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J Neurophysiol 98: 1953-1964, 2007. First published August 8, 2007; doi:10.1152/jn.00427.2007
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Heterogeneous Biophysical Properties of Frog Dorsal Medullary Nucleus (Cochlear Nucleus) Neurons

Sungchil Yang and Albert S. Feng

Department of Molecular and Integrative Physiology and Beckman Institute, University of Illinois at Urbana-Champaign, Urbana, Illinois

Submitted 15 April 2007; accepted in final form 5 April 2007


 ABSTRACT
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
The cochlear nucleus (CN) in mammals, or its counterpart in birds, has multiple subdivisions each containing distinct morphological and functional (i.e., temporal discharge patterns and biophysical properties) cell types that project to different auditory nuclei in the brain stem in parallel. The analogous structure in frogs, the dorsal medullary nucleus (DMN), is a single phylogenetically older structure with no subdivision. Similar to the CN, the DMN has complex cytoarchitecture and contains neurons with diverse morphological phenotypes, but whether these cell types possess distinct biophysical characteristics, like their counterparts in mammals and avians, is unclear. Here we show that DMN neurons in young adult northern leopard frogs (Rana pipiens pipiens) possess heterogeneous biophysical properties. There are four major biophysical phenotypes on the basis of the unit's response (i.e., its temporal firing pattern) to depolarizing currents: onset, phasic-burst, sustained-chopper, and adapting. These cells have distinct membrane input resistances and time constants, spike shapes, current-voltage relationships, first-spike latencies, entrainment characteristics, and ionic compositions (i.e., low-threshold potassium current, Ikl, and hyperpolarization-activated current, Ih). Furthermore, these phenotypes correspond to cells' dendritic morphologies, and they bear similarities and differences to those found in the mammalian CN. The similarities are remarkable considering that amphibians are a distinct evolutionary lineage from birds and mammals.


 INTRODUCTION
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
The dorsal medullary nucleus (DMN) in the amphibian caudal brain stem is analogous to the cochlear nucleus (CN) in mammals. It is the first auditory station in the brain receiving a direct projection from the auditory nerve (Feng 1986Go; Wilczynski and Endepols 2006Go). Although the DMN is a single auditory nucleus, its neurons exhibit diverse temporal discharge patterns in response to tone bursts at the units' characteristic frequencies (Feng and Lin 1994Go; Hall and Feng 1990Go, 1991Go), as observed in the mammalian and avian CN (Koppl and Carr 2003Go; Sullivan 1985Go; see reviews in Rhode and Greenberg 1992Go). These temporal discharge patterns are distinct from those observed in auditory nerve fibers, reflecting the transformation taking place in the DMN and the signal processing therein. DMN neurons having different temporal discharge patterns show varying entrainment abilities when presented with amplitude-modulated stimuli. For example, the phasic-burst and phasic neurons have the highest entrainment ability, i.e., showing time-locked firing to amplitude-modulated stimuli ≤250 Hz (Feng and Lin 1994Go; Hall and Feng 1991Go). The DMN also contains a number of morphological cell types with distinct somatic and dendritic characteristics (Feng and Lin 1996Go)—these show remarkable resemblances to the morphological cell types observed in the mammalian and avian CN (Cant 1992Go; Carr and Boudreau 1991Go, 1993Go; Soares et al. 2002Go).

Although the different morphological cell types in the mammalian CN (mostly in neonates) have been shown to possess distinct biophysical properties and temporal discharge patterns (Manis and Marx 1991Go; Oertel 1999Go; Rhode and Greenberg 1992Go), virtually nothing is known about the biophysical properties of DMN neurons and their underlying cellular mechanisms or their structure–function relationships. In this study, we used whole cell patch recording from brain slices of young adult northern leopard frogs (Rana pipiens pipiens) to investigate the biophysical properties of single DMN neurons. The cells were filled with biocytin to study their morphological characteristics and topographical profiles and structure–function relationships. We found that DMN neurons consist of four major phenotypes based on their intrinsic membrane biophysical properties and dynamic response properties, i.e., firing patterns in response to depolarization currents and entrainment ability in response to repetitive depolarization pulses. In addition, pharmacological studies, using specific blockers for hyperpolarization-activated current (Ih) and low-threshold potassium current (Ikl), revealed their differential expressions in these cell types. These biophysical phenotypes generally corresponded to cells having distinct somatic and dendritic morphologies. The resemblances in the biophysical and morphological characteristics of neurons in the frog DMN and those of mammalian and avian CN suggest the possibility of shared neural coding strategies across the different vertebrate classes.


 METHODS
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
Slice preparation and electrophysiological recordings

To prepare frog brain slices, young adult northern leopard frogs (R. pipiens pipiens) weighing 5–20 g were anesthetized in 0.2% tricaine methanesulfonate (MS-222, Sigma, St. Louis, MO) and decapitated. Once the brain was extracted, it was immediately placed in an appropriate oxygenated (95% O2-5% CO2) Ringer solution (in mM): 112 NaCl, 2 KCl, 3 MgCl2, 24.2 D-glucose, 17 NaHCO3, and 3 CaCl2 (pH 7.4) (Malayev and Debski 1998Go). After removal of the dura and pia mater, the tissue was embedded in a 3.3% solution of low-melting-point agarose (Sigma) dissolved in Ringer solution. After hardening and cooling the agarose block in the freezer (–12°C) for 5–7 min, the block was trimmed to obtain desired slice orientation. The brain stem was sectioned along the transverse plane into 250 to 260 µm slices using a vibratome (Ted Pella, 1,000 plus); only one or two of these brain slices contained the posterior branch of the eighth cranial nerve that innervates the auditory organs in the inner ear. Brain slices were immersed in oxygenated Ringer solution in a tissue chamber for 1–2 h at room temperature before the electrophysiological recording; the chamber was continuously perfused with Ringer solution at a rate of 2 ml/min. A fixed stage microscope (Zeiss Axioskop-2FS) equipped with differential interference contrast optics and a x63 water-immersion objective was used to visualize individual neurons in the slices.

The experimental protocols were reviewed and approved by the University of Illinois Institutional Animal Use and Care Committee (Protocol 02033).

Patch electrodes were fabricated from 1.5-mm-diameter borosilicate glass micropipettes and had impedance of 3–8 M{Omega} when back-filled with the following solution (in mM): 117 K-gluconate, 13 KCl, 1.0 MgCl26H2O, 0.07 CaCl22H2O, 0.1 EGTA, 10 HEPES, 3 ATP-Mg, 0.3 GTP-Na, and 0.3% biocytin (pH 7.4–7.6; osmolarity = 260–270 mOsm). The recording electrode was slowly advanced into the slice until the tip encountered a cell surface under visual monitor. After tight seal formation, the whole cell configuration was obtained by application of a negative pressure to the patch pipette. The initial access resistance typically ranged from 10 to 13 M{Omega} and remained stable during the recording session. Under the current-clamp mode, recordings were accepted when cells had a resting membrane potential between –58 and –70 mV and a series resistance of 9–15 M{Omega}. Depolarizing and hyperpolarizing current steps (250 ms duration) were applied, with sufficient intensity to induce maximal firing and negative peak membrane voltage of up to –120 mV. In addition to current steps, we also applied repetitive stimuli consisting of depolarizing current (1 ms duration or 2 ms for sustained-chopper type II) at various repetition rates, from 5 to 500 pulses/s, at threshold and suprathreshold levels. All recordings were performed in room temperature (~22.5°C) using a Multiclamp 700B amplifier (Molecular Devices, Sunnyvale, CA). Data were collected and analyzed by means of pCLAMP software (Molecular Devices).

