directed molecular beam: The transfer from the sample supply slide (1) to the desorption wheel (2) is made via a soft felt wheel. The glassy carbon wheel (2) turns at about 1 Hz to expose a fresh sample spot for every laser shot. The desorbed molecules are injected into a noble gas beam emerging from a cold pulsed valve (3). The molecules are cooled in the gas expansion and form clusters with water inside a 40 mm long collision channel (4).
(a) Hydrated clusters of vanillin, generated in free supersonic noble gas expansion. Here the intensity of the pure n = 2 cluster drawn in red is artificially reduced by a factor of 0.5. The inset shows up to the m = 5 water cluster. (b) Pure tryptophan clusters (Trpn,, n = 1–30) and (c) their respective water clusters (Trpn(H2O)m) can be prepared by thin-film laser desorption into a noble gas jet. The inset in (c) illustrates this for the n = 3, m = 0–4 cluster. The same method is capable of producing beams of polypeptide monomers and their water clusters as shown for (d) indolicidin [136] and (e) multiply hydrated gramicidin D [137]. The asterisks in (c) and (d) denote spurious sample fragments and impurities.
Perspectives for quantum interference with biomolecules and biomolecular clusters

June 2016

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236 Reads

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20 Citations

Modern quantum optics encompasses a wide field of phenomena that are either related to the discrete quantum nature of light, the quantum wave nature of matter or light–matter interactions. We here discuss new perspectives for quantum optics with biological nanoparticles. We focus in particular on the prospects of matter-wave interferometry with amino acids, nucleotides, polypeptides or DNA strands. We motivate the challenge of preparing these objects in a 'biomimetic' environment and argue that hydrated molecular beam sources are promising tools for quantum-assisted metrology. The method exploits the high sensitivity of matter-wave interference fringes to dephasing and shifts in the presence of external perturbations to access and determine molecular properties.


Matter-wave interferometry with composite quantum objects

January 2015

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267 Reads

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15 Citations

We discuss modern developments in quantum optics with organic molecules, clusters and nanoparticles -- in particular recent realizations of near-field matter-wave interferometry. A unified theoretical description in phase space allows us to describe quantum interferometry in position space and in the time domain on an equal footing. In order to establish matter-wave interferometers as a universal tool, which can accept and address a variety of nanoparticles, we elaborate on new quantum optical elements, such as diffraction gratings made of matter and light, as well as their absorptive and dispersive interaction with complex materials. We present Talbot-Lau interferometry (TLI), the Kapitza-Dirac-Talbot-Lau interferometer (KDTLI) and interferometry with pulsed optical gratings (OTIMA) as the most advanced devices to study the quantum wave nature of composite matter. These experiments define the current mass and complexity record in interferometric explorations of quantum macroscopicity and they open new avenues to quantum assisted metrology with applications in physical chemistry and biomolecular physics.


