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Department of Anatomy and Cell Biology, Indiana University School of Medicine, Indianapolis, Indiana
Submitted 19 July 2004; accepted in final form 10 October 2004
| ABSTRACT |
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70% of the recorded neurons on stimulation of the Schaffer collaterals or the contralateral commissural path. The size of L-PSP was linearly correlated to the decay time constant but not the rising slope of the initial excitatory PSP (EPSP). Intravenous administration of the N-methyl-D-aspartate (NMDA) receptor blocker MK-801 and the GABAA receptor blocker picrotoxin significantly reduced the size of the L-PSP. The spine density and apical dendritic branching length of the neurons that displayed L-PSPs was significantly greater than those that do not. These results indicate that NMDA receptor and GABAA receptor-mediated depolarizing postsynaptic potentials can be revealed in CA1 pyramidal neurons of adult rats in vivo, supporting the physiological relevance of GABAA-mediated depolarization in normal neuronal information processing. The difference in electrophysiological properties and morphological features between neurons that display the L-PSP and the other neurons suggest that they might represent two different subtypes of CA1 pyramidal neurons. | INTRODUCTION |
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-amino-3-hydroxy-5-methyl-4-isoxazolepropionate (AMPA), kainate, and N-methyl-D-aspartate (NMDA) receptors. AMPA and kainate receptors mediate fast excitatory postsynaptic potentials (EPSPs), whereas NMDA receptors mediate slower-rising and slower-decaying EPSPs.
The excitability of hippocampal pyramidal neurons is also influenced by the feedback recurrent (Andersen et al. 1963
, 1964
) and the feedforward (Alger and Nicoll 1982a
) GABA receptormediated synaptic inhibition. GABA mediates its action through both ionotropic GABAA and metabotropic GABAB receptors, which underlie the fast and slow phases of inhibitory postsynaptic potentials (IPSPs), respectively (Sivilotti and Nistri 1991
).
It is traditionally believed that, in the adult mammalian CNS, GABA assumes an inhibitory role, keeping neuronal excitability under control (Macdonald and Olsen 1994
). However, this oversimplified notion has been challenged by many in vitro studies that use adult animals (Stein and Nicoll 2003
). In those studies, exogenous and synaptically released GABA was shown to mediate a long-lasting depolarizing potential that enhanced neuronal excitability under certain conditions (Alger and Nicoll 1982b
; Andersen et al. 1980
; Avoli 1992
; Grover et al. 1993
; Gulledge and Stuart 2003
; Perreault and Avoli 1988
; Staley et al. 1995
; Taira et al. 1997
; Thalmann et al. 1981
; Wong and Watkins 1982
).
The exact mechanisms of the depolarizing effect of GABA in adult animals have been under active investigation. Some studies suggest that there are two types of GABAA receptors on hippocampal pyramidal neurons. The hyperpolarizing responses reflect the activation of synaptic receptors, which are highly concentrated on the pyramidal cell soma and initial segment, whereas depolarizing responses reflect the activation of extra-synaptic or dendritic receptors (Alger and Nicoll 1982a, b
; Gulledge and Stuart 2003
). Other studies show that a collapse in the transmembrane Cl gradient, as well as outflux of HCO3 through GABAA receptor channels, might also play a role (Kaila 1994
; Staley et al. 1995
).
Despite the wealth of literature describing the depolarizing action of GABA in the mature mammalian central neurons, it is not yet clear whether this occurs in vivo. Thus the physiological relevance of the GABAA-mediated depolarization in adult animal has been challenged. We address this issue using sharp-electrode intracellular recording and staining in vivo in CA1 pyramidal neurons of adult rats. This approach offers the advantage of preserving neuronal circuitry as well as minimizing the perturbation to the cytoplasmic content. We found a long-lasting depolarizing postsynaptic potential that resembles the effect of GABA described in vitro but has an additional NMDA receptormediated component. These data support the view that GABAergic interneuron networks can have an excitatory role in vivo in information processing in mature CNS.
| METHODS |
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Intracellular recording and staining in vivo
Anesthetized rats were fixed in the stereotaxic apparatus. The skull was opened to expose the recording site and to place the electrodes. Recording electrodes were pulled with a Kopf pipette puller (model 750, David Kopf Instruments, Tujunga, CA) from glass capillaries with a filament. Tip resistance ranged from 50 to 80 M
when filled with a solution of 5% neurobiotin (Vector Laboratories, Burlingame, CA) in 2 M potassium acetate. Bipolar stimulating electrodes (1 mm apart) were made from insulated stainless steel pins with 1 mm of exposed tip. The stimulating electrodes were placed into the contralateral commissural pathway (AP: 3.74.7 mm, ML: 1.5 mm, DV: 3.5 mm) and/or ipsilateral Schaffer collaterals pathway (AP: 4.75.7 mm, ML: 5.6 mm, DV: 3.9 mm, vertical angle: 25°; Fig. 1).