Biocytin labeling

To identify the locations of the recorded neurons in the DMN and the cells' morphological characteristics, the cells were filled with biocytin while they were held in whole cell patch mode. Because the cell group spans 400 µm mediolaterally and 300 µm dorsoventrally (Fig. 1) (Feng and Lin 1996Go), we selected DMN neurons from a depth of 300 µm of the dorsal margin of the brain slice. To avoid inadvertent recording from the dorsal extension of the medial vestibular nucleus, the extreme lateral and medial extensions of the DMN were not recorded.


Figure 1
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FIG. 1. Schematic diagram of the frog dorsal medullary nucleus (DMN). A: frog DMN comprises a single auditory nucleus located in dorsolateral medulla oblongata. B: different morphological cell types occupy different regions of nucleus (Feng and Lin 1996Go). VIII nerve, cranial auditory nerve; LVN, lateral vestibular nucleus; MVN, medial vestibular nucleus. Scale bar = 100 µm.

 
At the end of a recording session, we placed the slice(s) in 4% paraformaldehyde overnight. Slices were reacted with avidin-biotin-peroxidase complex (ABC Elite, Vector Labs) (Cox et al. 1996Go), mounted, and cover slipped with permount (Fisher Scientific, Pittsburgh, PA). Labeled neurons were examined under a light microscope and drawn with the aid of a camera lucida drawing attachment. To obtain the mean soma diameter, two measurements of the major (long) axis and the minor (short) axis were averaged and indicated.

Chemicals

Concentrated stock solutions of pharmacological agents were prepared and diluted in Ringer solution to a final concentration before use: ZD 7288 (N-ethyl-1,6-dihydro-1,2-dimethyl-6-methylimino-N-phenyl-4-pyrimidin amine, 50 µM), a specific blocker for Ih, was purchased from Tocris (Ellisville, MO), {alpha}-DTX (a blocker for Ikl, 50 nM) from Alomone Labs (Israel), and TEA (a blocker for Ikh, 2 mM) from Sigma. These drugs were bath applied in final concentrations.

Data analysis

The resting membrane potential (RMP) was measured from the voltage trace 1 min after whole cell configuration was achieved; the potential was corrected for a measured junctional potential of –10 mV. The membrane time constant was represented by the elapse time for the voltage to reach 63% of the peak value and determined by fitting exponential curves to hyperpolarizing voltage responses. The cell's input resistance was calculated from its steady-state membrane potential, i.e., from the voltage change induced by small hyperpolarizing current pulses (–10 to –50 pA). We used the peak amplitude of the first spike (relative to the after-spike membrane potential) at the lowest depolarizing current as the spike amplitude. The first-spike latency at threshold was the time from the onset of a stimulus to the time of occurrence of the peak of the first spike at threshold depolarizing current. The spike half-width was the width of an action potential at the half-maximum amplitude (re: threshold). Numerical results are given as means ± SD in Table 1. Differences of the means among groups were evaluated using Tukey mutiple comparison ANOVA test; difference was significant if P < 0.05 (SAS program).


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TABLE 1. Biophysical and membrane characteristics of the major cell types in the DMN

 
To assess the regularity of firing in neurons displaying sustained discharges, we measured the CVs from their interspike interval histograms. Neurons having a CV of >0.3 were defined as adapting neurons, and those having a CV of 0.3 or lower as chopper neurons (Peruzzi et al. 2000Go).

To gain insight into the strength of hyperpolarization-activated current (Ih) in the different functional cell types, inward currents were induced in voltage-clamp mode in 10 mV steps from –50 to –130 mV. The Ih magnitude was measured by subtracting the peak current amplitude with the peak current amplitude after application of ZD 7288. All negative current values (–pA) obtained for maintaining the negative potentials (–50 to –130 mV) were converted into positive values (pA) and plotted.


 RESULTS
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
The DMN is situated in the dorsolateral region of the medulla at the entrance of the eighth cranial nerve (Fig. 1A) (Butler and Hodos 1996Go; Feng and Lin 1996Go; Wilczynski and Endepols 2006Go). As a reference, the various cell types and their topographical distributions within the DMN are shown in Fig. 1B. We performed intracellular recordings (in whole cell patch mode) from 75 DMN neurons in brain slices of 58 young adult R. pipiens pipiens. Under current-clamp mode, DMN neurons displayed four dominant temporal discharge patterns in response to depolarizing currents (250 ms): onset, phasic-burst, sustained-chopper, and adapting.

Onset neurons

Onset neurons fired one spike with short latencies in response to depolarizing currents, irrespective of the current magnitude between 200 and 800 pA (Fig. 2, A and D). Of the 29 onset neurons recorded, only two cells produced two spikes at the maximum suprathreshold depolarization. To observe the subthreshold voltage transients (or humps) of onset neurons, we applied fine step currents with 25 pA increments, following the procedure described for the mammalian and avian CN (Golding et al. 1999Go; Zhang and Trussell 1994Go). The current increments induced stepwise humps in onset neurons (Fig. 2A, inset), and eventually triggered the firing of an action potential.


Figure 2
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FIG. 2. Representative onset type I neuron in the DMN. A: responses to step depolarizing currents of 0.2, 0.4, and 0.6 nA (under current-clamp mode; resting membrane potential = –62 mV) feature a single spike at current onset, irrespective of magnitude of current. Arrow in inset indicates several depolarizing voltage transients (humps) and spike waveform at an expanded scale. B: responses to hyperpolarizing current steps are characterized by a depolarization sag (shown as transient hyperpolarizing current) and a rebound spike after termination of hyperpolarizing currents of –0.4 nA (not of –0.2 nA). C: I-V relationship between current injection (nA) and membrane voltage (mV) for both the transient (bullet) and steady-state components ({circ}); difference in the two responses to hyperpolarizing currents is caused by depolarization sag. D: firing rate (bullet) and 1st-spike latency ({square}) of this unit as a function of depolarization current; cell's firing rate is unchanged over a wide range of step currents, and change in 1st-spike latency (from 3.61 to 1.75 ms) is smallest among all cell types. E: camera lucida drawings of biocytin-filled onset neurons have appearance of large bushy cells (Ei) or octopus cells (Eii). Inset: schematic outline of transverse section to locate cell. Mean soma diameter is 22.0 (Ei) and 18.5 µm (Eii). Top and bottom calibration bars represent 10 and 100 µm, respectively. a, axon.

 
In response to hyperpolarizing current, these neurons showed an overt depolarization sag, and for 15 of the 29 onset neurons (i.e., the onset type-I neurons), there was a rebound spike when the current was withdrawn (Fig. 2B). In light of the depolarization sag, the cell's current-voltage (or I-V) response curves for its transient and steady-state responses to hyperpolarizing currents showed a divergence (Fig. 2C). The depolarization sag is attributed to the strong presence of a hyperpolarization-activated current (Ih); as to be described later (see GoGoGoGoGoGoGoFig. 10), Ih was abolished with bath application of ZD 7288 (an Ih blocker).


Figure 3
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FIG. 3. Representative onset type II neuron in DMN. A: responses to step depolarizing currents of 0.1, 0.3, and 0.5 nA (under current-clamp mode; resting membrane potential = –64 mV) feature a single spike at current onset, irrespective of magnitude of current. Inset: spike waveform at an expanded scale. B: responses to hyperpolarizing current steps features a depolarization sag (shown as transient hyperpolarizing current) and no rebound spike immediately after termination of hyperpolarizing currents of –0.1 and –0.2 nA. C: I-V relationship between current injection (nA) and membrane voltage (mV) for both the transient (bullet) and steady-state components ({circ}); difference in the 2 responses to hyperpolarizing currents is caused by depolarization sag. D: firing rate (bullet) and 1st-spike latency ({square}) of this unit as a function of depolarization current; cell's firing rate is unchanged over a wide range of step currents, and change in 1st-spike latency is from 3.55 to 1.21 ms. E: camera lucida drawing of biocytin-filled onset neurons has appearance of small bushy cells. Mean soma diameter is 11.5 µm. Left and right calibration bars represent 10 and 100 µm, respectively. a, axon.

