Directionality of acoustic orientation in flying crickets

Summary Abdominal flexions associated with flight steering were measured in tethered flyingTeleogryllus oceanicus stimulated with a model of conspecific calling song presented at various intensities and from many directions.Flexions increased in size with stimulus intensity until a plateau level was reached. Flexion amplitude was then approximately constant over a range of 20–30 dB, and decreased at still higher intensities (Figs. 2, 3). The shape of this intensity function results from binaural processing; in unilaterally deafened crickets flexion amplitude increased monotonically with stimulus intensity (Fig. 4).Abdominal flexions were graded with respect to sound location; they were larger for laterally placed sound sources and smaller for sound sources near the midline (Figs. 5, 6).A model for the specification of flight steering movements is presented which accounts for our findings (Fig. 7).     

Responses and song pattern copying of Omega-type I-neurons in the cricket,Gryllus bimaculatus,at different prothoracic temperatures

Summary Omega-type I-neurons (ON/1) (Fig. 1A) were recorded intracellularly with the prothoracic ganglion kept at temperatures of either 8–9°, or 20–22° or 30–33 °C and the forelegs with the tympanal organs kept at ambient temperature (20–22 °C). The neurons were stimulated with synthetic calling songs (5 kHz carrier frequency) with syllable periods (SP in ms) varying between 20 and 100, presented at sound intensities between 40 and 80 dB SPL. The amplitude and duration of spikes as well as response latency decreased at higher temperatures (Figs. 1 B, 2, 6). At lower prothoracic temperatures (8–9 °C) the neuron's responses to songs with short SP (20 ms) failed to copy single syllables, or with moderate SP (40 ms) copied the syllable with low signal to noise ratio (Fig. 3). The auditory threshold of the ON/1 type neuron, when tested with the song model, was temperature-dependent. At 9° and 20 °C it was between 40 and 50 dB SPL and at 33 °C it was less than 40 dB SPL (Fig. 4). For each SP, the slope of the intensity-response function was positively correlated with temperature, however, at low prothoracic temperatures the slope was lower for songs with shorter SPs (Fig. 5). The poor copying of the syllabic structure of the songs with short SPs at low prothoracic temperatures finds a behavioral correlate because females when tested for phonotaxis on a walking compensator responded best to songs with longer SPs at a similar temperature.Abbreviations epsps excitatory postsynaptic potentials - ON/1 omega-type I-neuron - SP syllable period - SPL sound pressure level     

Physiology and tonotopic organization of auditory receptors in the cricketGryllus bimaculatus DeGeer

Summary Physiological recordings were obtained from identified receptors in the tympanal organ ofGryllus bimaculatus. By immersing the prothoracic leg in Ringer solution and removing the anterior tympanic membrane the auditory receptors were exposed without significantly altering the frequency response of the auditory organ (Fig. 1). Each receptor was tuned to a specific sound frequency. For sound frequencies below this characteristic frequency the roll-off in sensitivity decreased from 20–30 dB/octave to 10–15 dB/octave as the characteristic frequency of receptors increased from 3–11 kHz (Fig. 4A). For each individual receptor the slope, dynamic range and maximum spike response were similar for different sound frequencies (Fig. 9A). The receptors were tonotopically organized with the characteristic frequency of the receptors increasing from the proximal to the distal end of the array (Figs. 5, 6). Several receptors had characteristic frequencies of 5 kHz. These receptors were divided into two groups on the basis of their maximum spike response produced in response to pure tones of increasing intensity (Fig. 7). Independent of the tuning of the receptor no two-tone inhibition was observed in the periphery, thus confirming that such interactions are a property of central integration.     

