Abstract
Phasic activity in supraoptic nucleus vasopressin neurones is characterized by alternating periods of activity (bursts) and silence. During bursts, activation of a medium afterhyperpolarization induces spike frequency adaptation. Antagonism of A1 adenosine receptors within the supraoptic nucleus decreases spike frequency adaptation and prolongs phasic bursts in vivo, indicating that endogenous adenosine contributes to spike frequency adaptation. Here we used sharp electrode intracellular recordings from supraoptic nucleus neurones in hypothalamic explants to show that endogenous adenosine increases medium afterhyperpolarization amplitude to enhance spike frequency adaptation during phasic bursts. Superfusion of the A1 receptor antagonist 8-cyclopentyl-1,3-dimethylxanthine (CPT, 10 μm) increased intraburst firing rate of phasic neurones (by 2.0 ± 0.7 spikes s−1, P= 0.03) and burst duration (by 141 ± 113 s, P= 0.03). The CPT-induced increase in intraburst firing rate developed over the first few seconds of firing and persisted thereafter. In a separate series of experiments, CPT reduced the amplitude of the medium afterhyperpolarization evoked by a 1 s 20 Hz spike train (by 0.8 ± 0.3 mV, P < 0.001) in supraoptic nucleus neurones; this inhibition was not prevented by 3 mm CsCl (0.8 ± 0.1 mV decrease, P < 0.01) to block the afterdepolarization (which overlaps temporally with the medium afterhyperpolarization). In the presence of apamin to block the medium afterhyperpolarization, CPT did not alter afterdepolarization amplitude. Taken together, these data show that endogenous adenosine enhances medium afterhyperpolarization amplitude to contribute to spike frequency adaptation in phasic supraoptic nucleus neurones.
Vasopressin neurones are principally located within the hypothalamic paraventricular nucleus and supraoptic nucleus and project to the posterior pituitary gland where they release vasopressin (the antidiuretic hormone) into the general circulation to maintain plasma osmolality and blood pressure by promoting antidiuresis and vasoconstriction (Holmes et al. 2001). Vasopressin neurone axon terminals do not sustain intrinsic repetitive firing (Bourque, 1990) and so vasopressin secretion is largely determined by action potential (spike) discharge initiated at the soma. In vivo, vasopressin neurones display a range of spike discharge patterns under basal conditions: some are silent, some are irregular, some display rhythmic ‘phasic’ activity and some are continuously active (Brown et al. 1998, 2007).
Phasic activity is highly efficient for secretion of vasopressin into the circulation (Leng et al. 1999) and is characterized by spike discharge in periods of firing (bursts) that each last tens of seconds, separated by silent periods (interburst intervals) of similar duration (Brown, 2004; Brown & Bourque, 2006). Phasic bursts are sustained by plateau potentials that are generated by temporal summation of non-synaptic afterdepolarizations (ADPs) that follow each spike (Andrew & Dudek, 1983; Armstrong et al. 1994; Li et al. 1995; Li & Hatton, 1997; Ghamari-Langroudi & Bourque, 1998; Brown & Bourque, 2004). Phasic activity is not simply an on–off pattern; spike discharge within bursts undergoes spike frequency adaptation, whereby there is a progressive decrease in firing rate over the first few seconds of bursts (to a steady state rate that is maintained until burst termination) due to activation of a medium afterhyperpolarization (mAHP) (Kirkpatrick & Bourque, 1996).
Vasopressin neurones contain large amounts of neuropeptide in their soma and dendrites from which vasopressin is secreted by exocytosis (Pow & Morris, 1989). This somato-dendritic release is important for modulating phasic activity; vasopressin administration excites irregular or weakly phasic vasopressin neurones (Gouzenes et al. 1998) but inhibits vasopressin neurones displaying robust phasic spike discharge or continuous spike discharge (Ludwig & Leng, 1997; Gouzenes et al. 1998). Hence, somato-dendritic vasopressin might function as a ‘population feedback signal’ to equalize the activity level amongst vasopressin neurones (Moos et al. 1998).
Vasopressin neurones also synthesize and secrete several other factors that have been implicated in modulation of phasic spike discharge in vasopressin neurones (Brown et al. 2008), including the κ-opioid peptide dynorphin (Watson et al. 1982); bursts are terminated by autocrine feedback inhibition of ADPs by somatodendritic dynorphin (Brown & Bourque, 2004; Brown et al. 2006), as well as by activation of a slow afterhyperpolarization (sAHP) (Greffrath et al. 1998; Ghamari-Langroudi & Bourque, 2004), each of which reduce the probability of spontaneous spikes firing as bursts progress (Brown et al. 2006).