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Signals were amplified by a high-input impedance amplifier (Axoclamp 2B, Axon instrument, Foster City, CA). The bridge balance was monitored throughout the experiments and adjusted appropriately. Data were digitized at 45 KHz via a computer interface (ITC-16, Instrutech Corp., Long Island, NY) controlled by the data acquisition program (Axodata, Axon Instruments) and stored on a Macintosh computer for off-line analysis. After each successful recording, neurobiotin was iontophoresed into the cell by applying depolarizing current pulses (2 Hz, 300 ms, 1.01.5 nA) for >10 min to ensure sufficient loading.
At the end of the experiment, the animal was deeply anesthetized and transcardially perfused with 0.01 M PBS followed by 4% paraformaldehyde. The brain was removed and stored in the same fixative overnight at 4°C. Coronal sections were cut at 80 µm thickness using a vibratome and incubated in 0.01 M potassium PBS (KPBS, pH 7.4) containing 0.1% horseradish peroxidaseconjugated avidin-D (Vector) and 0.5% Triton X-100 overnight at room temperature. After detection of peroxidase activity with 3,3'-diaminobenzidine (DAB), sections were examined in KPBS. Sections containing labeled cells and stimulating electrode tracks were mounted on gelatin-coated slides and counterstained with cresyl violet for light microscopy.
Three-dimensional reconstruction of the labeled neurons and quantitative analysis of the spine density
Brain sections containing DAB-labeled neurons were incubated with 0.25% osmium tetroxide (OsO4) for 1 h to intensify the staining. The sections were dehydrated and embedded with Embed 812 (EMS, Hatfield, PA). Optimally labeled CA1 neurons in the serial sections were reconstructed using a 60x water-immersion lens and a computer-based neuronal reconstruction program (Neurolucida, Microbrightfield, Colchester, VT). Morphometric data for the dendrites was calculated with the data analysis program NeuroExplore (Microbrightfield, Colchester, VT). These data include total dendritic branch end number (TDBEN), total dendritic branch length (TDBL), and mean dendritic branch length (MDBL; by dividing TDBL with the number of primary dendrites). The dendritic spines of CA1 neurons were examined using a 100x oil-immersion objective lens. From each neuron, five branches of
1 µm diam were selected from the basal dendrites (30100 µm from soma), the proximal portion (50100 µm from the soma), and the distal portion (200300 µm from the soma) of the apical oblique dendrites. The number of the spines on a 20-µm segment of each dendrite was counted, and spine density was calculated as the number of spines per unit length of dendrite.
Electrophysiological data analysis
Both evoked postsynaptic potentials and intrinsic membrane properties of CA1 pyramidal neurons were analyzed using the data analysis program AxoGraph (Axon Instruments). The amplitudes of the postsynaptic potentials were measured as the difference between resting membrane potential and the peak of the response. The duration of the postsynaptic potential was measured at one-half of the peak amplitudes. The slope of the initial EPSP was measured as the time between 10 and 90% of the peak amplitudes. The decay time constant of the EPSP was derived from monoexponential fitting of the decay part of the potentials. The rheobase was defined as the minimum magnitude required for a 200-ms depolarizing current pulse to evoke an action potential at soma. Analysis of action potentials (spike) was performed from the action potentials evoked by the rheobasic current. The spike height was measured as the difference between the resting membrane potentials and the peak of action potentials. The spike duration was measured at one-half of the peak amplitude of the action potentials. The spike threshold was measured at the visually determined inflection point at the onset of an action potential. The membrane time constant was calculated as the time required for the membrane potential to reach 63% of the steady-state amplitudes in response to a hyperpolarizing current pulse (0.3 nA, 200 ms). Input resistance of the membrane was derived from the linear portion of the I-V relationship as the slope of the linear regression fitting line. For calculating the reversal potential of each postsynaptic potential, the amplitude of each component was measured and plotted as a function of corresponding membrane potential. The reversal potential was extrapolated by the intersection of the linear regression line with the membrane potential axis at which the amplitude of the component would be zero.