Setup for cluster interferometry using three pulsed, absorptive standing lightwave gratings. (a) Mirror deformations shift the nodes of the standing waves within the laser spot. This reduces the fringe visibility due to averaging over the phase-shifted interference patterns. This is indicated by the solid and dashed semiclassical paths for two particles that start with the same velocity and direction but at different positions. A mirror reflectivity R < 0.96 and limited laser coherence are the reasons why a running wave overlays the periodic gratings. The figure is drawn not to scale to illustrate the effects of minuscule mirror deformations. (b) Mass spectrum of ferrocene clusters that are detected after the third grating pulse using VUV photoionization in a time-of-flight mass spectrometer. We compare the interference signal S Int (blue dashed line) with a reference signal S Ref (red solid line), as shown in the inset for the model system Fc 7 . (c) The normalized signal contrast S N (see text) is shown for the clusters Fc 3 to Fc 9 .
Theoretical visibility V for different values of the optical polarizability. (a) Contrast as a function of the pulse separation time T , in multiples of the Talbot time T T . It is plotted for varying phase shifts (polarizabilities) in the antinodes of the second standing wave ( Φ 0 ( 2 ) = 7.5 , dotted; Φ 0 ( 2 ) = 3 , dashed; Φ 0 ( 2 ) = 1.5 , solid). (b) Contrast as a function of Φ 0 ( 2 ) , i.e., for varying optical polarizability α λ , plotted for three different pulse separation times ( T = 0.75 T T , dashed; T = 0.9 T T , dotted, T = T T , solid). For T = T T , the particle polarizability does not affect the interference contrast at all, while at 0.75 T T the contrast oscillates with Φ 0 ( 2 ) . The arrows and colors link plot (a) with plot (b). For both panels, the transmission through all three gratings was fixed by setting n 0 ( i ) = 6.
Measured interference contrast as a function of the mean number n 0 ( 2 ) of standing wave photons absorbed in the antinode of the second grating. (a) Interference measurements for three different laser energies reveal the shift of the maximal interference contrast toward higher masses for lower laser pulse energy. The triangles link the plots (a) and (b). (b) Normalized contrast for anthracene clusters of size N = 6 –9: Ac 6 (gray, dashed–dotted), Ac 7 (red, dotted), Ac 8 (light red, solid), Ac 9 (brown, dashed). The lines are fits based on the model discussed in the text. Error bars represent one standard deviation of statistical error.
Quantum interference of ferrocene clusters from N = 6 – 9 . It is shown as a function of number of absorbed photons in G 2 , which is also a measure for the open fraction of the grating. Fc 6 (gray, dashed–dotted fit), Fc 7 (dark blue, dotted fit), Fc 8 (light blue, solid fit), Fc 9 (blue, dashed fit). Error bars represent one standard deviation of statistical error.
Refined model for Talbot–Lau matter-wave optics with pulsed photodepletion gratings

December 2014

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42 Reads

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7 Citations

We analyze time-domain Talbot–Lau interferometry of organic cluster beams that are exposed to pulsed photodepletion gratings in the vacuum ultraviolet. We focus particularly on the analysis of the complex (phase and absorption) character of the optical elements. The discussion includes the role of wavefront distortions due to mirror imperfections on the nanometer level and the effect of finite coherence in the diffraction gratings. This improved understanding of the interferometer allows us to extract new information on optical properties of anthracene and ferrocene clusters and to define conditions for future matter-wave experiments.


Photofragmentation Beam Splitters for Matter-Wave Interferometry

July 2014

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42 Reads

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34 Citations

Physical Review Letters

Extending the range of quantum interferometry to a wider class of composite nanoparticles requires new tools to diffract matter-waves. Recently, pulsed photoionization light gratings have demonstrated their suitability for high mass matter-wave physics. Here we extend quantum interference experiments to a new class of particles by introducing photofragmentation beam splitters into time-domain matter-wave interferometry. Photofragmentation gratings can act on objects as different as van der Waals clusters and biomolecules which are thermally unstable and often resilient to single-photon ionization. We present data that demonstrate this coherent beam splitting mechanism with clusters of hexafluorobenzene and we show single-photon depletion gratings based both on fragmentation and ionization for clusters of vanillin.


Citations (10)


... Notably, the use of a central wavelength of 1030 nm has proven beneficial for high average power EUV light sources [27]. Combined with various pulse compression techniques and double and triple frequency techniques, HHG conversion efficiency can be further improved [28][29][30]8]. It has been reported that a single 26.5 eV harmonic average power of 12.9 mW is obtained by combining a high-average power laser with additional compression using chirped mirrors [8]. Clearly, the combination of high average power and ultrashort pulse duration significantly improves EUV average power, further advancing the application of HHG in desktop setting [31]. ...

Reference:

Tabletop ptychographic imaging system with a 515 nm laser driven high-order harmonic source
Phase-Matched Extreme-Ultraviolet Frequency-Comb Generation

... Furthermore, certain tests of gravity would profit from the possibility to compare in the same setup the free fall of atoms, clusters and nanoparticles, with different mass, different materials, different internal energy, and many different types of angular momentum. 5 ...