Vasopressin neurosecretory granules also contain ATP (Poisner & Douglas, 1968), which is presumably co-released upon somato-dendritic exocytosis. Although ATP induces vasopressin secretion from hypothalamic explants, these effects are truncated by rapid catabolism to adenosine in the extracellular space (Kapoor & Sladek, 2000); this adenosine also influences the spike discharge of vasopressin neurones; in anaesthetized rats, the major effects of endogenous adenosine on spike discharge are to enhance spike frequency adaptation and to reduce burst duration in phasic vasopressin neurones (Bull et al. 2006), suggesting that these effects of endogenous adenosine are activity dependent. A2A receptors are also expressed by supraoptic nucleus neurones (and glia) and activation of these receptors induces depolarization of supraoptic neurones to increase spike discharge (Ponzio et al. 2006). Nevertheless, the major functional role of endogenous adenosine appears to be inhibition (via A1 receptor activation) because inhibition of adenosine uptake reduces spike discharge (Ponzio & Hatton, 2005).
As the major in vivo effects of endogenous adenosine (Bull et al. 2006) are similar to those induced by activation of the mAHP in vitro (Kirkpatrick & Bourque, 1996), we used intracellular sharp electrode recordings from supraoptic nucleus neurones in hypothalamic explants to test the hypothesis that endogenous adenosine increases mAHP amplitude to enhance spike frequency adaptation during spontaneous phasic bursts in supraoptic nucleus neurones.
Methods
Electrophysiology
Conscious female Sprague–Dawley rats (∼200–250 g) were restrained in a soft plastic cone (5–10 s), decapitated and the brains rapidly removed according to a procedure approved by the University of Otago Animal Ethics Committee. A block of tissue 8 mm × 8 mm × 2 mm containing the basal hypothalamus was excised using razor blades and pinned, ventral surface up, to the silicone elastomer base of a superfusion chamber. Within 2–3 min, the excised hypothalamic explant was superfused (at 0.5–1.0 ml min−1 at 32–33°C) with carbogenated (95% oxygen; 5% carbon dioxide) artificial CSF (aCSF; see below) delivered via tubing placed over the medial tuberal region. The arachnoid membrane overlying the supraoptic nucleus was removed using fine forceps, and a tissue paper wick was placed at the rostral tip of the explant to facilitate aCSF drainage. The aCSF (pH 7.4; 295 ± 3 mosmol kg−1) was comprised of (in mm): 120 NaCl, 3 KCl, 1.2 MgCl2, 26 NaHCO2, 2.5 CaCl2 and 10 glucose (Sigma).
Intracellular recordings were made using sharp micropipettes prepared from glass capillaries (1.5 mm O.D. 0.86 mm I.D) pulled on a P-97 Flaming-Brown puller (Sutter Instruments, Novato, CA, USA). Micropipettes were filled with 2 m potassium acetate to yield DC resistances of 70–160 MΩ to a Ag–AgCl wire electrode immersed in aCSF. Voltage recordings were obtained using an Axoclamp 2B amplifier (Molecular Devices, Foster City, CA, USA) in continuous current-clamp (‘bridge’) mode. Digitized signals (5 kHz; DigiData 1320 Interface, Molecular Devices) were stored on a personal computer running pClamp 9.2 (Molecular Devices) and analysed offline.
Recordings were made from supraoptic nucleus neurones impaled with sharp electrodes in superfused hypothalamic explants. The cells had resting membrane potentials more negative than –50 mV, input resistances of > 150 MΩ, and spike amplitudes of > 60 mV when measured from baseline. Each cell displayed frequency-dependent spike broadening and transient outward rectification when depolarized from initial membrane potentials more negative than −75 mV (characteristics specific to supraoptic nucleus neurones (Renaud & Bourque, 1991)). Vasopressin neurones were differentiated from oxytocin neurones by applying increasing hyperpolarizing pulses of 1.5 s duration from a membrane potential of about −50 mV; using this protocol most oxytocin but no vasopressin neurones express a sustained outward rectification and a rebound depolarization (Stern & Armstrong, 1995); none of the neurones reported here expressed a sustained outward rectification and so it is likely that most, if not all, of the neurones tested contained vasopressin.
The adenosine A1 receptor antagonists, 8-cyclopentyl-1,3-dimethylxanthine (CPT; Sigma) and 1,3-dipropyl-8-cyclopentylxanthine (DPCPX; Sigma), were prepared (10 mm) in deionized water, stored frozen until the day of use and bath applied after dilution to 10 μm in aCSF. Apamin (1 mm; Sigma) was prepared in deionized water and bath applied after dilution to 1 μm in aCSF. CsCl (3 m) was prepared in deionized water and bath applied after dilution to 3 mm in aCSF.