Phonotactic specificity of the cricketTeleogryllus oceanicus: intensity-dependent selectivity for temporal parameters of the stimulus

Summary We have investigated the effects of alterations of several temporal parameters of auditory stimuli, as well as of stimulus intensity changes, on the attractiveness of these stimuli to femaleTeleogryllus oceanicus, as measured by monitoring sound-elicited flight steering responses. AlthoughT. oceanicus has a rhythmically complex calling song, females are attracted by a simpler model consisting of regularly repeating sound pulses. We have found that the two major temporal features of this model, sound pulse duration and pulse repetition rate, are both important for eliciting phonotactic steering responses.Stimuli with altered temporal features had intensity thresholds indistinguishable from the control stimulus (Fig. 3). The majority of crickets, however, ceased to respond to the altered stimuli when the stimulus intensity was sufficiently increased (Figs. 4–7). In some cases, intensity increases resulted in a reversal of the steering response from positive to negative (Fig. 10). Effects of altered temporal parameters were also apparent at lower stimulus intensities, where the amplitudes of steering responses to stimuli with altered parameters were smaller than those in response to the control stimulus (Figs. 8, 9).We considered the possibility that the cessation of responsiveness to stimuli with altered temporal features was due to a temporal pattern-specific diminution of binaural cues for sound localization at high intensities. Experiments performed with unilaterally deafened crickets (Fig. 11) led us to conclude that this was not the case, and that our findings instead reflect the properties of the song recognition mechanism.Abbreviations UIL upper intensity limit - RAF ratio of abdominal flexion     

Mechanics of the transduction of sound in the tympanal organ of adults and larvae of locusts

Summary The mechanical transmission of sound in the tympanal organ of adults and 5th instar larvae ofLocusta migratoria andSchistocerca gregaria has been investigated by means of stroboscopic measurements within a frequency range from 1–20 kHz.Frequency dependent spatial distributions of amplitudes and phases of oscillation on the tympanal membrane and the Müller's organ could be demonstrated. Cuticular structures on the membrane may act as a lever arm (e.g. elevated process) and cause a transformation of the (unidimensional) membrane motion into components of displacements in the Müller's organ perpendicular, as well as even parallel, to the membrane.Sites of maximum relative displacements at distinct frequencies are found to be correlated to the course of the dendrites of the acoustic receptor cells. Differences in morphology of the tympanal organ between the two species as well as between adults and larvae always correspond to differences in the mechanical properties (resonances etc.). Consequently, differences or changes in the neurophysiological response characteristics of the different receptor cells have been found.Based upon these findings a correlation between the anatomical and physiological classification of the receptor cell groups is presented.Abbreviations T1, T2, T3, T6, T7 reference points on the tympanal membrane - M1, M4 reference points on the ganglion of the Müller's organ - K1, K2 reference points on the elevated process     

Efferent activity in theOctopus statocyst nerves

Summary Single unit electrophysiological recordings were obtained from efferent fibres in the statocyst nerves ofOctopus vulgaris. A preparation comprising the CNS and a single statocyst was employed. 42% of the efferents displayed a level of resting activity; transient changes in this activity occurred at irregular intervals.The responses of the efferent units were examined during sinusoidal oscillations of the statocyst at stimulus frequencies between 0.01–1 Hz, and amplitudes up to 35°. 84% of the units showed activity synchronised with the imposed oscillations; the time taken to establish this response varied for different units (Fig. 1).The lowest stimulus frequency at which a unit could be entrained varied for different units, with those units with a resting level of activity having the lowest thresholds. The peak firing frequency of the efferents was found to increase with increasing stimulus frequency or amplitude (Fig. 3). However, the change in firing frequency was much smaller than that reported for the statocyst afferents to similar stimuli.The efferent units of the posterior crista nerve were found to respond to clockwise or anticlockwise rotations (Fig. 4), with the individual units having unipolar responses. The phase response of the units changed little with increasing stimulus amplitude but an increase in phase lag occurred with an increase in the stimulus frequency (Fig. 5). The form of this relationship (Fig. 6) was similar to that reported for the statocyst crista afferents.The principal source of the input to the efferents in these experiments was shown to be afferents from the contralateral statocyst. These results are discussed and compared with data from the vertebrate semicircular canal system.     

Response to sound in crickets without tympanal organs (Gryllus campestris L.)

Summary Acoustic signals (10–100 msec, 5kHz, 70 or 80 dB) have an inhibitory effect on chirping in the cricketGryllus campestris L. After a reaction time of approximately 50 msec there is a period of about 150 msec (at 27 °C) during which it is very unlikely that a chirp will begin. The effect is not abolished by removal of the tympanal organs, antennae and cerci. Electrophysiological recordings made from the neck connectives in freely moving insects show that tympanal ablation does not abolish sound reception.     