All values are presented as mean ± SE. ANOVA, posthoc Scheffés test, and paired or unpaired Students t-test were used to detect statistical difference (StatView, Abacus Concepts). P < 0.05 was considered to be significant.
| RESULTS |
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Synaptic responses of the CA1 pyramidal neurons to afferent stimulation
Consistent with previous literature (Schwartzkroin 1986
), low-intensity stimuli (1.5 times of the threshold intensity to evoke EPSP, 1.5 T) to the contralateral commissural path elicited a postsynaptic potential starting with an initial EPSP followed by an IPSP (Fig. 2A). However, with the increase of stimulus intensity to about 3 T, many neurons (62 of 86) began to exhibit a late depolarizing postsynaptic potential (L-PSP) interposed between the fast and slow IPSPs (Fig. 2B). This late component typically saturated at six times the threshold stimulus intensity (6 T). At 6-T stimulation, the amplitude of L-PSPs was 7.3 ± 0.7 mV (n = 29), and the duration was 186.2 ± 10.8 ms (n = 29). Occurrence of the L-PSP was associated with an increase in membrane conductance as indicated by the decrease in the amplitude of membrane potential deflections in response to hyperpolarizing current pulse (Fig. 2C). Although the induction of the L-PSP required relatively strong afferent stimulation, it was not dependent on the appearance of evoked action potentials arising from the EPSPs. Furthermore, L-PSP could not be evoked by direct depolarizing current injection to the soma (Fig. 2D). In some cases, a single stimulus to the afferent could generate spikes from the late depolarizing component while paired-pulse stimulation consistently potentiated the late depolarizing components (Fig. 2, E and F).
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To understand the underlying ionic mechanism of the L-PSP, we first measured the reversal potentials of different components of the postsynaptic potentials. Currents were injected into the recorded neurons to maintain the membrane potential at different levels, and the amplitudes of each postsynaptic potential were measured accordingly (Fig. 6A). The initial EPSP reversal potential was 46.1 mV (n = 18); the fast IPSP reversal potential was 65.5 mV (n = 18); the late IPSP reversal potential was 94.4 mV (n = 18); and the L-PSP reversal potential was 58.4 mV (n = 18; Fig. 6B).
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To test if the difference in electrophysiological properties of recorded neurons had any relationship to the their difference in anatomical locations within hippocampus, we plotted the recording sites with microscopy after staining. We found that the recording sites were randomly distributed within the CA1 region, and the distribution pattern of the morphologically identified L-PSP neurons and nonL-PSP neurons had no detectable difference. Both types of the cells scattered fairly homogeneously within the CA1 region (Fig. 8A). Since the L-PSP had a MK-801sensitive component, we hypothesized that neurons that displayed the L-PSP might receive a relatively higher excitatory drive. Since the excitatory inputs of the CA1 pyramidal neurons mainly impinge on the dendritic spines, we compared spine density between the neurons that displayed L-PSP and those neurons that did not. On the basal dendrites, the spine density in the neurons that displayed the L-PSP (34.5 ± 2.8, n = 12) was significantly higher than that of the neurons that did not display the L-PSP (27.1 ± 2.9, n = 5, P < 0.05; Fig. 8, B and C). The spine density on the proximal portion of the apical dendrites in the neurons that displayed the L-PSP (37.3 ± 3.9) was significantly higher than that of the neurons that did not (31.6 ± 2.3, P < 0.05; Fig. 8C). The spine density on the distal portion of the apical dendrites in the neurons that displayed the L-PSP (30.6 ± 3.6) was also higher than that of the neurons that did not (28.9 ± 3.4), but no statistical significance was detected (Fig. 8C).
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| DISCUSSION |
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70% of the recorded neurons. Both NMDA receptors and GABAA receptors contribute to the generation of the L-PSP. Approximately 30% of the recorded neurons fail to exhibit the L-PSP response under the same stimulation conditions. These neurons have a significantly lower input resistance and display differences in dendritic spine density and branching complexity. Stimulation of afferent, but not direct suprathreshold depolarizing current injection to the soma, can evoke the L-PSP, suggesting that the L-PSP is a synaptically driven event instead of a somatic regenerative event. Consistent with this observation, the generation of the L-PSP is not dependent on the initiation of the evoked action potentials arising from the initial EPSPs. Thus it is unlikely that back-propagating action potentials play a role in L-PSP induction. The induction of L-PSPs requires relatively strong stimulation intensities (>3 T), suggesting that a threshold amount of presynaptic fibers has to be activated (cooperativity). The input-output property of L-PSPs reaches an asymptotic level at higher stimulation intensities (>5 T), which might reflect saturation of receptor activation. L-PSP response does not exhibit input-specificity, since both SC and CC stimulation can elicit indistinguishable response. The lack of input-specificity suggests that the L-PSP might not be specifically mediated through the CA3CA1 connections.