Spontaneous phasic activity data analysis
Spikes were identified during spontaneous phasic bursts using the threshold search function on Clampfit (pClamp 9.2) and bursts identified using the ‘bursts analysis’ function with the minimum events set at five spikes.
Intraburst firing rate was measured in 1 s bins. Spike frequency adaptation was calculated as the change of firing rate from the maximum intraburst firing rate to the mean steady-state firing rate between 10 and 15 s after the maximum (expressed as a percentage of maximum intraburst firing rate).
The probability of spike firing (hazard) was calculated from the interspike interval distribution of individual cells using the formula:
where h[i−1,i] is the hazard at interval i, n[i−1,i] is the number of spikes in interval i, n[0,i−1] is the total number of spikes preceding the current interval and N is the total number of spikes in all intervals. This gives the inferred probability (as a decimal) of a cell firing a subsequent spike in any interval after a spike (at time 0), given that another spike has not occurred earlier.
Statistics
All statistical comparisons were completed using SigmaStat software (SPSS Science, Chicago, IL, USA). Non-parametric analyses were used where data failed normality and/or equal variance tests. Where analysis of variance (ANOVA) was used, post hoc Students–Newman–Keuls tests were used only when the F ratio of the ANOVA was significant. P≤ 0.05 was considered statistically significant.
Results
Endogenous adenosine decreases intraburst firing rate, burst duration and increases spike frequency adaptation during spontaneous phasic activity
A1 adenosine receptor antagonism with CPT increases intraburst firing rate and burst duration, and decreases spike frequency adaptation of spontaneously phasic supraoptic nucleus neurones in vivo (Bull et al. 2006). To determine whether these effects are also evident in vitro, we recorded the activity of six supraoptic nucleus neurones displaying spontaneous phasic bursts in hypothalamic explants (e.g. Fig. 1A).
Under basal conditions, the mean (±s.e.m.) firing rate of these neurones was 1.5 ± 0.6 spikes s−1 (measured over ≥ 10 min), and this was not altered by superfusion of 10 μm CPT (P= 0.16, Wilcoxon signed rank test). Nevertheless, 10 μm CPT consistently increased the intraburst firing rate from 5.7 ± 1.1 spikes s−1 to 7.7 ± 0.8 spikes s−1 (P= 0.03) and the burst duration from 29.8 ± 12.2 s to 171.7 ± 111.1 s (P= 0.03), but did not change interburst interval (49.8 ± 16.0 s and 68.5 ± 19.2 s, before and during CPT administration, respectively; P= 0.47; Fig. 1B).
Detailed analysis of the temporal evolution of activity over the course of bursts by calculation of the firing rate in 1 s bins from the onset of burst firing revealed that the CPT-induced increase in firing rate was not evident at the onset of burst firing but increased progressively over the first 3 s of bursts and persisted thereafter (Fig. 1C), indicating that endogenous adenosine inhibition of spike firing is absent at burst onset but rapidly reaches a maximum within the first few seconds of spike firing during spontaneous bursts.
Spike frequency adaptation (calculated by the change of firing rate from the maximum intraburst firing rate to the mean steady-state firing rate between 10 and 15 s after the maximum) was reduced from 48 ± 4% change in firing rate to 39 ± 4% change (P= 0.03, Wilcoxon signed rank test; Fig. 1D).
Endogenous adenosine decreases post-spike excitability during spontaneous phasic bursts in vitro
CPT increases post-spike excitability during phasic bursts in vivo (Bull et al. 2006), and this has been inferred to reflect changes in the post-spike potentials that underpin the plateau potential (Brown et al. 2004, 2006; Sabatier et al. 2004). Accordingly, we calculated the post-spike excitability of supraoptic nucleus neurones during spontaneous phasic bursts in vitro using plots of the hazard function (Brown & Leng, 2000; Sabatier et al. 2004; Brown et al. 2006), which reflect the changes in excitability of neurones after spontaneous spikes by displaying the inferred probability of spike firing with time after the preceding spike, calculated from the interspike interval distribution (Fig. 2A and B). CPT increased the post-spike excitability from ∼50 to 400 ms after each spike (Fig. 2B and C), indicating that endogenous adenosine decreases the probability of spike firing in the period 50–400 ms after each spike during spontaneous phasic bursts.