Intracellular responses from cells of the medulla of the fly,Calliphora erythrocephala

1. Intracellular recordings were made from cells in medullae of immobilized, intact flies Calliphora erythrocephala. Stimuli were moving gratings or small spots projected onto translucent hemispheres before the fly.—2. Responses to stationary flashes included tonic and phasic slow potentials only. Sustaining and On/Off discharges were recorded from cells silent in the dark. Sustaining, dimming, On/Off, +On-Off, and-On/-Off discharges were recorded from cells spontaneous in the dark (Fig. 1, 2, and 3).—3. Some cells were relatively sensitive to 3 log unit changes in flash intensities; others were insensitive (Fig. 4).—4. Receptive fields of a few cells tested were small-field ipsilateral monocular, large-field ipsilateral monocular, or large-field binocular.—5. A number of types of nondirectional cells were found. Some gave stronger discharges to movement than to stationary flashes (Fig. 5).—6. Directionally-selective cells were generally spontaneous. Some simply fired faster in the preferred direction. Others (Fig. 6) had inhibition in the null diriction with or without hyperpolarizations.—7. Possibly-new nondirectional cells were found that were inhibited by changes of direction of movement (Fig. 7)—8. A number of cells were stained with Procion yellow, using high voltage pulses. Double stainings sometimes occurred (Fig. 8). Present Address: Psychological Laboratory, Downing Street, Cambridge CB2 3EB, U.K.     

Representation of Time-Varying Stimuli by a Network Exhibiting Oscillations on a Faster Time Scale

Sensory processing is associated with gamma frequency oscillations (30–80 Hz) in sensory cortices. This raises the question whether gamma oscillations can be directly involved in the representation of time-varying stimuli, including stimuli whose time scale is longer than a gamma cycle. We are interested in the ability of the system to reliably distinguish different stimuli while being robust to stimulus variations such as uniform time-warp. We address this issue with a dynamical model of spiking neurons and study the response to an asymmetric sawtooth input current over a range of shape parameters. These parameters describe how fast the input current rises and falls in time. Our network consists of inhibitory and excitatory populations that are sufficient for generating oscillations in the gamma range. The oscillations period is about one-third of the stimulus duration. Embedded in this network is a subpopulation of excitatory cells that respond to the sawtooth stimulus and a subpopulation of cells that respond to an onset cue. The intrinsic gamma oscillations generate a temporally sparse code for the external stimuli. In this code, an excitatory cell may fire a single spike during a gamma cycle, depending on its tuning properties and on the temporal structure of the specific input; the identity of the stimulus is coded by the list of excitatory cells that fire during each cycle. We quantify the properties of this representation in a series of simulations and show that the sparseness of the code makes it robust to uniform warping of the time scale. We find that resetting of the oscillation phase at stimulus onset is important for a reliable representation of the stimulus and that there is a tradeoff between the resolution of the neural representation of the stimulus and robustness to time-warp.     

Information processing at a central synapse suggests a noise filter in the auditory pathway of the noctuid moth

1. The central projections of the A1 afferent were confirmed via intracellular recording and staining with Lucifer Yellow in the pterothoracic ganglion of the noctuid moths, Agrotis infusa and Apamea amputatrix (Fig. 1). Simultaneous recordings of the A1 afferent in the tympanal nerve (extracellularly) and in the pterothoracic ganglion (intracellularly) confirm the identity of the stained receptor as being the A1 cell. 2. The major postsynaptic arborizations of interneurone 501 in the pterothoracic ganglion were also demonstrated via intracellular recording and staining (Fig. 2). Simultaneous recordings of the A1 afferent (extracellularly) and neurone 501 (intracellularly) revealed that each A1 spike evokes a constant short latency EPSP in the interneurone (Fig. 2Bi). Neurone 501 receives only monaural input from the A1 afferent on its soma side as demonstrated by electrical stimulation of each afferent nerve (Fig. 2Bii). EPSPs evoked in neurone 501 by high frequency (100 Hz) electrical stimulation of the afferent nerve did not decrement (Fig. 2Biii). These data are consistent with a monosynaptic input to neurone 501 from the A1 afferent. 3. The response of neurone 501 to a sound stimulus presented at an intensity near the upper limit of its linear response range (30 ms, 16 kHz, 80 dB SPL) was a plateau-like depolarization, with tonic spiking activity which continued beyond the end of the tone. The instantaneous spike frequency of the response was as high as 800 Hz, and was maintained at above 600 Hz for the duration of the tone (Fig. 3). 4. The relationship between the instantaneous spike frequency in the A1 afferent and that recorded simultaneously in neurone 501 is linear over the entire range of A1 spike frequencies evoked by white noise sound stimuli (Fig. 4). Similarly, the relationship between instantaneous spike frequency in the A1 afferent and the mean depolarization evoked in neurone 501 is also linear for all A1 spike frequencies tested (Fig. 5). No summation of EPSPs occurred for A1 spike frequencies below 100 Hz.(ABSTRACT TRUNCATED AT 250 WORDS)     