The L-PSP can evoke bursts of spikes, supporting the excitatory nature of this component. It has been shown that strong excitatory synaptic activation can lead to "action potentials" generated within the dendrites, independent of the soma or axon initial segment (Regehr et al. 1993
; Stuart et al. 1997
). The burst of spikes on the L-PSP could also have a dendritic origin.
Since glutamate is the main excitatory neurotransmitter in the hippocampus, and the NMDA component of the synaptic current rises slowly to a peak (
20 ms) and decays bi-exponentially with time constants of 40 and 200 ms, respectively (Lester et al. 1990
), the prolonged duration of the L-PSP prompted us to initially hypothesize that L-PSPs were mediated by NMDA receptors. Regression analysis indicated that the amplitude and duration of the L-PSP was positively correlated to the decay time constant, but not to the rising slope of initial EPSPs. Since, in synapses containing both AMPA and NMDA receptors, the rising slope of EPSP is mainly contributed by the AMPA component, whereas the decay of EPSP is mainly contributed by the NMDA component, the most parsimonious interpretation of this result is that the L-PSP bears certain relationship with the NMDA receptor strength. More direct evidence supporting the role of NMDA receptors in mediating the L-PSP comes from the result that MK-801, the NMDA receptorgated channel blocker, significantly suppresses this response.
On the other hand, a possible role for GABAA receptor involvement needs to be considered. In our study, the GABAA receptor blocker, PTX, significantly reduced the amplitude of the L-PSPs. This indicates that GABAA receptor activation can indeed mediate a depolarizing effect in vivo.
In support of its mixed nature, L-PSPs reverse at 58.4 mV, which lies between the reversal potentials of the glutamatergic receptormediated EPSP and the GABAergic IPSPs. It should be noted that, as a caveat, due to the lack of pharmacological isolation in our in vivo preparation, postsynaptic potentials (i.e., excitatory and inhibitory) temporally overlap with each other to a certain degree. Thus the actual reversal potential for the EPSP should be more depolarized and the fast IPSP reversal potential should be more hyperpolarized than our measured values. Similarly, the true reversal potential of L-PSPs might be more depolarized if measured in the absence of the hyperpolarizing effect of its neighboring fast and slow IPSPs. Additionally, the reversal potential of more distal dendritic synapses is probably not accurately assessed with somatic current injection.
Although the L-PSP has both a MK-801sensitive component and a PTX-sensitive component, due to the lack of an additive effect of MK-801 and PTX in blocking the L-PSP, it is unlikely that it is simply an arithmetic sum of independent NMDA and GABAA receptormediated conduction. According to the feedforward inhibition theory postulated by Alger and Nicoll (1982a)
, a population of interneurons receive afferent excitation and make synapses on pyramidal neuronal dendrites to form the feedforward inhibition. Indeed, there is a strong excitatory drive to the GABAergic interneurons in CA1 region, which is mediated by ionotropic glutamatergic receptors (Davies et al. 1990
). Furthermore, the effect of GABA on dendrites has been shown to be depolarizing (Alger and Nicoll 1979
, 1982a, b
; Andersen et al. 1980
; Gulledge and Stuart 2003
). In line with this theory, it is plausible that MK-801 mainly exerts its effect presynaptically, which leads to a reduction in the NMDA receptormediated excitatory drive to these interneurons and subsequent reduction in GABA release. The reduction in GABA release in turn causes less GABAA receptormediated depolarization on CA1 pyramidal neurons.
Nevertheless, one should not rule out the contribution of the postsynaptic NMDA receptors on CA1 pyramidal neuron to L-PSP expression. The postsynaptic NMDA receptor activation could occur secondary to the depolarization initially caused by GABAA receptor activation, greatly boosting the amplitude of the L-PSP. The findings that MK-801 preferentially affects the later phase of the L-PSP, whereas PTX suppresses the L-PSP fairly uniformly, fit such an explanation.