Isotope-selective high-order interferometry with large organic molecules in free fall

... A beam of light moving towards a Black Hole or away from a Black Hole will keep the same speed of light. But the intensity of the beam of Light will increase when the beam of light moves towards a Black Hole and the intensity will decrease when a beam of light moves away from a Black 28 Hole. This type of confinement has been called a "Longitudinal Black Hole" in which the confined light always propagates in the direction of the gravitational field of the Black Hole. ...

New Avenues for Matter-Wave-Enhanced Spectroscopy

... [102][103][104][105][106] Speeding up the gas flow to refresh the gas medium faster and reduce accumulated plasma, the JILA team reported generated HHG powers of >1 mW/harmonic for the 11th harmonic of 1070 nm in Xe (12.8 eV), but only transiently. 107 The JILA team has also explored non-collinear HHG for generating and outcoupling low-order harmonics. 108 Now, nearly 20 years since the first demonstration, CE-HHG is a mature technology with well-understood trade-offs impacting system design, which we discuss in the following in regard to the parameters listed in Sec. ...

Phase-matched extreme-ultraviolet frequency-comb generation

Nature Photonics

... The de Broglie wave nature has also been shown for large molecules, from fullerenes 11 and molecular clusters 12 up to tailor-made macromolecules 13 . Such experiments probe the quantum-to-classical interface and can be used to characterize neutral molecules in the gas phase, through interference fringe deflection in electric and magnetic fields 14 or minimally invasive spectroscopy 15,16 . ...

New avenues for matter-wave-enhanced spectroscopy

Applied Physics B

... Interestingly enough, matterwave interferometry can also find novel applications in quantum-assisted measurements on large biomolecules and biomolecular clusters [94]. Typical techniques seek to exploit the high sensitivity of matter-wave spatial interference fringes to circumvent the issues of dephasing and decoherence in such sensitive experiments (in the presence of external perturbative effects) [95] to measure and investigate the molecular properties of a large class of biomolecules. ...

Perspectives for quantum interference with biomolecules and biomolecular clusters

... The observation of coherent, wave-like properties in vapors of neutral atoms is relatively recent, brought about by advances in the cooling and trapping of atoms [36,37,38,39]. Atomic matter-waves can be collimated into beams [40] and focused [21], reflected [41,42], and coherently interfered [43], in direct analogy with optical waves. The ability to perform these basic atom-optical manipulations with high precision is crucial for more sophisticated atomic physics experiments and devices, such as atom lasers [6], quantum emulators [44,45] and atom interferometers [46]. ...

Matter-wave interferometry with composite quantum objects

... Modeling. We model the expected signal by evolving the transverse Wigner function w(x, p x ) 27 , taking into account tilted and divergent molecular beams, as well as mirror and grating imperfections 28 . As a phase space description, it allows comparing the experiment with both the quantum and the classical expectation within the same framework (see Methods). ...

Refined model for Talbot–Lau matter-wave optics with pulsed photodepletion gratings

... Beam splitters are crucial optical components in modern optical systems and are widely employed in applications such as optical communication [1], holography [2], and interferometry [3][4][5]. Beam splitters are primarily realized through three methods: refraction [6,7], diffraction [8][9][10], and metasurfaces [11][12][13][14]. While traditional beam splitters can be achieved by utilizing birefringence in photonic crystals or multifilm structures. ...

Photofragmentation Beam Splitters for Matter-Wave Interferometry
  • Citing Article
  • July 2014

Physical Review Letters

... The concept of employing standing light waves as an optical grating for electrons was initially suggested by Kapitza and Dirac 46 and was later experimentally demonstrated for the scattering 47 and diffraction 48 of low-energy electrons. Optical gratings are also employed in matter-wave interferometry for molecules and clusters 49 . ...

A universal matter-wave interferometer with optical ionization gratings in the time domain

Nature Physics