Control of the nonlinear response of bulk GaAs induced by long-wavelength infrared pulses.

The nonlinear optical response of GaAs is studied using extremely nonresonant 10 µm laser pulses with peak intensities greater than 2 GW/cm 2. We observe over an order of magnitude enhancement in the four-wave mixing efficiency by decreasing the CO 2 laser beat-wave frequency. This enhancement is attributed to currents of photoexcited unbound carriers modulated at the beat frequency, confirmed by measurements of nonlinear absorption at this long wavelength as well as a fully microscopic analysis of the excitation dynamics. Modeling of such nonperturbative semiconductor-laser interactions predicts that further decreasing the beat frequency can increase the nonlinear response and allow for its control over two orders of magnitude.

Interlayer excitons in transition-metal dichalcogenide heterostructures with type-II band alignment.

Combining ab initio density functional theory with the Dirac-Bloch and gap equations, excitonic properties of transition-metal dichalcogenide hetero-bilayers with type-II band alignment are computed. The existence of interlayer excitons is predicted, whose binding energies are as large as 350 meV, only roughly 100 meV less than those of the coexisting intralayer excitons. The oscillator strength of the interlayer excitons reaches a few percent of the intralayer exciton resonances and their radiative lifetime is two orders of magnitude larger than that of the intralayer excitons.

Lightwave valleytronics in a monolayer of tungsten diselenide.

As conventional electronics approaches its limits 1 , nanoscience has urgently sought methods of fast control of electrons at the fundamental quantum level 2 . Lightwave electronics 3 -the foundation of attosecond science 4 -uses the oscillating carrier wave of intense light pulses to control the translational motion of the electron's charge faster than a single cycle of light5-15. Despite being particularly promising information carriers, the internal quantum attributes of spin 16 and valley pseudospin17-21 have not been switchable on the subcycle scale. Here we demonstrate lightwave-driven changes of the valley pseudospin and introduce distinct signatures in the optical readout. Photogenerated electron-hole pairs in a monolayer of tungsten diselenide are accelerated and collided by a strong lightwave. The emergence of high-odd-order sidebands and anomalous changes in their polarization direction directly attest to the ultrafast pseudospin dynamics. Quantitative computations combining density functional theory with a non-perturbative quantum many-body approach assign the polarization of the sidebands to a lightwave-induced change of the valley pseudospin and confirm that the process is coherent and adiabatic. Our work opens the door to systematic valleytronic logic at optical clock rates.

Symmetry-controlled time structure of high-harmonic carrier fields from a solid.

High-harmonic (HH) generation in crystalline solids1-6 marks an exciting development, with potential applications in high-efficiency attosecond sources7, all-optical bandstructure reconstruction8,9, and quasiparticle collisions10,11. Although the spectral1-4 and temporal shape5 of the HH intensity has been described microscopically1-6,12, the properties of the underlying HH carrier wave have remained elusive. Here we analyse the train of HH waveforms generated in a crystalline solid by consecutive half cycles of the same driving pulse. Extending the concept of frequency combs13-15 to optical clock rates, we show how the polarization and carrier-envelope phase (CEP) of HH pulses can be controlled by crystal symmetry. For some crystal directions, we can separate two orthogonally polarized HH combs mutually offset by the driving frequency to form a comb of even and odd harmonic orders. The corresponding CEP of successive pulses is constant or offset by π, depending on the polarization. In the context of a quantum description of solids, we identify novel capabilities for polarization- and phase-shaping of HH waveforms that cannot be accessed with gaseous sources.

Lightwave-driven quasiparticle collisions on a subcycle timescale.

