Dark Pulses Research Articles

Effects of light intensity and restraint on dark-pulse-induced circadian phase shifting during subjective night in Syrian hamsters.

Dark pulses presented on a background of constant light (LL) result in phase advances during midsubjective day and early subjective night, and phase delays during late subjective night, as shown in the dark-pulse phase response curve. In hamsters, the phase-shifting effects of dark pulses are thought to be mediated by increased activity, as previous studies have shown that restraining animals during dark pulses blocks the phase shifts observed in midsubjective day and late subjective night. This study focuses on dark-pulse-induced phase shifting during early subjective night, examining the influence of both LL intensity and restraint on the magnitude of these phase shifts. Syrian hamsters were maintained in LL of four different illumination levels (1, 10, 100, or 600 lux) and periodically presented with 6-h pulses (dark pulse alone, restraint alone, or dark pulse plus restraint) beginning at circadian time 11. Phase advances were observed in response to dark pulses alone, and the magnitude of these shifts was dependent on background illumination, with significantly larger advances seen under higher intensities. No relationship was found between the amount of activity displayed during dark pulses and phase shift magnitude. Six-hour periods of restraint resulted in phase delays, the magnitude of which was also dependent on background illumination. Restraining hamsters during dark pulses reduced the magnitude of phase advances, but the extent of this reduction could be predicted from the additive effects of the dark-pulse-alone and restraint-alone conditions. These results indicate that the phase-shifting effects of dark pulses during early subjective night are not mediated by behavioral activation and may instead reflect a mirror image of the phase-delaying effects of light pulses at this phase.

Is the PRC for Dark Pulses in LL a Mirror Image of the PRC for Light Pulses in DD in Mice?

The phase-response curves (PRC) for light pulses in continuous darkness (DD) have been described in many mammals, especially in nocturnal rodents. The PRC for dark pulses in continuous light (LL), however, has been described in a few mammals only, in nocturnal for bat and for hamster and in diurnal for Octodon degus, suggesting that this PRC is mirror imaging the PRC for light pulses. Therefore, the effect of 1-h and 3-h lasting dark pulses on the circadian wheel-running activity rhythm of mice in continuous light was investigated and then the PRC for dark pulses in LL was drawn up. For comparison, the effect of 1-h lasting light pulses on the circadian wheel-running activity rhythm of mice in DD was examined and the PRC for light pulses in DD was constructed. It appeared that the PRC for dark pulses, to a certain degree, represents a mirror image of the PRC for light pulses in mice. However, the advance region of this PRC is longer than that of delay. The mechanism of dark pulses action is discussed.

Optimal control of one- and two-photon transitions with shaped femtosecond pulses and feedback

This paper reports two pump–probe experiments in sodium where dynamically tailored ultrashort pulses from a Ti:Sapphire-pumped optical parametric amplifier were employed. The first study focuses on the one-photon Na(3s→3p) transition to derive sensitive criteria which judge the performance of a frequency-domain pulse shaper using a spatial light modulator. On the basis of the interpretation, follow-up experiments are suggested to test their cogency. The second experiment uses coherent quantum control by placing an appropriate phase distribution on the incident beam to enhance or cancel the transition probability in the nonresonant two-photon process Na(3s→→5s). Ignorant of the “ideal” phase function, an evolutionary algorithm which uses a feedback derived from the experiment performs the optimization and produces the desired bright or dark pulses within a few minutes. Attention is given to the role of resonant 3s→3p transitions excited by the spectral wings of the pump pulse. Different parametrizations of the phase distribution have been examined. Two of these produced solutions which had not previously been predicted by theory still meet the objective of the experiment. The study represents the first successful application of a feedback-organized self-learning algorithm to the design of dark pulses.

CikA, a bacteriophytochrome that resets the cyanobacterial circadian clock.

The circadian oscillator of the cyanobacterium Synechococcus elongatus, like those in eukaryotes, is entrained by environmental cues. Inactivation of the gene cikA (circadian input kinase) shortens the circadian period of gene expression rhythms in S. elongatus by approximately 2 hours, changes the phasing of a subset of rhythms, and nearly abolishes resetting of phase by a pulse of darkness. The CikA protein sequence reveals that it is a divergent bacteriophytochrome with characteristic histidine protein kinase motifs and a cryptic response regulator motif. CikA is likely a key component of a pathway that provides environmental input to the circadian oscillator in S. elongatus.

Age-related changes in circadian responses to dark pulses.