 

Figure 4
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FIG. 4. Representative phasic-burst neuron in DMN. A: responses to step depolarizing currents of 0.1, 0.3, and 0.5 nA (under current-clamp mode; resting membrane potential = –60 mV) are characterized by a single spike in response to small current and 2–4 spikes to stronger currents. Inset: spike waveform at an expanded scale. B: responses to hyperpolarizing current steps (–0.1, –0.2 nA) show a rapid but small depolarization sag and no rebound spike. C: I-V relationship between current injection (nA) and membrane voltage (mV) for both the transient (bullet) and steady-state components ({circ}); this cell shows little difference between transient and steady-state responses to hyperpolarizing currents. D: firing rate (bullet) and 1st-spike latency ({square}) of this unit as a function of depolarization current; rate-level function is nonmonotonic but latency shows a monotonic decreasing function. E: biocytin filled phasic-burst cells are located in medial region of DMN, have the appearance of small bushy cells, and project to ipsilateral (Ei), contralateral superior olivary nucleus (Eii), or both (Eiii). Mean soma diameter is 9.2 (Ei), 11.7 (Eii), and 12.1 µm (Eiii). Top and bottom calibration bars represent 10 and 100 µm, respectively. a, axon; arrows represent projection targets as observed in single brain slices.

 

Figure 5
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FIG. 5. Representative type I sustained-chopper in DMN. A: responses to step depolarizing currents of 0.02, 0.1, and 0.2 nA (under current-clamp mode; resting membrane potential = –62 mV) is characterized by a constant interspike interval by progressively greater number of spikes with increasing step current. Inset: spike waveform at expanded scale. B: responses to hyperpolarizing current steps of –0.05 and –0.1 nA are characterized by a depolarization sag with initial hyperpolarizing current, but unlike onset type I neurons, there is no rebound spike after withdrawal of hyperpolarizing current. C: I-V relationship between injection current (nA) and membrane voltage (mV) for both the transient (bullet) and steady-state components ({circ}); transient and steady-state responses to hyperpolarizing currents show a divergence caused by occurrence of depolarization sag. D: firing rate (bullet) and 1st-spike latency ({square}) of this unit as a function of depolarization current; firing rate of sustained-chopper type I neurons can be a monotonic (7 of 16 cells) or a nonmonotonic (9 of 16) function of current. E: biocytin-filled sustained-chopper type I neurons have appearance of fusiform (Ei) or stellate (Eii) cells; these are located in the central or ventral area of DMN. Mean soma diameter is 8.9 (Ei) and 12.5 µm (Eii). Top and bottom calibration bars represent 10 and 100 µm, respectively. a, axon.

 

Figure 6
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FIG. 6. Representative type II sustained-chopper in DMN. A: responses to step depolarizing currents of 0.005, 0.02, and 0.05 nA (under current-clamp mode; resting membrane potential = –60 mV) features a progressively greater spike count (and a constant interspike interval) with increasing step current, but rate decreases with a further increase in current. Note that a small current induces large voltage change caused by high-input resistance (2,579 M{Omega}). B: responses to hyperpolarizing current steps of –0.005 and –0.01 nA. C: I-V relationship between injection current (nA) and membrane voltage (mV) for steady-state components ({circ}). D: firing rate (bullet) and 1st-spike latency ({square}) of this unit as a function of depolarization current. Type II sustained-choppers exhibit strictly nonmonotonic rate level functions. E: biocytin-filled sustained-chopper type II neurons have appearance of small radiate cells and are located in lateral area of DMN. Mean soma diameter is 7.8 µm (Eii). Left and right calibration bars represent 10 and 100 µm, respectively. a, axon.

 

Figure 7
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FIG. 7. Representative adapting neuron in frog DMN. A: responses to step depolarizing currents of 0.06, 0.08, and 0.1 nA (under current-clamp mode; resting membrane potential = –61 mV) feature an overt increase in interspike intervals over time. B: responses to hyperpolarizing current steps of –0.05 and –0.1 nA show a small depolarization sag and no rebound spike. C: I-V relationship between injection current and membrane voltage for both transient (bullet) and steady-state components ({circ}); these 2 components show little difference. D: firing rate (bullet) and 1st-spike latency ({square}) of this unit as a function of depolarization current. Adapting neurons display nonmonotonic rate-level functions. E: biocytin-filled adapting neurons show appearance of radiate (cartwheel) cells, are located in medial portion of DMN, and project to fringe area of DMN. Mean soma diameter is 14.7 µm (Eii). Left and right calibration bars represent 10 and 100 µm, respectively. a, axon.

 

Figure 8
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FIG. 8. Four DMN cell types exhibit different entrainment abilities. A: responses of different DMN phenotypes to repetitive depolarizing pulses (1 or 2 ms duration for sustained-chopper type-II) at near threshold level show that phasic-burst neurons have the strongest entrainment ability (up to 333 pps), whereas type II sustained-choppers fail to follow repetitive pulses even at 20 pps. Arrows point to subthreshold voltage responses. B: entrainment ability for each phenotype is maintained, having a linear relationship from near threshold to suprathreshold level. Current intensities were normalized: Low threshold, 1–1.2; Mid, 1.3–1.5; High, 1.6–2 times threshold current.

 

Figure 9
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FIG. 9. Effect of ZD 7288 on phasic-burst neurons. Ai: application of 50 µM N-ethyl-1,6-dihydro-1,2-dimethyl-6-methylimino-N-phenyl-4-pyrimidin amine (ZD 7288) abolishes depolarizing sag, hyperpolarizes resting membrane potential, and increases cell's input resistance. IC and VC indicate current-clamp and voltage-clamp data, respectively. Voltage-clamp data shows that with drug application, there is a reduction in inward current; difference in current between control and drug conditions is taken as ZD 7288-sensitive Ih current—this is quantitatively plotted in Aii as a function of holding potential (mV). Bi: application of ZD 7288 elevates threshold current, thereby weakening response of a train of depolarization pulses at 333 and 500 pps. However, SD of response latency remains unchanged. Bii: effects of ZD 7288 on threshold for 1–1 firing ({square}) and SD of response latency ({blacksquare}). Error bars represent SE; **P < 0.01 and n.s.P > 0.05, paired Student's t-test.

 

Figure 10
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FIG. 10. Differential effects of ZD 7288 on onset, phasic-burst, and sustained-chopper type I neurons. A: 3 phenotypes show different magnitudes of hyperpolarization-activated inward current. Application of 50 µM ZD 7288 abolished ZD-sensitive Ih current. Bottom traces show voltage steps from –50 to –130 mV with 10 increments (1 s duration). B: plots of ZD-sensitive Ih current as a function of holding potential for the 3 phenotypes. I/V curves of Ih current are very well fitted by exponential curves, with R2 correlation of ~1.

 
Onset type I neurons had the lowest input resistance (44 ± 17 M{Omega}) among all functional phenotypes (Table 1), presumably because of the widespread distribution of Ih channels that are active even at resting membrane potentials and the comparatively large cell size. On average, these cells had a mean soma diameter of 18.8 ± 3.7 µm (n = 6)—this was 46% larger than that of the other cell types (12.5 ± 5.1 µm, n = 16). These neurons also had the shortest time constant (1.3 ± 0.8 ms) and first-spike latency (3.7 ± 2.1 ms).

All but two biocytin-filled onset neurons were large bushy cells (Fig. 2Ei); the two exceptions were octopus cells (Fig. 2Eii) having a soma shaped like an octopus's head and two to three primary dendrites arising from two corners of its soma (Feng and Lin 1996Go). The majority of onset neurons were found in the dorsomedial region of the DMN.