Ever since Ernest Rutherford scattered α-particles from gold foils, collision experiments have revealed insights into atoms, nuclei and elementary particles. In solids, many-body correlations lead to characteristic resonances--called quasiparticles--such as excitons, dropletons, polarons and Cooper pairs. The structure and dynamics of quasiparticles are important because they define macroscopic phenomena such as Mott insulating states, spontaneous spin- and charge-order, and high-temperature superconductivity. However, the extremely short lifetimes of these entities make practical implementations of a suitable collider challenging. Here we exploit lightwave-driven charge transport, the foundation of attosecond science, to explore ultrafast quasiparticle collisions directly in the time domain: a femtosecond optical pulse creates excitonic electron-hole pairs in the layered dichalcogenide tungsten diselenide while a strong terahertz field accelerates and collides the electrons with the holes. The underlying dynamics of the wave packets, including collision, pair annihilation, quantum interference and dephasing, are detected as light emission in high-order spectral sidebands of the optical excitation. A full quantum theory explains our observations microscopically. This approach enables collision experiments with various complex quasiparticles and suggests a promising new way of generating sub-femtosecond pulses.

Real-time observation of interfering crystal electrons in high-harmonic generation.

Acceleration and collision of particles has been a key strategy for exploring the texture of matter. Strong light waves can control and recollide electronic wavepackets, generating high-harmonic radiation that encodes the structure and dynamics of atoms and molecules and lays the foundations of attosecond science. The recent discovery of high-harmonic generation in bulk solids combines the idea of ultrafast acceleration with complex condensed matter systems, and provides hope for compact solid-state attosecond sources and electronics at optical frequencies. Yet the underlying quantum motion has not so far been observable in real time. Here we study high-harmonic generation in a bulk solid directly in the time domain, and reveal a new kind of strong-field excitation in the crystal. Unlike established atomic sources, our solid emits high-harmonic radiation as a sequence of subcycle bursts that coincide temporally with the field crests of one polarity of the driving terahertz waveform. We show that these features are characteristic of a non-perturbative quantum interference process that involves electrons from multiple valence bands. These results identify key mechanisms for future solid-state attosecond sources and next-generation light-wave electronics. The new quantum interference process justifies the hope for all-optical band-structure reconstruction and lays the foundation for possible quantum logic operations at optical clock rates.

Quantum-memory effects in the emission of quantum-dot microcavities.

The experimentally measured input-output characteristics of optically pumped semiconductor microcavities exhibits unexpected oscillations modifying the fundamentally linear slope in the excitation power regime below lasing. A systematic microscopic analysis reproduces these oscillations, identifying them as a genuine quantum-memory effect, i.e., a photon-density correlation accumulated during the excitation. With the use of projected quantum measurements, it is shown that the input-output oscillations can be controlled and enhanced by an order of magnitude when the quantum fluctuations of the pump are adjusted.

Anti-insulin antibodies and birth weight in pregnancies complicated by diabetes.

Free insulin cannot cross the placenta but insulin complexed to anti-insulin antibodies has been demonstrated in cord blood. We studied whether antibody-bound insulin in diabetic patients can evoke fetal macrosomia independently of maternal metabolic control. In 457 non insulin-treated controls and 173 insulin-treated diabetic patients we measured 1187 anti-insulin antibody levels and maternal blood glucose, maternal fructosamine, cord blood insulin, cord blood C-peptide, cord blood fructosamine and amniotic fluid insulin. Mean anti-insulin antibody levels in maternal blood and cord blood were significantly higher in insulin treated diabetic patients (4.6 and 5.4 U/ml) than in controls (1.8 and 1.7 U/ml) with maxima of 89.2 in maternal and 120.0 U/ml in cord blood, respectively. In insulin treated diabetic patients 16.6% (maternal blood) and 22% (cord blood) anti-insulin antibody levels were above the 97th percentile. There was a high significant correlation between maternal and cord blood anti-insulin antibodies (R = 0.987, P = < 0.0001), but no correlation of anti-insulin antibodies with maternal (glucose, fructosamine) or fetal (insulin, C-peptide, and fructosamine in cord blood, amniotic fluid insulin) metabolic parameters. While maternal and fetal metabolic parameters correlated with birth weight neither maternal nor cord blood anti-insulin antibody levels correlated with birth weight. These findings do not support the hypothesis that maternal anti-insulin antibodies independently influence fetal weight.

Levels of amniotic fluid insulin and profiles of maternal blood glucose in pregnant women with diabetes type-I.