Aging involves many alterations in circadian rhythms, including a loss of sensitivity to both photic and nonphotic time signals. This study investigated the sensitivity of young and old hamsters to the phase advancing effect of a 6-h dark pulse on the locomotor activity rhythm. Each hamster was tested four times during a period of approximately 9 mo; periods of exposure to a 14-h photoperiod were alternated with the periods of exposure to constant light (20-80 lx), during which the dark pulses were administered. There was no significant difference in the phase shifts exhibited by the young (4-10 mo) and old hamsters (19-25 mo) or in the amount of wheel running activity displayed during each dark pulse. However, young hamsters had a significantly greater propensity to exhibit split rhythms immediately after the dark pulses. These results suggest that, although aging does not reduce the sensitivity of the circadian pacemaker to this nonphotic signal, it alters one property of the pacemaker, i.e., the flexibility of the coupling of its component oscillators.

Circadian clock-protein expression in cyanobacteria: rhythms and phase setting.

The cyanobacterial gene cluster kaiABC encodes three essential circadian clock proteins: KaiA, KaiB and KaiC. The KaiB and KaiC protein levels are robustly rhythmical, whereas the KaiA protein abundance undergoes little if any circadian oscillation in constant light. The level of the KaiC protein is crucial for correct functioning of the clock because induction of the protein at phases when the protein level is normally low elicits phase resetting. Titration of the effects of the inducer upon phase resetting versus KaiC level shows a direct correlation between induction of the KaiC protein within the physiological range and significant phase shifting. The protein synthesis inhibitor chloramphenicol prevents the induction of KaiC and blocks phase shifting. When the metabolism is repressed by either translational inhibition or constant darkness, the rhythm of KaiC abundance persists; therefore, clock protein expression has a preferred status under a variety of conditions. These data indicate that rhythmic expression of KaiC appears to be a crucial component of clock precession in cyanobacteria.

Pathophysiology of human circadian rhythms.

The 24 h profiles of hormonal secretions represent a good model for the study of the human circadian system. Diurnal hormonal variations generally reflect the modulation of ultradian or pulsatile release at 1-2 h intervals by signals occurring at nearly 24 h periods and result from the interaction of an internal timekeeping system--or circadian clock--with the sleep-wake homeostasis and various environmental factors, including the light-dark cycle, periodic changes in activity levels and the meal schedule. This temporal organization is altered in many pathophysiological conditions, including ageing, sleep loss, night or shift work, jet lag, affective disorders and endocrine diseases. Both photic and non-photic stimuli may affect the regulation of the circadian pacemaker and, therefore, the diurnal pattern of hormonal secretions. Appropriately timed stimuli may induce either a phase-advance or a phase-delay of the circadian clock, according to the timing of administration. Phase-shifting effects have been shown in humans for light and for dark pulses, physical exercise, melatonin and melatonin agonists, and benzodiazepine hypnotics. These results open new perspectives for the treatment of a variety of disorders involving dysregulation of the circadian rhythmicity.

Observation of dark-pulse formation in gain-clamped semiconductor optical amplifiers by cross-gain modulation

We have measured the ultrafast simultaneous cross-gain and laser mode dynamics in a gain-clamped semiconductor amplifier perturbed by an intense detuned 150 fs pump pulse. Besides relaxation oscillations, we demonstrate the instantaneous formation of a dark pulse in the laser mode that repeats itself with a period given by the cavity round-trip time. The dark pulse sequence subsequently decays into two-mode beating and is shown to weakly cross modulate the amplifier gain. To describe dark-pulse formation a time- and spatially dependent model based on rate equations is necessary. The experimental results are in reasonable agreement with numerical simulations.

Influence of hot carrier dynamics on pulse propagation in semiconductor lasers

We time resolve the dynamic response of InGaAsP quantum-well semiconductor diode lasers after injection of a femtosecond pulse, using ultrafast upconversion. The injection of a single off-resonant pulse leads to a very fast generation of picosecond ‘dark pulses’, which then generate bright pulses again, leading to dark-pulse–bright-pulse oscillations with a change-over period of 500 ps. We suggest that nonlinear gain compression causes these oscillations.

Shock waves in discrete nonlinear Schrödinger equations

It is shown that in nonlinear differential–difference equations, which in the continuum limit are reduced to the nonlinear Schrödinger equation, localized excitations, reminding shock waves in liquids and gasses can propagate. Such waves may have either the conventional profile of shock waves or a shape of dark pulses evolving against a background. At the initial stages of evolution the shock waves are described by the equation u t + uu x =0 and split out in a train of soliton-like pulses after the shock is developed.