For the remaining 14 onset cells (i.e., the onset type-II neurons), there was no rebound spike even in response to strong (>300 pA) hyperpolarizing currents (Fig. 3B). Similar to type I, type II onset neurons fired only one spike, followed by a brief hyperpolarizing undershoot. Compared with onset type I neurons, the input resistances of type II onset neurons were markedly higher (142 ± 30 M{Omega}), and their time constant (4.0 ± 1.6 ms) was longer, but the first-spike latency was indifferent (Table 1). Onset type II neurons also displayed a strong depolarization sag and divergent I-V curves in response to hyperpolarizing currents (Fig. 3, B and C). Onset type II neurons were concentrated in the medioventral region of the DMN instead of the dorsomedial region where the onset type I cells resided. Their somatic morphology resembled that of small bushy cells (11.1 ± 1.3 µm, n = 5) having ovoidal somata; their dendritic arborization was characterized by several primary dendrites radiating out of different poles of the cell soma, and their axons projected along the ventral or dorsal acoustic tract (Fig. 3E).

Phasic-burst neurons

Phasic-burst neurons also fired only one spike in response to weak depolarizing currents, but unlike onset neurons, application of stronger currents (>300 pA) consistently elicited two to four spikes at increasing interspike intervals (Fig. 4A). A further increase in depolarization current typically suppressed the late spikes, reducing the spike count from four to three to two, without affecting the early spikes or the first-spike latency (Fig. 4D). Phasic-bursts also differed from onset neurons in that they exhibited depolarization sag that was smaller but more rapid than that of onset neurons (Fig. 4B). As such, their transient and steady-state responses to hyperpolarizing currents generally also showed a slight divergence (Fig. 4C). Phasic-bursts had the smallest first-spike amplitude (20.0 ± 6.6 mV) among all functional phenotypes. They had a short first-spike latency (6.8 ± 2.6 ms), a narrow spike half-width (1.0 ± 0.2 ms), and a membrane time constant (5.1 ± 2.4 ms) that ranked second shortest behind the onset neurons.

Inspection of biocytin-filled phasic-burst neurons showed that they showed appearance of small bushy cells with axons projecting to the superior olivary nucleus (SON), either ipsilaterally (Fig. 4Ei), contralaterally (Fig. 4Eii), or bilaterally (Fig. 4Eiii).

Sustained-chopper neurons

The most broadly distributed functional phenotype in the DMN was sustained-choppers. In response to depolarizing currents, these cells showed regular discharges at constant interspike intervals (CV < 0.3) over the duration of the current injection (Fig. 5A). Sustained-choppers (n = 23) could also be divided into two subcategories based on the cell's input resistance and the presence/absence of depolarization sag. Type I sustained-choppers (n = 16) had input resistances of <500 M{Omega} (average = 306 ± 116 M{Omega}; Table 1). The spikes of type I cells displayed overt undershoot and rapid repolarization compared with type II sustained-choppers (Fig. 5A, inset). In response to hyperpolarizing currents, they showed a depolarization sag (Fig. 5B) and hence a divergence of the transient and steady-state responses to hyperpolarization currents (Fig. 5C). About one half of type I sustained choppers exhibited a progressively higher spike count, showing a higher frequency of firing and a shorter interspike interval with increasing current level, i.e., monotonic rate-level functions (Fig. 5D). The remainder of type I sustained-choppers displayed nonmonotonic rate-level functions (data not shown). Biocytin-filled type I sustained-choppers showed appearances of fusiform or stellate neurons (Fig. 5, Ei and Eii).

As shown in Table 1, type II sustained-choppers had the highest input resistance among all functional cell types in the DMN (2,579 ± 484 M{Omega}), the longest time constant (79.9 ± 26.2 ms), and the longest first-spike latency (147 ± 49 ms). Despite the very high-input resistances, during the entire recording period, these cells maintained a stable resting membrane potential and access resistance. Because of the high-input resistance, responses of type II sustained-choppers to depolarizing and hyperpolarizing currents were very slow (Fig. 6, A and B); measurement of their transient response to hyperpolarizing current was meaningless and therefore not carried out. Unlike type I, the spikes of type II sustained-choppers displayed less pronounced undershoot and slow repolarization (Fig. 6A).

All type II sustained-choppers displayed nonmonotonic rate-level functions (Fig. 5D), due presumably to depolarization block (Sivaramakrishnan et al. 2004Go). Biocytin-filled type II sustained-choppers corresponded to "small neurons" presumably considered as local interneurons in the DMN (Feng and Lin 1996Go) (Fig. 6E).

Adapting neurons

Adapting neurons were characterized by a marked firing adaptation (CV > 0.3), i.e., increasing interspike intervals over time with depolarizing current injections (Fig. 7A). These neurons generally showed nonmonotonic rate-level functions (5/7 cells; Fig. 7D). Like phasic-burst neurons, in response to hyperpolarization currents, these cells displayed a small depolarization sag and thus a slight divergence in the hyperpolarization responses of their I-V curves (Fig. 7, B and C). Adapting neurons had intermediate membrane input resistance (208 ± 75 M{Omega}) and time constant (7.2 ± 4.8 ms). Biocytin-filled adapting neurons showed radiating dendritic arborization patterns (Fig. 7E) (Feng and Lin 1996Go), similar to cartwheel cells in the mammalian CN (Golding and Oertel 1997Go).

Entrainment characteristics of DMN neurons

To gain insight into the functional significance of DMN neurons with different biophysical properties, we studied their entrainment ability in response to depolarizing pulse trains at different repetition rates, from 5 to 500 pulses per second (pps). We found that, with near-threshold stimulations, phasic-burst neurons exhibited the strongest entrainment ability with 1–1 firing up to a few hundred pulses per second (Fig. 8A). In contrast, sustained-chopper neurons showed the lowest entrainment ability, with some having difficulties following the pulse train even at 20 pps (Fig. 8A); the absolute position of the aborted spike varied with repetition rate and from cell to cell. Adapting and onset neurons had intermediate entrainment abilities (Fig. 8A). The pooled data for near threshold stimulations (n = 7, 6, 6, 3, and 3 for onset neurons, phasic-burst, type I sustained-choppers, type II sustained-choppers, and adapting neurons, respectively) are shown in Fig. 8B. The differences in the entrainment ability among cell types are statistically significant (P < 0.01, ANOVA test; Fig. 8B).

The differential entrainment ability for the different functional cell types was maintained over a wide range of stimulation levels, from near- to supra-threshold. Because of the broad range of input resistances for these cell types, the absolute currents that could be applied to them were different and thus are normalized in Fig. 8B (low, mid, and high referred to 1–1.2, 1.3–1.5, and 1.6–2 times threshold currents, respectively). The maximum following frequency for phasic-bursts averaged 388 ± 55 pps; those for onset neurons, adapting neurons, type I sustained-choppers, and type II sustained-choppers were 255 ± 18, 333 ± 00, 250 ± 00, and 166 ± 00 pps, respectively.

Strength and role of hyperpolarization-activated current (Ih)

To determine the presence of Ih and its functional role in the different cell types, we applied 50 µM ZD 7288 to the bath and examined the units' responses to membrane polarizations under current-clamp and voltage-clamp modes. All phasic-burst neurons tested showed a robust depolarization-sag when membrane was hyperpolarized, indicating the presence of Ih (Fig. 9Ai); Ih was stronger with increasing membrane hyperpolarization (Fig. 9Aii). Application of ZD 7288 abolished the depolarization sag in the current clamp data and the hyperpolarization-activated inward current in the voltage clamp data (Fig. 9Ai). Drug application also hyperpolarized the cell's resting membrane potential by 10 ± 2.7% and increased the cell's input resistance by 101 ± 27%. Note that Ih remained active at membrane potential of between –60 and –70 mV, around which the entrainment took place.

To assess the contribution of Ih to the cell's entrainment ability, we performed the entrainment tests before and during bath application of ZD 7288. We found that drug application lowered phasic-burst cell's entrainment ability; under current-clamp mode, the drug elevated the threshold for 1:1 firing (Fig. 9Bii) and reduced the number of spikes (500 pps) at suprathreshold levels (Fig. 9Bi), without any effect on the response latency (Fig. 9Bii). The jitter of response latency (the elapse time from the onset of stimulation to the peak of the action or subthreshold potential) was measured by calculating the SD of the average response latency to the five current pulses.