Otoacoustic emissions from insect ears having just one auditory neuron

Sensitive hearing organs often employ nonlinear mechanical sound processing which produces distortion-product otoacoustic emissions. Such emissions are also recorded from insect tympanal organs. Here we report high frequency distortion-product emissions, evoked by stimulus frequencies up to 95 kHz, from the tympanal organ of a notodontid moth, Ptilodon cucullina, which contains only a single auditory receptor neuron. The 2f1–f2 distortion-product emission reaches sound levels above 40 dB SPL. Most emission growth functions show a prominent notch of 20 dB depth (n = 20 trials), accompanied by an average phase shift of 119°, at stimulus levels between 60 and 70 dB SPL, which separates a low- and a high-level component. The emissions are vulnerable to topical application of ethyl ether which shifts growth functions by about 20 dB towards higher stimulus levels. For the mammalian cochlea, Lukashkin and colleagues have proposed that distinct level-dependent components of nonlinear amplification do not necessarily require interaction of several cellular sources but could be due to a single nonlinear source. In notodontids, such a physiologically vulnerable source could be the single receptor cell. Potential contributions from accessory cells to the nonlinear properties of the scolopidial hearing organ are still unclear.     

Zum Mechanismus der biologischen 24-Stunden-Periodik

Summary The level (=arithmetic average of all instantaneous values)of a self-sustained oscillation in general influences all properties of the oscillation, including period, amplitude and shape of the oscillation, and the rate of exchange of energy between the oscillator and its environment. Only when the non-linear damping factor does not depend on the instantaneous value of the oscillating function, but only on the amplitude of the oscillation, are the other properties independent of the average level. The differential equations describing self-sustained oscillations cannot be solved exactly, but methods of approximation are applicable. Numerical solutions to several different forms of the equations will be discussed.In the simplest case (van der Pol equation) all properties of the self-sustained oscillation (e.g. period, amplitude) are extreme when the level is zero. The oscillation continues only within a given range of levels (oscillating range); outside this range, the oscillation damps out. In other modifications of the equation, the oscillating function cannot assume a zero value. In all cases, the extent to which the average level influences the different properties depends on the factor , which describes the position of the oscillation within the range between harmonic and relaxation types of oscillation.In the elementary van der Pol equation, the correlation between level and frequency changes sign within the oscillating range; that is, the circadian rule, demanding an always positive correlation between level and frequency, cannot be fulfilled. Only with an additional non-linearity in the energy of recoil does the correlation remain unchanged in sign throughout the oscillating range. A stability condition demands a positive sign for this non-linearity, and hence, for the correlation (fulfilling the circadian rule); if the sign is negative (violating the circadian rule), the oscillation becomes unstable. With an additional term of the third order, the oscillation acquires a two-peaked shape typical of many circadian oscillations.A simple differential equation describing all general properties of the circadian periodicity must fulfil these conditions: the oscillation must be self-sustained and limited to positive values; and the energy of recoil must be non-linear with a positive coefficient to obtain the appropriate correlation between level and frequency. In the equations here developed the environment directly influences only one parameter of the oscillation, i.e. the level. In addition to the circadian periodicity, the differential equations here examined describe the behavior of several other biological oscillations.