A small proportion of the CA1 neurons failed to exhibit the L-PSPs regardless of the stimulation intensities and the stimulation pathways (contralateral commissural path or ipsilateral Schaffer collateral path). This group of neurons shows indistinguishable resting membrane potentials and action potential properties compared with the group of neuron exhibiting L-PSPs. However, the input resistance and membrane time constant of these neurons were significantly lower. In theory, these passive membrane properties determine the temporal and spatial summation of the synaptic potential (Koester and Siegelbaum 2000
), thus one can argue that the neurons with smaller input resistance and time constant are not able to amplify and propagate the remotely generated synaptic potentials and therefore fail to display a L-PSP. However, this possibility is not supported by the fact that the failure to elicit a L-PSP is not dependent on the stimulation intensities in these neurons. Rather, the failure to exhibit a L-PSP in these neurons is more likely due to the difference in their synaptic inputs. Since L-PSP generation is dependent on NMDA receptors and GABAA receptors, the failure to generate a L-PSP response could result from the lack of enough glutamatergic excitatory synaptic input to these neurons, as well as the lack of innervations from feedforward interneurons. Such an explanation is supported by the discernible difference in spine density and the proximal apical dendrite branch pattern between the L-PSP neurons and nonL-PSP neurons. Since spines are the site of glutamatergic synaptic contact on the hippocampal pyramidal neurons (Harris and Kater 1994
), the difference in spine expression levels between these two groups of neurons implies that they receive different levels of excitatory input. In addition, previous studies have shown that the proximal dendrites of pyramidal neurons can initiate regenerative local spikes, including sodium, calcium, and NMDA receptormediated spikes (Larkum et al. 2001
; Schiller et al. 2000
), it is likely that these morphological features might correlate to the generation of the L-PSP.
L-PSPs may have important functional implications. Since the hippocampus is implicated in learning and memory formation and hippocampal long-term potentiation (LTP) is postulated to be an underlying cellular substrate (Bliss and Collingridge 1993
; Eichenbaum 1994
), we speculate that the L-PSP could play a potentially important role in synaptic integration and activity-dependent synaptic plasticity. First, prolonged synaptic depolarization would lead to more Ca2+ influx through NMDA receptors and voltage-gated calcium channels, activating a variety of Ca2+-dependent signal transduction cascades that are critically involved in information processing and storage. Second, prolonged synaptic depolarization could promote dendritic spike initiation and back-propagation of somato-axonal action potentials, both of which are critical for spike-timing dependent long-term synaptic plasticity (Hoffman et al. 1997
; Magee and Johnston 1997
; Watanabe et al. 2002
). Indeed, the spiking activities elicited from the L-PSP resemble previously well-documented complex spike bursting that is typical of hippocampal pyramidal cells (Ranck 1973
). This bursting may represent an important form of information coding in the hippocampus (Lisman 1997
). In agreement with this notion, it has been shown that strong stimulation to the Schaffer collateral at theta frequencies can trigger the complex spike bursting, which enables the induction of LTP (Thomas et al. 1998
). It is important to note that the GABAA receptor-mediated depolarization will relieve the Mg2+ block of the NMDA receptor, thus facilitating NMDA receptor-dependent plasticity (Ben-Ari et al. 1997
). Furthermore, the dendritic spike initiation may be facilitated by the cooperative activation of both NMDA and depolarizing GABAA receptors (Larkum and Zhu 2002
; Schiller et al. 2000
). In addition to the implication in physiological situation, the depolarizing effect of GABA has also been implicated in the pathogenesis of epilepsy. There is evidence that interictal epileptic activity in the human temporal lobe is critically dependent on the excitatory action of GABA (Cohen et al. 2002
).
These results provide the first in vivo evidence for the existence of GABAA-mediated excitation under normal physiological conditions in mature neurons. These findings suggest that GABA may play a far more sophisticated role than its postulated inhibitory role in controlling neuronal excitability.
| GRANTS |
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| ACKNOWLEDGMENTS |
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Present addresses: Y. Fan, Department of Neuroscience, Baylor College of Medicine, One Baylor Plaza, Houston, TX 77030; B. Zou, Department of Pharmaceutical Chemistry, UCSF, San Francisco, CA 94131; Z. Pang, Center for Basic Neuroscience, University of Texas Southwestern Medical Center, 6000 Harry Hines Blvd, Dallas, TX 75390.
| FOOTNOTES |
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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: Z. C. Xu, MS 507, Dept. of Anatomy and Cell Biology, Indiana Univ. School of Medicine, 635 Barnhill Dr., Indianapolis, IN 46202 (E-mail: zxu{at}anatomy.iupui.edu)
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