Of all the functional cell types, onset neurons showed the strongest ZD 7288–sensitive Ih (n = 4, 315 ± 41 pA at –100 mV; Fig. 10, A and B). In contrast, at the same membrane potential (–100 mV), type I sustained-choppers (n = 2) showed generally weak Ih, averaging 38 ± 20 pA (Fig. 10, A and B), with phasic-bursts having an intermediate Ih (n = 3, 179 ± 37 pA; Fig. 10) . The magnitude of Ih (to –100 mV holding potential) was significantly different between cell types (P < 0.01, ANOVA test). In mammals, Ih shows a sigmoidal function of the membrane potential—it begins to activate near the RMP, and its activity is saturated at approximately –110 mV (Pape 1996Go). In frog DMN, however, Ih was well fitted with an exponential (rather than sigmoidal) curve even to membrane potential of –130 mV.

Roles of low-threshold (Ikl) and high-threshold potassium current (Ikh)

To assess the magnitude and role of Ikl in the different cell types, we applied 50 nM {alpha}-DTX, an Ikl blocker, into the bath. We found that application of {alpha}-DTX transformed the firing patterns of onset type I and type II neurons as well as that of phasic-bursts. Under {alpha}-DTX, onset type I neurons showed sustained firing at suprathreshold depolarization, onset type II gave transient-chopper discharge (with successively decreasing spike amplitude) followed by rippled membrane oscillation, and phasic-bursts exhibited sustained rhythmic firing of mini-spikes (Fig. 11A). In contrast, application of {alpha}-DTX did not change the firing pattern of type II sustained choppers; the unit's responses to depolarization current overlapped completely before and after {alpha}-DTX application (Fig. 11A).


Figure 11
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FIG. 11. Effects of {alpha}-DTX on various DMN phenotypes. A: application of 50 nM {alpha}-DTX has no effect on the temporal firing pattern (in current-clamp mode) of sustained-choppers, but transforms those of onset type I, onset type II, and phasic-burst neurons into sustained, phasic-burst, and sustained-chopping patterns, respectively. Responses to depolarizing current and resting membrane potentials on {alpha}-DTX application are shown in gray color. Bi: effect of {alpha}-DTX on the entrainment ability of an onset type I neuron; shown are its responses to depolarization pulse trains (frequency = 166–333 pps) at various current levels (250–550 pA). Arrows indicate delayed responses under {alpha}-DTX (gray color). Bottom traces show repetitive current stimulations. Bii: application of {alpha}-DTX increases the number of spikes per train of 5 pulses at all current levels (control and {alpha}-DTX data are shown in black and gray symbols, respectively)—currents are normalized because of differential thresholds for onset type I and type II neurons. Biii: application of {alpha}-DTX delays response latencies—delay is significant at low and moderate current levels (P < 0.01, paired Student's t-test).

 
We also examined the effect of {alpha}-DTX on the entrainment ability of DMN neurons to depolarization pulse trains. The action potentials of phasic-bursts were too small for them to be distinguished from the subthreshold responses, and thus these data were not analyzed further. During the control (i.e., no drug) condition, onset neurons tested (n = 5) exhibited 1–1 firing (having different thresholds) to pulse trains from 166 at a low depolarization current to 250 pps at high currents (Fig. 11Bi). Application of {alpha}-DTX increased the spike count at all current levels and lowered the threshold for 1–1 firing, thereby enabling this neuron to give 1–1 firing to pulse train at 333 pps at smaller depolarization currents (Fig. 11, Bi and Bii). Whereas the neuron's ability to fire 1–1 was strengthened on {alpha}-DTX application, its jitter was more pronounced (showing variable response latencies at low current levels; Fig. 11, Bi and Biii). These data suggest that Ikl plays an important role in membrane excitability and precision of temporal coding in the frog DMN.

In contrast to {alpha}-DTX, TEA had a minor effect on the excitability and time coding. Figure 12 shows the effects of TEA on two onset neurons. Application of 2 mM TEA that blocked Ikh broadened the spike half-width (from ~0.7 to ~3.0 ms) and increased the spike amplitude (from ~73 to ~79 mV; Fig. 12, A and B). Application of TEA reduced the units' entrainment ability, mostly because of broadening of their spikes and increasing of spike amplitude (Fig. 12C)—these results suggest the importance of Ikh in determining the shape of action potentials.


Figure 12
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FIG. 12. Effects of TEA on onset neuron. A: application of 2 mM TEA increases half-width and amplitude of action potentials. Shown in gray traces are responses to depolarizing current and resting membrane potentials under TEA application. B: effects of TEA on action potentials. AP, action potential. C: effects of TEA on the entrainment ability of an onset type II neuron; shown are its responses to depolarization pulse trains (frequency: 50–333 pps) at 300 pA current level. Bottom traces show repetitive current stimulations.

 
Topographical distribution of DMN neurons

The majority of onset type I and phasic-burst neurons occupied the dorsomedial region of the DMN. Relative to the above, type II onset neurons showing no rebound spike were distributed more centrally and ventrally. In contrast, sustained-chopper neurons occupied throughout much of the DMN, except the extreme dorsal and medial region of the nucleus. Adapting neurons were found in the medioventral region of the DMN.


 DISCUSSION
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
This study represents the first comprehensive investigation of the biophysical characteristics of central auditory neurons in anurans, providing insight into the cellular basis of central auditory processing. Previous in vitro intracellular studies of frog central auditory neurons have focused primarily on describing their connectivity patterns and basic responses to stimulation of their ascending and descending afferent sources (Christensen-Dalsgaard and Walkowiak 1999Go; Endepols and Walkowiak 1999Go, 2001Go; Luksch and Walkowiak 1998Go; Luksch et al. 1996Go). Results of our patch-clamp experiments showed that DMN neurons exhibit four basic temporal discharge patterns in response to membrane depolarizations, onset, phasic-burst, sustained-chopper, and adapting, similar to what is observed in the CN of birds and mammals that contains multiple subdivisions (Fukui and Ohmori 2004Go; Manis and Marx 1991Go; Oertel 1999Go; Oertel et al. 2000Go; Ostapoff et al. 1994Go; Rhode and Greenberg 1992Go; Soares et al. 2002Go). These four functional cell-types possess distinct intrinsic membrane properties (Table 1), morphological characteristics, and ionic compositions.

Onset neurons

Onset neurons in the DMN typically elicit a single spike at the beginning of depolarization current, and they have a very short time constant, very low input resistance, narrow spike half-width, and very short first-spike latency (Table 1). These properties resemble those of bushy and octopus neurons in the ventral cochlear nucleus in mammals and of principal neurons in the avian magnocellularis nucleus (Carr and Soares 2002Go; Ferragamo and Oertel 2002Go; Golding et al. 1999Go; Manis and Marx 1991Go; Oertel et al. 2000Go; Rothman and Manis 2003Go; Schwarz and Puil 1997Go). Interestingly, labeled DMN onset neurons also have large cell bodies with appearance of bushy cells or octopus cells (Feng and Lin 1996Go).

As is in the avian magnocellularis nucleus (Fukui and Ohmori 2004Go), onset neurons in the frog DMN consist of two subpopulations with distinct biophysical characteristics. Onset type I shows a single spike in response to depolarizing currents and a rebound spike immediately after withdrawal of hyperpolarization currents. The onset type II features an onset spike in response to depolarizing currents but shows no rebound spike even in response to strong hyperpolarizing currents (that induces –120 mV anti-peak response); these cells have higher input resistances compared with the first population. All onset neurons that were successfully labeled appear to be projection neurons within the transverse plane of the brain slice. Axons project either along the dorsal or the ventral acoustic tract (Figs. 2E and 3E); the destination of axonal projection cannot be determined, however, because of the limited thickness of the slice, but in one case, the axon can be seen to project to the contralateral SON.