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Die benutzten mathematischen Begriffe folgen — soweit dort angeführt — den Benennungen des DIN-Blattes 1311; im Anhang I sind die wichtigsten Begriffe noch einmal zusammenfassend definiert.     

Dominant side in single-leg stance stability during floor oscillations at various frequencies

Background

We investigated lateral dominance in the postural stability of single-leg stance with anteroposterior floor oscillations at various frequencies.

Methods

Thirty adults maintained a single-leg stance on a force platform for 20 seconds per trial. Trials were performed with no oscillation (static condition) and with anteroposterior floor oscillations (2.5-cm amplitude) at six frequencies: 0.25, 0.5, 0.75, 1.0, 1.25 and 1.5 Hz (dynamic condition). A set of three trials was performed on each leg in each oscillation frequency in random order. The mean speed of the center of pressure in the anteroposterior direction (CoP_ap) was calculated as an index of postural stability, and frequency analysis of CoP_ap sway was performed. Footedness for carrying out mobilizing activities was assessed with a questionnaire.

Results

CoP_ap speed exponentially increased as oscillation frequency increased in both legs. The frequency analysis of CoP_ap showed a peak <0.3 Hz at no oscillation. The frequency components at 0.25-Hz oscillation included common components with no oscillation and those at 1.5-Hz oscillation showed the maximum amplitude among all conditions. Postural stability showed no significant difference between left- and right-leg stance at no oscillation and oscillations ≤1.25 Hz, but at 1.5-Hz oscillation was significantly higher in the right-leg stance than in the left-leg stance. For the lateral dominance of postural stability at individual levels, the lateral difference in postural stability at no oscillation was positively correlated with that at 0.25-Hz oscillation (r = 0.51) and negatively correlated with that at 1.5-Hz oscillation (r = -0.53). For 70% of subjects, the dominant side of postural stability was different at no oscillation and 1.5-Hz oscillation. In the subjects with left- or right-side dominance at no oscillation, 94% or 38% changed their dominant side at 1.5-Hz oscillation, with a significant difference between these percentages. In the 1.5-Hz oscillation, 73% of subjects had concordance between the dominant side of postural stability and that of mobilizing footedness.

Conclusion

In static conditions, there was no lateral dominance of stability during single-leg stance. At 1.5-Hz oscillation, the highest frequency, right-side dominance of postural stability was recognized. Functional role in supporting leg may be divided between left and right legs according to the change of balance condition from static to dynamic.     

Sound-evoked oscillation and paradoxical latency shift in the inferior colliculus neurons of the big fruit-eating bat, <Emphasis Type="Italic">Artibeus jamaicensis</Emphasis>

Frequency tuning, temporal response pattern and latency properties of inferior colliculus neurons were investigated in the big fruit-eating bat, Artibeus jamaicensis. Neurons having best frequencies between 48–72 kHz and between 24–32 kHz are overrepresented. The inferior colliculus neurons had either phasic (consisting in only one response cycle at all stimulus intensities) or long-lasting oscillatory responses (consisting of multiple response cycles). Seventeen percent of neurons displayed paradoxical latency shift, i.e. their response latency increased with increasing sound level. Three types of paradoxical latency shift were found: (1) stable, that does not depend on sound duration, (2) duration-dependent, that grows with increasing sound duration, and (3) progressive, whose magnitude increases with increasing sound level. The temporal properties of paradoxical latency shift neurons compare well with those of neurons having long-lasting oscillatory responses, i.e. median inter-spike intervals and paradoxical latency shift below 6 ms are overrepresented. In addition, oscillatory and paradoxical latency shift neurons behave similarly when tested with tones of different durations. Temporal properties of oscillation and PLS found in the IC of fruit-eating bats are similar to those found in the IC of insectivorous bats using downward frequency-modulated echolocation calls.     