Generation of vector dark-soliton trains by induced modulational instability in a highly birefringent fiber

We present a set of experimental observations that demonstrate the generation of vector trains of dark-soliton pulses in the orthogonal axes of a highly birefringent optical fiber. We generated dark-soliton trains with terahertz repetition rate in the normal group-velocity dispersion regime by inducing a polarization modulational instability by mixing two intense, orthogonal continuous laser beams. Numerical solutions of the propagation equations were used to optimize the emission of vector dark pulses at the fiber output.

Light-Dark Entrainment of Circadian Activity Rhythms of the Diurnal Indian Palm Squirrel (Funambulus pennanti)

A recent focus of chronobiological studies has been to establish diurnal models as alternatives to the more frequently used nocturnal rodents. In the present study, light-dark (LD) entrainment characteristics were examined in one diurnal species, the Indian palm squirrel (Funambulus pennanti). Palm squirrels showed strongly diurnal locomotor activity rhythms (˜ 88 percent) under light-dark (LD) cycles, with activity bimodally distributed during the L phase. In comparison to a dim LD cycle, exposure to a bright LD cycle caused a phase advance in the onset of activity, an increase in daily activity levels and an increase in the duration of activity. Percentage diurnality, however, did not vary between bright and dim LD cycles. Activity rhythms reentrained in significantly fewer days after an 8 hour phase delay of the LD cycle compared to an 8 hour phase advance. In both cases, the direction of reentrainment followed the direction of the LD shift. When exposed to single light pulses (1 hour) presented at the same time each day, 6/7 squirrels entrained. Under a skeletal photoperiod cycle (2 x 1 hour light pulses each day), 6/8 squirrels showed stable entrainment. The remaining squirrels exhibited rhythm splitting, with each component synchronising in an unstable manner with one of the light pulses. Under entrainment to single light pulses and to the skeletal photoperiod cycle, the phase angle of entrainment was negatively correlated with t. Finally, when exposed to a skeletal scotoperiod cycle (2 x 1-hour dark pulses each day), only 3/8 squirrels entrained, while the others free-ran. Two of the entrained squirrels showed spontaneous phase reversals during entrainment. As with other species, the activity rhythm of palm squirrels appears to be controlled by two separate self-sustaining oscillators. The strongly diurnal nature of palm squirrels make them a promising diurnal model for studies examining endogenous and exogenous influences on circadian functioning.

Natural entrainment without dawn and dusk: the case of the European ground squirrel (Spermophilus citellus).

Observational data collected in the field and in enclosures show that diurnal, burrow-dwelling European ground squirrels (Spermophilus citellus) never were above ground during twilight at dawn or at dusk. The animals emerged on average 4.02 h (SD = 0.45) after civil twilight at dawn and retreated in their burrows on average 2.87 h (SD = 0.47) before civil twilight at dusk. Daily patterns of light perceived by these burrowing mammals were measured with light-sensitive radio collar transmitters in an enclosure (the Netherlands) and in the field (Hungary). The observational data are corroborated by the telemetry data, which show clear daily patterns of timing of light perception including light perceived from the burrow entrances. The first light was observed by the animals on average 3.54 h (enclosure, SD = 0.45) and 3.60 h (field, SD = 0.31) after civil twilight at dawn, whereas the final observed light was on average 3.04 h (enclosure, SD = 0.64) and 2.02 h (field, SD = 0.72) before civil twilight at dusk. Thus, the animals do not perceive the rapid natural light-dark (LD) transitions that occur at civil twilight. Instead, they generate their own pattern of exposure to light within the natural LD cycle. The classical phase response model for entrainment by light or dark pulses cannot explain how the circadian system of this species remains entrained to the external, natural LD cycle while the major LD transitions are created by its own behavior.

Coherent quantum control of multiphoton transitions by shaped ultrashort optical pulses

Multiphoton transitions can be reached by many routes through a continuum of virtual levels. We show that the transition probability of two-photon and multiphoton processes can be controlled by tailoring the shape of an ultrashort excitation pulse, so that the many paths leading to the final state interfere to give a desired probability amplitude. We analyze the effect of pulse shapes on N-photon absorption as well as on Raman transitions. We show theoretically that certain tailored dark pulses do not excite the system at all, while other shaped pulses induce transitions as effectively as transform limited pulses, even when their peak amplitudes are greatly reduced. These results are confirmed experimentally for two-photon transitions in atomic cesium. @S1050-2947~99!00808-2#

Complete population transfer between nonresonant tunneling states induced by a train of laser pulses

Complete population transfer between nonresonant tunneling states in a double-well system is predicted to occur when a train of bright or dark laser pulses drives transitions to an excited state in the system. The transition induces the phase shift of the wave packet involved in the transition and alters successive evolutions of the wave packets of the nonresonant states as a result of quantum interference, resulting in complete tunneling.