The larger soma size and the low input resistance of onset neurons implicate that a large conductance is needed for initiating an action potential. As suggested previously (Carr and Soares 2002Go; Ferragamo and Oertel 2002Go; Oertel et al. 2000Go), this feature is important for detecting the depolarizations at synapses with the afferent auditory nerve fibers and for reducing the voltage fluctuations. In the DMN, type I onset neurons exhibit linear I-V relationship in response to depolarizing currents—they can thus summate multiple inputs linearly. Indeed, onset neurons give finely graded voltage humps (indicative of low-threshold potassium conductance, Ikl) to stepwise increasing depolarizing currents because of their low input resistance (Fig. 2A, inset), as shown also for octopus cells in the CN of mammals and nucleus magnocellularis neurons in the avian (Bal and Oertel 2001Go; Golding et al. 1999Go; Oertel et al. 2000Go; Zhang and Trussell 1994Go).

Results of {alpha}-DTX experiments suggested that Ikl plays a role in determining the cell's temporal discharge pattern in response to membrane depolarization. We found that blocking of Ikl transforms a single spike response of onset type I neurons into chopper-like pattern or of onset type II neurons into transient-chopper pattern (Fig. 11). Ikl generally promotes rapid repolarization and thus rapid adaptation of firing. We were therefore surprised that {alpha}-DTX application does not markedly prolong the spike width or increase the spike amplitude; these two parameters under the drug condition (0.73 ± 0.15 ms and 76 ± 2.3 mV) are not significantly different from the control condition (0.72 ± 0.16 ms and 76 ± 1.8 mV; P > 0.05, paired Student's t-test, n = 5). Blocking of Ikl merely reduces the amount of positive current required to reach spike threshold, and increases the spike count, indicating an increase in membrane excitability. In contrast, bath application of 2 mM TEA mostly broadens the cell's spike half-width and increases the spike amplitude. Thus it seems that, for onset neurons, Kv1 is responsible for the cell's temporal precision and Kv3 is involved in determining the spike shape. In the mammalian CN, however, Kv1 seems to be responsible for shaping the peak and half-width of action potentials (Bal and Oertel 2001Go).

Phasic-burst neurons

Phasic-burst neurons feature the smallest spike amplitude and a very short time constant (Table 1), and they exhibit the highest entrainment ability in response to repetitive current stimulation (Fig. 8, phasic-burst). These firing properties and intrinsic membrane characteristics are similar to those of spherical bushy cells in the anteroventral cochlear nucleus (AVCN) and principal neurons in the bird nucleus magnocellularis (Fukui and Ohmori 2004Go; Manis and Marx 1991Go; Oertel 1999Go; Schwarz and Puil 1997Go; Trussell 1999Go)—these cells are well suited for rapid signal transmission and phase locked discharges.

In the frog DMN, the second and third spikes in phasic-burst neurons generally have lower amplitudes (n = 13/15; Fig. 4A), as reported previously for spherical bushy cells in the AVCN (Schwarz and Puil 1997Go). In the AVCN, the reduced amplitudes are shown to be caused by Na+ inactivation and/or voltage-activated K+ conductance. Na+ inactivation together with voltage-activated K+ conductance is also responsible for suppressing the firing duration (Rothman and Manis 2003Go; Schwarz and Puil 1997Go). In the frog DMN, application of blocker of Ikl transforms phasic-burst into sustained-chopper (Fig. 11), suggesting that low-threshold potassium conductance alone (without Na+ inactivation) can account for the phasic-burst pattern.

Like onset neurons, phasic-burst neurons also show a robust Ih, as shown by their responses to hyperpolarization voltage steps, despite exhibiting only a small depolarization sag in response to hyperpolarizing current (Fig. 9A). The small size of depolarization sag is likely attributed to the depolarization effect of Ih (shown by membrane hyperpolarization after the application of ZD7288 that abolishes the Ih) as well as the sizable ZD-nonsensitive current (Fig. 10A).

Earlier studies have suggested that Ih improves temporal precision of firing by shortening the cell's time constant and reducing temporal summation, suggesting (but without empirical validation) that these would enhance the cell's entrainment ability (Bal and Oertel 2000Go; Koch and Grothe 2003Go). The result of our ZD experiment shows directly that blocking of Ih reduces the cell's entrainment ability at threshold and suprathreshold levels (Fig. 9Bi)—this is the first direct evidence for the importance of Ih on cell's entrainment ability. However, in agreement with the results of a recent study (Leao et al. 2006aGo), ZD7288 has no effect on the precision of the response latency of AVCN neurons (Fig. 9Bii).

Sustained chopper neurons

Sustained-choppers show sustained and regular firing patterns over the duration of stimulation, and they have the highest input resistance, the longest first-spike latency, and the longest time constant (Table 1). Type I sustained-choppers show depolarization sag in response to hyperpolarization currents; they have an Ih of 38 ± 20 pA at –100 ml. These neurons closely resemble tonic I neurons in the avian nucleus angularis (Soares et al. 2002Go), and stellate neurons in the mammalian CN (Ostapoff et al. 1994Go). As shown in Fig. 8, in response to a train of depolarization pulses, type I sustained choppers show generally inferior entrainment ability compared with onset and phasic-burst neurons.

Type II sustained-choppers have unusually high-input resistance (Table 1). These cells differ from type I sustained-choppers, having different membrane properties and morphologies. Type I and type II sustained-choppers likely serve different functional roles. The very high-input resistance of type II sustained-choppers indicates that they probably have small cell size; anatomical recovery of type II neurons validates this hypothesis, showing that they correspond to small neurons in the DMN (Feng and Lin 1996Go).

In the CN of mammals, there are also two subtypes of sustained-choppers: stellate-D and stellate-T cells; they differ in their biophysical characteristics and in their innervation patterns and axonal/dendritic morphology (Oertel et al. 1999Go; Rodrigues and Oertel 2006Go). The input resistance for stellate-T cells is higher than that for stellate-D cells, but both input resistances are <100 M{Omega}—these are more than one order lower than that of type II sustained choppers in the DMN. Although type II tonic neurons in the nucleus of angularis in birds show a higher input resistance than that of stellate-T and -D cells, having a value in the range of 200–250 M{Omega} (Soares et al. 2002Go), this is still one order below that of type II sustained-choppers in the DMN. Also, neither the stellate-T and stellate-D cells in mammals nor type II tonic cells in avians show the very low entrainment ability exhibited by type II sustained-choppers in the DMN (Fig. 8). It thus seems that type II sustained-choppers are unique, having no obvious biophysical counterpart in other vertebrates.

It is possible that the differences simply reflect the disparities in the age group and myelination pattern of the experimental animals (neonatal in birds and mammals vs. young adult in frogs) or in the absolute cell size (type II sustained choppers in the DMN are very small neurons). It is noted, however, that there are many tiny cells (e.g., granule and golgi cells) in the mammalian CN; these have not been carefully sampled, and it is possible that they may share similar biophysical properties to those reported for type II sustained choppers in the frog DMN.

In response to repetitive depolarization pulses, sustained-choppers exhibit the worst entrainment ability (Fig. 8A). Therefore coding time-varying signals using a temporal code is problematic, particularly at high rates; they are presumably involved in transforming the auditory input into a rate code, as suggested previously (Peruzzi et al. 2000Go). Thus in contrast to onset and phasic-burst neurons, which are well suited for temporal processing, sustained-choppers most likely process nonlocalization tasks in the ascending auditory pathways, e.g., processing of intensity cues. Interestingly, in vivo extracellular studies from the DMN have also shown that the entrainment ability of DMN neurons varies among DMN neurons (Feng and Lin 1994Go). In particular, neurons exhibiting phasic-burst and a class of primarily-like (i.e., PL-3) tone-evoked discharge patterns display superior time-locked responses to a wide range of AM frequencies compared with neurons showing other firing patterns. Whether phasic-burst biophysical phenotype in vitro corresponds to phasic-burst and PL-3 tone-evoked temporal discharge patterns in vivo is unclear.

