Femtosecond Photodissociation of Molecules Facilitated by Noise

We investigate the dynamics of diatomic molecules subjected to both a femtosecond mid-infrared laser pulse and Gaussian white noise. The stochastic Schr\"odinger equation with a Morse potential is used to describe the molecular vibrations under noise and the laser pulse. For weak laser intensity, well below the dissociation threshold, it is shown that one can find an optimum amount of noise that leads to a dramatic enhancement of the dissociation probability. The enhancement landscape which is shown as a function of both the noise and the laser strength, exhibits a global maximum. A frequency-resolved gain profile is recorded with a pump-probe set-up which is experimentally realizable. With this profile we identify the linear and nonlinear multiphoton processes created by the interplay between laser and noise and assess their relative contribution to the dissociation enhancement.Comment: 5 pages,5 figure

Self-Assembled Monolayers prepared from alkanethiols or dialkyl disulfides on Au: evidence of influence of the anchoring group

Mainly based on electrochemical investigations, this work provides evidence of discrimination between self-assembled monolayers (SAMs) prepared from alkanethiols or symmetrical dialkyl disulfides on gold. Gravimetric experiments carried out by quartz crystal microbalance during the elaboration of ferrocene based SAMs (from alkanethiols FcC15SH and dialkyl disulfides FcC15SSC15Fc), showed significant differences between monolayers made from the two precursors. The recorded mass was almost 60 % more important with FcC15SH by comparison with FcC15SSC15Fc. The resulting cyclic voltammograms also highlighted a 60 % difference concerning the surface coverage of ferrocene heads. Moreover, dialkyl disulfide and thiol anchoring groups led to symmetrical and dissymmetrical peaks, respectively, suggesting not insignificant differences concerning interactions between adsorbed species into the two kinds of elaborated monolayers. These observations were confirmed on SAMs obtained from other precursors possessing shorter chain length or another functional moiety

Non-classical properties of quantum wave packets propagating in a Kerr-like medium

We investigate non-classical effects such as fractional revivals, squeezing and higher-order squeezing of photon-added coherent states propagating through a Kerr-like medium.The Wigner functions corresponding to these states at the instants of fractional revivals are obtained, and the extent of non-classicality quantified.Comment: 8 pages, 10 figure

Mean parity of single quantum excitation of some optical fields in thermal environments

The mean parity (the Wigner function at the origin) of excited binomial states, excited coherent states and excited thermal states in thermal channel is investigated in details. It is found that the single-photon excited binomial state and the single-photon excited coherent state exhibit certain similarity in the aspect of their mean parity in the thermal channel. We show the negative mean parity can be regarded as an indicator of nonclassicality of single-photon excitation of optical fields with a little coherence, especially for the single-photon excited thermal states.Comment: 4 pages, 4 figures, RevTex4; PACS numbers: 42.50.Dv, 03.65.Yz, 05.40.Ca; Three typo errors have been correcte

Non-Hermitian trimers: PT-symmetry versus pseudo-Hermiticity

We study a structure composed of three coupled waveguides with gain and loss, a non-Hermitian trimer. We demonstrate that the mode spectrum can be entirely real if the waveguides are placed in a special order and at certain distances between each other. Such structures generally lack a spatial symmetry, in contrast to parity-time symmetric trimers which are known to feature a real spectrum. We also determine a threshold for wave amplification and analyse the scattering properties of such non-conservative systems embedded into a chain of conservative waveguides.SVS and AAS were supported by the Australian Research Council (ARC), Discovery Project DP160100619. SVS acknowledges financial support from the Russian Foundation for Basic Research, grant No.15-31-20037 mol_a

Simultaneous determination of the kinetics of cardiac output, systemic O2 delivery and lung O2 uptake at exercise onset in men.

We tested whether the kinetics of systemic O2 delivery (Q'aO2) at exercise start was faster than that of lung O2 uptake (V' O2), being dictated by that of cardiac output (Q'), and whether changes in Q' would explain the postulated rapid phase of the V'O2 increase. Simultaneous determinations of beat-by-beat (BBB) Q' and Q' aO2, and breath-by-breath V'O2 at the onset of constant load exercises at 50 and 100 W were obtained on six men (age 24.2 +/-3.2 years, maximal aerobic power 333 +/- 61 W). V'O2 was determined using Grønlund’s algorithm. Q' was computed from BBB stroke volume (Qst, from arterial pulse pressure profiles) and heart rate (fH, electrocardiograpy) and calibrated against a steadystate method. This, along with the time course of hemoglobin concentration and arterial O2 saturation (infrared oximetry) allowed computation of BBB Q'aO2. The Q', Q'aO2 and V'O2 kinetics were analyzed with single and double exponential models. fH, Qst, Q', and V'O2 increased upon exercise onset to reach a new steady state. The kinetics of Q'aO2 had the same time constants as that of Q'. The latter was twofold faster than that of V'O2. The V'O2 kinetics were faster than previously reported for muscle phosphocreatine decrease. Within a two-phase model, because of the Fick equation, the amplitude of phase I Q' changes fully explained the phase I of V'O2 increase. We suggest that in unsteady states, lung V' O2 is dissociated from muscle O2 consumption. The two components of Q' and Q'aO2 kinetics may reflect vagal withdrawal and sympathetic activation