The aim of this study was to investigate the relationship between amniotic fluid insulin (AF-insulin) measurements and maternal blood glucose levels in pregnancies complicated by insulin-dependent maternal diabetes mellitus (IDDM). Twenty-five patients with IDDM underwent amniocentesis (AC) in the third trimester. Twelve patients had a second amniocentesis after 2-3 weeks. The maternal blood glucose values (MBG) 2 weeks before amniocentesis were correlated with AF-insulin. Mean (+/-S.D.) MBG in the group with AF-insulin > 97th centile (n = 7) was 6.1 +/- 1 mmol/l. MBG in the group with AF-insulin < 97th centile (n = 18) was 5.3 +/- 1.2 mmol/l (r = 0.2948; P-value 0.162). In the group with repeated AC and AF-insulin > 97th centile (n = 6) the correlation coefficient was 0.722 (P = 0.043), whereas in the group with normal AF-insulin (n = 6) no correlation was found (r = -0.213; P = 0.686). These results indicate that no significant correlation exists between MBG values and concentration of AF-insulin. MBG is not appropriate for the diagnosis of fetal hyperinsulinism in well-controlled women with IDDM. In individual cases with AF-insulin > 97th centile a decrease of MBG causes lower AF-insulin levels. These results indicate that there seems to be an individual threshold for maternal MBG which causes hyperinsulinism. Fetal hyperinsulinism not only depends on blood glucose levels. Different fetal sensitivity to maternal glucose stimuli or a different glucose transport across the placenta in the individual fetus could be responsible for these results.

Ultrasound growth parameters in relation to levels of amniotic fluid insulin in women with diabetes type-I.

The aim of the study was to investigate the correlation between ultrasound parameters and levels of amniotic fluid insulin (AF-insulin) in pregnancies complicated by insulin-dependent diabetes mellitus (IDDM). In 129 women with IDDM amniocentesis was performed between 28 and 35 weeks of gestation. The levels of AF-insulin were measured by radioimmunoassay (Pharmacia RIA 100) and were correlated with biparietal diameter (BPD), abdominal diameter (AD), abdominal circumference (AC), and femur length (FL). The women were maintained at good glycemic control (fructosamine level: mean +/- S.D.: 236.3 +/- 40 micromol/l) and delivered infants with a mean (+/- S.D.) birth weight of 3477 +/- 640 g. The sensitivity of BPD, AD, AC and FL to detect fetuses with pathological levels of AF-insulin was 50%, 62%, 67% and 49%, respectively. The sensitivities of AD and AC in a selected group (n = 14) with highly pathological levels of AF-insulin (> 20 microU/ml) were both 80%, whereas the specificity was 56% and 46%, respectively. In women with IDDM, fetal biparietal diameter, abdominal diameter, abdominal circumference, and femur length are not reliable markers for the identification of fetal hyperinsulinism. Only cases with highly pathological levels of AF-insulin can be detected by abdominal measurements.

[Fetal ultrasound biometry and amniotic fluid insulin concentration in pregnant diabetic patients]. / Fetale Ultraschallbiometrie und Fruchtwasserinsulinkonzentration bei diabetischen Schwangeren.

OBJECTIVE: The aim of the study was to prove the sensitivity of sonographic measurements for the presence of a fetal hyperinsulinism. METHODS: In a longitudinal examination of 102 insulin-dependent diabetics we show the correlation between the amniotic fluid insulin level and the biparietal diameter, abdominal diameter and femur length in the third trimester. The control of the maternal metabolic state was done by measuring the glycosylated hemoglobin and fructosamine at the time of the amniocentesis. RESULTS: The sensitivity, specificity, positive and negative predictive value of sonographic measurements > 75th percentile in fetal hyperinsulinism was for the biparietal diameter 21, 96, 81 and 62%, for the abdominal diameter 48, 82, 69 und 66%, and for the femur length 22, 90, 67 and 57%. The maternal glycoproteins did not show any correlation with the amniotic fluid insulin level. CONCLUSIONS: The results demonstrate that fetal hyperinsulinism cannot be proved by fetal biometry or evaluation of the maternal metabolic state.