Adapting neurons

Adapting neurons are characterized by a rapid burst of action potentials in response to onset of depolarizing current, followed by spikes whose interspike interval increases over time. Other than the invariance in spike amplitude, these neurons have similar biophysical characteristics as those of phasic-bursts (Table 1), i.e., short time constant, low input resistance, little depolarization sag in response to hyperpolarizing current, and short first-spike latency. Adapting neurons are also found in much the same topographical locations in the DMN as phasic-bursts. However, in addition to having a different temporal firing pattern, adapting neurons differ from phasic-bursts in their somatic and dendritic morphology. Adapting neurons have the appearance of radiate cells (Fig. 7) (Feng and Lin 1996Go). Adapting neurons presumably account for the diversity of tone-induced primary-like firing patterns found in the frog DMN (Feng and Lin 1994Go; Hall and Feng 1990Go), e.g., primary-like type 1 to 3 with differing adaptation rates, from slow to very fast.

Adapting neurons in the DMN are similar to the radiate (type III tonic) neurons in the avian nucleus angularis (Soares et al. 2002Go); they show linear I-V relationship and they fire a train of overtly adapting spikes in response to strong depolarizing currents. To date, there is no published report of adapting neurons in the mammalian CN; adapting neurons have been observed at lateral lemniscus nuclei and the inferior colliculus (Peruzzi et al. 2000Go; Zhao and Wu 2001Go). However, a recent study showed that cartwheel cells in the dorsal CN exhibit marked adaptations in response to depolarizing currents (J Mancilla and PB Manis, unpublished observations). Thus adapting neurons are present in the first central auditory center across all vertebrates after all.

Comparisons with avian and mammalian CN

As described above, despite the fact that amphibians arise from a different evolutionary lineage, the frog DMN shares many similar coding strategies with the CN of birds and mammals. The similarities suggest that the cell-specific biophysical characteristics in amphibians, avians, and mammalians might have shared a common ancestral origin or alternatively evolved independently. Characterization of the biophysical properties of the first-order central auditory neurons in fishes is therefore crucial for determining the evolutionary origins of such properties in higher vertebrates.

There are specific differences in physiological and morphological features among the different vertebrate classes, however. First, octopus neurons are observed in the mammalian CN and the frog DMN but not in the avian CN. At the same time, the planar neurons that are found in the avian nucleus angularis (having a damped firing pattern; Carr and Soares 2002Go; Soares et al. 2002Go) are not observed in the frog DMN or the CN in mammals (Cant 1992Go). Second, neurons having a pause-build up firing pattern observed in the mammalian dorsal CN (pyramidal neuron; Kanold and Manis 1999Go), and a tonic II pattern observed in the avian nucleus angularis (radiate cell; Soares et al. 2002Go) have yet to be uncovered in the frog DMN. This discrepancy may simply be caused by an age difference in the preparations—in nucleus angularis of the chicken P-build-up pattern disappears after hatching (Fukui and Ohmori 2003Go). Third, as described previously, type II sustained choppers in the frog DMN have no counterparts in avians or mammals.

At this time, it is unclear whether these differences are attributed to the phylogeny of these different vertebrate classes or to the difference in the absolute cell size or the age of animals for slice preparations (i.e., young adult frogs vs. embryonic/neonatal organisms for avians and mammals) A recent study (Bortone et al. 2006Go) showed that the expressions of potassium channels change in developing rat auditory brain stem, with some showing a monotonic increase in the mRNA levels during early development and others showing the opposite trend. In the main nucleus of trapezoid body of mice, sodium persistent and resurgent currents are not present at postnatal day 7 but are robust at postnatal day 14 (Leao et al. 2006bGo). It is therefore possible that the age differences in the slice preparations can account for some of the differences in the findings in amphibians, avians, and mammals. Future research is necessary to pin down the origins of these discrepancies. In mammals, tone-induced temporal discharge patterns have been shown to correspond to neuronal morphology, albeit the correspondence is not one-to-one (Rhode and Greenberg 1992Go); the cell morphology also gives rise to distinct intrinsic membrane properties that again do not bear one-to-one relationships (as described earlier). The absence of 1–1 correspondences is understandable given the heterogeneity of channel expression and synaptic innervation patterns. At this time, it is unclear how the different in vitro biophysical cell types in the DMN correspond to the temporal discharge patterns in response to acoustic stimulation in vivo. Future research involving in vivo intracellular recordings is necessary to establish such correspondences definitively.


 GRANTS
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
This study was supported by National Institute on Deafness and Other Communication Disorders Grant R01-DC-04998 and the Research Board of the University of Illinois.


 ACKNOWLEDGMENTS
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
We thank W. Walkowiak for encouragement and guidance for carrying out the in vitro intracellular recording experiments and C. L. Cox for comments on earlier versions of this paper and for generosity in sharing one of his experimental rigs for this study. S. Yang assisted in many of the experimental phases.


 FOOTNOTES
 
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.

Address for reprint requests and other correspondence: S. Yang, Beckman Inst., Univ. of Illinois, Urbana, IL 61801 (E-mail: yang6{at}uiuc.edu)


 REFERENCES
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
Bal R, Oertel D. Hyperpolarization-activated, mixed-cation current (I-h) in octopus cells of the mammalian cochlear nucleus. J Neurophysiol 84: 806–817, 2000.[Abstract/Free Full Text]

Bal R, Oertel D. Potassium current in octopus cells of the mammalian cochlear nucleus. J Neurophysiol 86: 2299–2311, 2001.[Abstract/Free Full Text]

Bortone DS, Mitchell K, Manis PB. Developmental time course of potassium channel expression in the rat cochlear nucleus. Hear Res 211: 114–125, 2006.[CrossRef][Web of Science][Medline]

Butler AB, Hodos W. Comparative Vertebrate Neuroanatomy: Evolution and Adaptation. New York: John Wiley, 1996, p. 148–152.

Cant NB. The cochlear nucleus: neuronal types and their synaptic organization. In: The Mammalian Auditory Pathway: Neuroanatomy, edited by Webster DB, Popper AN, and Fay RR. New York: Springer-Verlag, 1992, p. 66–116.

Carr CE, Boudreau RE. Central projections of auditory nerve fibers in the barn owl. J Comp Neurol 314: 306–318, 1991.[CrossRef][Web of Science][Medline]

Carr CE, Boudreau RE. Organization of the nucleus magnocellularis and the nucleus laminaris in the barn owl: encoding and measuring interaural time differences. J Comp Neurol 334: 337–355, 1993.[CrossRef][Web of Science][Medline]

Carr CE, Soares D. Evolutionary convergence and shared computational principles in the auditory system. Brain Behav Evol 59: 294–311, 2002.[CrossRef][Web of Science][Medline]

Christensen-Dalsgaard J, Walkowiak W. In vitro and in vivo responses of saccular and caudal nucleus neurons in the grassfrog (Rana temporaria). Eur J Morphol 37: 206–210, 1999.[CrossRef][Web of Science][Medline]

Cox CL, Huguenard JR, Prince DA. Heterogeneous axonal arborizations of rat thalamic reticular neurons in the ventrobasal nucleus. J Comp Neurol 366: 416–430, 1996.[CrossRef][Web of Science][Medline]

Endepols H, Walkowiak W. Influence of descending forebrain projections on processing of acoustic signals and audiomotor integration in the anuran midbrain. Eur J Morphol 37: 182–184, 1999.[CrossRef][Web of Science][Medline]