Response characteristics of inferior colliculus neurons of the awake CF-FM batRhinolophus ferrumequinum

Summary The responses of 230 single neurons in the inferior colliculus of the horseshoebat to single tones have been studied, emphasizing systematic analysis of the effective frequency bands, dynamic properties and the time course of responses. Distribution of the units' best excitatory frequencies (BEF) is: low frequency neurons 23% (BEF 3–65 kHz); FM-frequency neurons 25% (BEF 65–81 kHz, i.e., frequencies occurring in the FM-part of the bat's echo signal); filter neurons 45% (BEF 81–88 kHz, i.e., frequencies occurring in the stabilized CF-part of the bat's echo=reference frequency (RF)); high frequency neurons about 7% (BEF > 88 kHz). Tuning curves show conventional shapes (Fig. 1), apart from those of filter neurons, which are extremely narrow. Accordingly, Q_10dB-values (BEF divided by the bandwidth of the tuning curve at 10 dB above threshold) are 80–450 in filter neurons (Fig. 2). Response patterns (Fig. 3) are similar to those of Nucleus cochlearis units (transient, sustained, negative and complex responders) with an increased percentage of complex responders up to 38% and a decreased number of transient responders.All types of spike-count functions are found (Fig. 4); nonmonotonic ones dominating. Maximal spike counts are not at the BEF but a few kHz below. Distinct upper thresholds, especially at the BEF of filter neurons (Fig. 5) lead to abrupt changes in activity by slightly shifting stimulus frequency or intensity.The hallmark of inferior colliculus neurons is inhibition, disclosed by distinct inhibitory areas enfolding and overlapping excitatory ones (Figs. 3 and 5). Duration of inhibition varies with stimulus frequency, but is largely independent of stimulus duration (Fig. 6), whereas rebound of inhibition depends on stimulus duration building up periodic rebound activities, if stimulus duration is lengthened. In addition, there are neurons responding only periodically, regardless of stimulus frequency and intensity (Fig. 7). Inhibition is discussed in terms of improving the neuronal signal/spontaneous noise ratio and altering responsiveness of neurons after stimulation, so that these neurons may be suited to time processing in the acoustic pathway.Supported by grants from Stiftung Volkswagenwerk Az. 111858 and DFG Ne. 146/6ffWe thank Mrs. Nasrin Chayegan and Mrs. Martha Gonnert for technical assistance and Mrs. Angie Barker for her suggestions concerning the English.     

Phasic Burst Stimulation: A Closed-Loop Approach to Tuning Deep Brain Stimulation Parameters for Parkinson’s Disease

We propose a novel, closed-loop approach to tuning deep brain stimulation (DBS) for Parkinson’s disease (PD). The approach, termed Phasic Burst Stimulation (PhaBS), applies a burst of stimulus pulses over a range of phases predicted to disrupt pathological oscillations seen in PD. Stimulation parameters are optimized based on phase response curves (PRCs), which would be measured from each patient. This approach is tested in a computational model of PD with an emergent population oscillation. We show that the stimulus phase can be optimized using the PRC, and that PhaBS is more effective at suppressing the pathological oscillation than a single phasic stimulus pulse. PhaBS provides a closed-loop approach to DBS that can be optimized for each patient.     

Effects of Time-Dependent Stimuli in a Competitive Neural Network Model of Perceptual Rivalry

We analyze a competitive neural network model of perceptual rivalry that receives time-varying inputs. Time-dependence of inputs can be discrete or smooth. Spike frequency adaptation provides negative feedback that generates network oscillations when inputs are constant in time. Oscillations that resemble perceptual rivalry involve only one population being “ON” at a time, which represents the dominance of a single percept at a time. As shown in Laing and Chow (J. Comput. Neurosci. 12(1):39–53, 2002), for sufficiently high contrast, one can derive relationships between dominance times and contrast that agree with Levelt’s propositions (Levelt in On binocular rivalry, 1965). Time-dependent stimuli give rise to novel network oscillations where both, one, or neither populations are “ON” at any given time. When a single population receives an interrupted stimulus, the fundamental mode of behavior we find is phase-locking, where the temporally driven population locks its state to the stimulus. Other behaviors are analyzed as bifurcations from this forced oscillation, using fast/slow analysis that exploits the slow timescale of adaptation. When both populations receive time-varying input, we find mixtures of fusion and sole population dominance, and we partition parameter space into particular oscillation types. Finally, when a single population’s input contrast is smoothly varied in time, 1:n mode-locked states arise through period-adding bifurcations beyond phase-locking. Our results provide several testable predictions for future psychophysical experiments on perceptual rivalry.