Phase dependent response of vasoactive intestinal polypeptide to light and darkness in the suprachiasmatic nucleus

Responsiveness of the vasoactive intestinal polypeptide (VIP) content to light and darkness in the rat suprachiasmatic nucleus (SCN) was examined by enzyme immunoassay of micropunched tissues. VIP content in the SCN has been shown to decrease monotonically in animals maintained in illumination. Decreases in VIP content in the SCN in response to both 6-h light and dark pulses depended on the phase of the circadian cycle when the pulses were applied. Light imposed at circadian time (CT) 18 or CT 22 was more effective in suppressing VIP levels than light exposure of the same intensity imposed at CT 0 or CT 6. Darkness interrupting continuous light was more effective at around CT 0 and less effective at around CT 12. These results suggest that VIP responsiveness to light and darkness in the SCN is regulated by the circadian clock in different ways and are correlated with phase-dependent phase shifts in the activity rhythm after light and dark pulses.

Generation of dark pulse trains from continuous-wave light using cross-phase modulation in optical fibers

A technique for the generation of dark pulse trains from continuous-wave (cw) light is presented. It consists of co-propagating a cw signal with intense pump pulses in an optical fiber where both the signal and the pump experience normal group-velocity dispersion. The pump imposes a positive frequency chirp on the signal through cross-phase modulation while normal dispersion tends to chip out the signal energy in the chirped region, thus leading to the generation of a dark pulse train with a repetition rate identical to that of the pump. A train of 30.3 ps dark pulses has been observed when using 31.7 ps pump pulses from an actively mode-locked fiber ring laser. The experimental results agree well with numerical simulations.

Coherent quantum control of two-photon transitions by a femtosecond laser pulse

Coherent quantum control1,2,3 has attracted interest as a means to influence the outcome of a quantum-mechanical interaction. In principle, the quantum system can be steered towards a desired state by its interaction with light. For example, in photoinduced transitions between atomic energy levels, quantum interference effects can lead to enhancement or cancellation of the total transition probability. The interference depends on the spectral phase distribution of the incident beam; as this phase distribution can be tuned, the outcome of the interaction can in principle be controlled. Here we demonstrate that a femtosecond laser pulse can be tailored, using ultrashort pulse-shaping4,5,6,7 techniques, to control two-photon transitions in caesium. By varying the spectral phases of the pulse components, we observe the predicted cancellation of the transitions due to destructive quantum interference; the power spectrum and energy of these ‘dark pulses’ are unchanged. We also show that the pulse shape can be modified extensively without affecting the two-photon transition probability.

An NK 1 receptor antagonist affects the circadian regulation of locomotor activity in golden hamsters

Substance P (SP) is a neuromodulator which may participate in the photic regulation of the circadian timing system in mammals. The biological effects of SP are mediated by interaction with specific receptors, designated as NK 1, NK 2, and NK 3. The NK 1 subtype receptor is expressed in the circadian system. Experiment 1 was designed to test whether an NK 1 antagonist mimics the effects of dark pulses. Hamsters were housed in constant lighting conditions, either constant darkness or constant light (around 250 lx), and they received an i.p. injection of either the specific NK 1 receptor antagonist, L-760,735 (5 mg/kg), or saline during the mid-subjective day, a time when dark pulses cause a phase-advance in circadian rhythm of locomotor activity. After treatment with the NK 1 antagonist, significant phase-advances of wheel-running activity rhythm were found in constant light, but not in constant darkness. Experiment 2 was designed to test the ability of the NK 1 antagonist to block the phase-delaying and/or the phase-advancing effects of light in animals kept in constant darkness. Phase-advances of locomotor activity rhythm that can normally be induced by light pulses given during the late subjective night were markedly reduced by pre-treatment with the NK 1 antagonist. By contrast, phase-delays that can be induced by lights pulses given during the early subjective night were unaffected by the NK 1 antagonist. These data support the hypothesis that SP within the circadian system may, by interacting with NK 1 receptors, modulate photic responses of the SCN pacemaker.

Ultrafast intensity modulation by Raman gain for all-optical in-fiber processing

We present experimental results on ultrafast intensity modulation using the Raman effect and demonstrate 10-Gbit/s selective pulse erasure. The technique is both broadband and polarization insensitive and has a potential speed in excess of 500 Gbits/s. In addition to performing pulse erasure, this all-optical modulator can shape pulses as a precise, soft aperture scalpel and create short, dark pulses.