Endepols H, Walkowiak W. Integration of ascending and descending inputs in the auditory midbrain of anurans. J Comp Physiol [A] 186: 1119–1133, 2001.[CrossRef]

Feng AS. Afferent and efferent innervation patterns of the cochlear nucleus (dorsal medullary nucleus) of the leopard frog. Brain Res 367: 183–191, 1986.[CrossRef][Web of Science][Medline]

Feng AS, Lin WY. Phase-locked response characteristics of single neurons in the frog cochlear nucleus to steady-state and sinusoidal-amplitude-modulated tones. J Neurophysiol 72: 2209–2221, 1994.[Abstract/Free Full Text]

Feng AS, Lin WY. Neuronal architecture of the dorsal nucleus (cochlear nucleus) of the frog, Rana pipiens pipiens. J Comp Neurol 366: 320–334, 1996.[CrossRef][Web of Science][Medline]

Ferragamo MJ, Oertel D. Octopus cells of the mammalian ventral cochlear nucleus sense the rate of depolarization. J Neurophysiol 87: 2262–2270, 2002.[Abstract/Free Full Text]

Fukui I, Ohmori H. Developmental changes in membrane excitability and morphology of neurons in the nucleus angularis of the chicken. J Physiol 548: 219–232, 2003.[Abstract/Free Full Text]

Fukui I, Ohmori H. Tonotopic gradients of membrane and synaptic properties for neurons of the chicken nucleus magnocellularis. J Neurosci 24: 7514–7523, 2004.[Abstract/Free Full Text]

Golding NL, Ferragamo MJ, Oertel D. Role of intrinsic conductances underlying responses to transients in octopus cells of the cochlear nucleus. J Neurosci 19: 2897–2905, 1999.[Abstract/Free Full Text]

Golding NL, Oertel D. Physiological identification of the targets of cartwheel cells in the dorsal cochlear nucleus. J Neurophysiol 78: 248–260, 1997.[Abstract/Free Full Text]

Hall JC, Feng AS. Classification of the temporal discharge patterns of single auditory neurons in the dorsal medullary nucleus of the Northern leopard frog. J Neurophysiol 64: 1460–1473, 1990.[Abstract/Free Full Text]

Hall JC, Feng AS. Temporal processing in the dorsal medullary nucleus of the Northern leopard frog (Rana pipiens pipiens). J Neurophysiol 66: 955–973, 1991.[Abstract/Free Full Text]

Kanold PO, Manis PB. Transient potassium currents regulate the discharge patterns of dorsal cochlear nucleus pyramidal cells. J Neurosci 19: 2195–2208, 1999.[Abstract/Free Full Text]

Koch U, Grothe B. Hyperpolarization-activated current (Ih) in the inferior colliculus: distribution and contribution to temporal processing. J Neurophysiol 90: 3679–3687, 2003.[Abstract/Free Full Text]

Koppl C, Carr CE. Computational diversity in the cochlear nucleus angularis of the barn owl. J Neurophysiol 89: 2313–2329, 2003.[Abstract/Free Full Text]

Leao KE, Leao RN, Sun H, Fyffe REW, Walmsley B. Hyperpolarization-activated currents are differentially expressed in mice brainstem auditory nuclei. J Physiol 576: 849–864, 2006a.[Abstract/Free Full Text]

Leao RN, Naves MM, Leao KE, Walmsley B. Altered sodium currents in auditory neurons of congenitally deaf mice. Eur J Neurosci 24: 1137–1146, 2006b.[CrossRef][Web of Science][Medline]

Luksch H, Walkowiak W. Morphology and axonal projection patterns of auditory neurons in the midbrain of the painted frog, Discoglossus pictus. Hear Res 122: 1–17, 1998.[CrossRef][Web of Science][Medline]

Luksch H, Walkowiak W, Munoz A, ten Donkelaar HJ. The use of in vitro preparations of the isolated amphibian central nervous system in neuroanatomy and electrophysiology. J Neurosci Methods 70: 91–102, 1996.[CrossRef][Web of Science][Medline]

Malayev AA, Debski EA. Serotonin modulates induced synaptic activity in the optic tectum of the frog. Brain Res 781: 167–181, 1998.[CrossRef][Web of Science][Medline]

Manis PB, Marx SO. Outward currents in isolated vental cochlear nucleus neurons. J Neurosci 11: 2865–2880, 1991.[Abstract]

Oertel D. The role of timing in the brain stem auditory nuclei of vertebrates. Ann Rev Physiol 61: 497–519, 1999.[CrossRef][Web of Science][Medline]

Oertel D, Bal R, Gardner SM, Smith PH, Joris PX. Detection of synchrony in the activity of auditory nerve fibers by octopus cells of the mammalian cochlear nucleus. Proc Natl Acad Sci USA 97: 11773–11779, 2000.[Abstract/Free Full Text]

Ostapoff EM, Feng JJ, Morest DK. A physiological and structural study of neuron types in the cochlear nucleus. II. Neuron types and their structural correlation with response properties. J Comp Neurol 346: 19–42, 1994.[CrossRef][Web of Science][Medline]

Pape HC. Queer current and pacemaker: the hyperpolarization-activated cation current in neurons. Annu Rev Physiol 58: 299–327, 1996.[CrossRef][Web of Science][Medline]

Peruzzi D, Sivaramakrishnan S, Oliver DL. Identification of cell types in brain slices of the inferior colliculus. Neuroscience 101: 403–416, 2000.[CrossRef][Web of Science][Medline]

Rhode WS, Greenberg S. Physiology of the cochlear nuclei. In: The Mammalian Auditory Pathway: Neurophysiology, edited by Popper AR and Fay RR. New York: Springer-Verlag, 1992, p. 94–152.

Rodrigues ARA, Oertel D. Hyperpolarization-activated currents regulate excitability in stellate cells of the mammalian ventral cochlear nucleus. J Neurophysiol 95: 76–87, 2006.[Abstract/Free Full Text]

Rothman JS, Manis PB. The roles potassium currents play in regulating the electrical activity of ventral cochlear nucleus neurons. J Neurophysiol 89: 3097–3113, 2003.[Abstract/Free Full Text]

Schwarz DWF, Puil E. Firing properties of spherical bushy cells in the anteroventral cochlear nucleus of the gerbil. Hear Res 114: 127–138, 1997.[CrossRef][Web of Science][Medline]

Sivaramakrishnan S, Sterbing-D'Angelo SJ, Filipovic B, D'Angelo WR, Oliver DL, Kuwada S. GABA(A) synapses shape neuronal responses to sound intensity in the inferior colliculus. J Neurosci 24: 5031–5043, 2004.[Abstract/Free Full Text]

Soares D, Chitwood RA, Hyson RL, Carr CE. Intrinsic neuronal properties of the chick nucleus angularis. J Neurophysiol 88: 152–162, 2002.[Abstract/Free Full Text]

Sullivan WE. Classification of response patterns in cochlear nucleus of barn owl—correlation with functional-response properties. J Neurophysiol 53: 201–216, 1985.[Abstract/Free Full Text]

Trussell LO. Synaptic mechanisms for coding timing in auditory neurons. Annu Rev Physiol 61: 477–496, 1999.[CrossRef][Web of Science][Medline]

Wilczynski W, Endepols H. Central auditory pathways in anuran amphibians: the anatomical basis of hearing and sound communication. In: Hearing and Sound Communication in Amphibians, edited by Narins PM, Feng AS, Fay RR, and Popper AN. New York: Springer-Verlag, 2006, p. 221–249.

Zhang S, Trussell LO. A characterization of excitatory postsynaptic potentials in the avian nucleus magnocellularis. J Neurophysiol 72: 705–718, 1994.[Abstract/Free Full Text]

Zhao M, Wu SH. Morphology and physiology of neurons in the ventral nucleus of the lateral lemniscus in rat brain slices. J Comp Neurol 433: 255–271, 2001.[CrossRef][Web of Science][Medline]





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