Cardiac output by model flow method from intra-arterial and finger tip pulse pressure profiles

Modelflow®, when applied to non-invasive fingertip pulse pressure recordings, is a poor predictor of cardiac output (Q’ litre· min-1). The use of constants established from the aortic elastic characteristics, which differ from those of finger arteries, may introduce signal distortions, leading to errors in computing Q’. We therefore hypothesized that peripheral recording of pulse pressure profiles undermines the measurement of Q’ withModelflow®, so we compared Modelflow® beat-by-beat Q’ values obtained simultaneously non-invasively from the finger and invasively from the radial artery at rest and during exercise. Seven subjects (age, 24.0 + - 2.9 years; weight, 81.2 + - 12.6 kg) rested, then exercised at 50 and 100 W, carrying a catheter with a pressure head in the left radial artery and the photoplethysmographic cuff of a finger pressure device on the third and fourth fingers of the contralateral hand. Pulse pressure from both devices was recorded simultaneously and stored on a PC for subsequent Q’ computation. The mean values of systolic, diastolic and mean arterial pressure at rest and exercise steady state were significantly (P < 0.05) lower from the finger than the intra-arterial catheter. The corresponding mean steady-state Q’ obtained from the finger (Q’porta) was significantly (P < 0.05) higher than that computed from the intra-arterial recordings (Q’pia). The line relating beat-by-beat Q’porta and Q’pia was y = 1.55x - 3.02 (r2 = 0.640). The bias was 1.44 litre · min-1 and the precision was 2.84 litre · min-1.The slope of this line was significantly higher than 1, implying a systematic overestimate of Q’ by Q’porta with respect to Q’pia. Consistent with the tested hypothesis, these results demonstrate that pulse pressure profiles from the finger provide inaccurate absolute Q’ values with respect to the radial artery, and therefore cannot be used without correction with a calibration factor calculated previously by measuring Q’ with an independent method

Phase I dynamics of cardiac output, systemic O2 delivery and lung O2 uptake at exercise onset in men in acute normobaric hypoxia.

We tested the hypothesis that vagal withdrawal plays a role in the rapid (phase I) cardiopulmonary response to exercise. To this aim, in five men (24.6+/-3.4 yr, 82.1+/-13.7 kg, maximal aerobic power 330+/-67 W), we determined beat-by-beat cardiac output (Q), oxygen delivery (QaO2), and breath-by-breath lung oxygen uptake (VO2) at light exercise (50 and 100 W) in normoxia and acute hypoxia (fraction of inspired O2=0.11), because the latter reduces resting vagal activity. We computed Q from stroke volume (Qst, by model flow) and heart rate (fH, electrocardiography), and QaO2 from Q and arterial O2 concentration. Double exponentials were fitted to the data. In hypoxia compared with normoxia, steady-state fH and Q were higher, and Qst and VO2 were unchanged. QaO2 was unchanged at rest and lower at exercise. During transients, amplitude of phase I (A1) for VO2 was unchanged. For fH, Q and QaO2, A1 was lower. Phase I time constant (tau1) for QaO2 and VO2 was unchanged. The same was the case for Q at 100 W and for fH at 50 W. Qst kinetics were unaffected. In conclusion, the results do not fully support the hypothesis that vagal withdrawal determines phase I, because it was not completely suppressed. Although we can attribute the decrease in A1 of fH to a diminished degree of vagal withdrawal in hypoxia, this is not so for Qst. Thus the dual origin of the phase I of Q and QaO2, neural (vagal) and mechanical (venous return increase by muscle pump action), would rather be confirmed

Initial-state dependence of coupled electronic and nuclear fluxes in molecules

We demonstrate that coupled electronic and nuclear fluxes in molecules can strongly depend on the initial state preparation. Starting the dynamics of an aligned D2 + molecule at two different initial conditions, the inner and the outer turning points, we observe qualitatively different oscillation patterns of the nuclear fluxes developing after 30 fs. This corresponds to different orders of magnitude bridged by the time evolution of the nuclear dispersion. Moreover, there are attosecond time intervals within which the electronic fluxes do not adapt to the nuclei motion depending on the initial state. These results are inferred from two different approaches for the numerical flux simulation, which are both in good agreement