Endogenous adenosine increases mAHP amplitude in supraoptic nucleus neurones
Activation of the mAHP causes spike frequency adaptation (Kirkpatrick & Bourque, 1996) and because we observed That CPT reduces spike frequency adaptation during spontaneous phasic bursts, we determined the effects of 10 μm CPT (n= 18) or 10 μm DPCPX (n= 4) (to confirm that the effects of CPT were mediated by antagonism of A1 adenosine receptors) on the amplitude of the mAHP elicited in supraoptic nucleus neurones every 20 s (using trains of 5–7 spikes evoked by an 80 ms depolarizing current pulse, with the number of spikes kept constant for each neurone; Fig. 3A). Two-way repeated measures ANOVA showed that the effects of CPT and DPCPX on mAHP amplitude were indistinguishable (P= 0.28). Under these conditions, 10 μm CPT/DPCPX decreased mAHP amplitude by 0.7 ± 0.2 mV (P= 0.02, Student–Newman–Keuls test, n= 22, Fig. 3B).
CPT/DPCPX did not alter the time course of the mAHP. Using pClamp, a standard exponential was fitted to the membrane potential for 1 s after the nadir of the mAHP (the correlation coefficient for all fitted curves was ≥ 0.99); the time constant for the decay of the mAHP was 166.5 ± 15.1 ms and 182.0 ± 32.2 ms, before and during 10 μm CPT/DPCPX administration, respectively (P= 0.44, paired t test, n= 22).
Concomitant with a decreased mAHP amplitude, CPT also increased ADP amplitude in neurones in which this potential was evident (none of the cells tested with DPCPX exhibited an ADP) from 1.7 ± 0.2 mV to 2.3 ± 0.3 mV (P= 0.04, paired t test, n= 11, Fig. 3C).
Endogenous adenosine enhancement of the mAHP is activity dependent
To determine whether the CPT-induced inhibition of mAHP amplitude was activity dependent, we evoked mAHPs using trains of 20 spikes at 1, 2, 5, 10 and 20 Hz in identified supraoptic nucleus neurones (e.g. Fig. 4A and B). CPT (10 μm) decreased the amplitude of the mAHP measured from supraoptic nucleus neurones after 2, 5, 10 and 20 Hz trains (two-way repeated measures ANOVA followed by Student–Newman–Keuls tests, n= 14, Fig. 4C) by 0.4 ± 0.1 mV (P= 0.03), 0.7 ± 0.2 mV (P= 0.003), 0.8 ± 0.2 mV (P= 0.001) and 0.8 ± 0.3 mV (P < 0.001), respectively, but not after a 1 Hz train (0.4 ± 0.1 mV decrease, P= 0.06). Indeed, there was a significant correlation between the frequency of stimulation and the CPT-induced decrease in mAHP amplitude (P= 0.04, Pearson product moment correlation, Fig. 4D), indicating that endogenous adenosine causes an activity-dependent increase in mAHP amplitude in these neurones.
Blockade of the ADP does not alter endogenous adenosine enhancement of the mAHP
The mAHP and ADP overlap temporally (Greffrath et al. 1998) and so it is possible that the observed CPT-induced decrease in mAHP amplitude might result from an offset of the mAHP by an increase in the amplitude of the concomitant ADP. Consequently, we used 3 mm CsCl to block the ADP (Ghamari-Langroudi & Bourque, 1998) to determine whether blocking the ADP would prevent CPT actions on the mAHP in supraoptic nucleus neurones.
In seven supraoptic nucleus neurones in which a clear ADP was present (> 0.5 mV), 3 mm CsCl reduced ADP amplitude from 2.3 ± 0.42 mV to 1.0 ± 0.2 mV (P= 0.02, paired t test; Fig. 5A and B). In eight neurones, the mAHP amplitude after trains of 20 spikes at 1, 2, 5, 10 and 20 Hz was increased by 3 mm CsCl by 0.6 ± 0.1 mV (P= 0.02), 0.7 ± 0.1 mV (P= 0.01), 0.8 ± 0.2 mV (P= 0.003), 1.1 ± 0.2 mV (P < 0.001) and 1.4 ± 0.3 mV (P < 0.001), respectively (Fig. 5C and D).
For four of these neurones, recordings were maintained for long enough to determine the effects of 10 μm CPT on mAHP amplitude after trains of 20 spikes at 1, 2, 5, 10 and 20 Hz in 3 mm CsCl. In 3 mm CsCl, 10 μm CPT reduced mAHP amplitude only after the 20 Hz train (by 0.8 ± 0.1 mV, P= 0.003, two-way repeated measures ANOVA followed by Student–Newman–Keuls tests; Fig. 5E). Nevertheless, in 3 mm CsCl, there was a significant correlation between the frequency of stimulation and the CPT-induced decrease in mAHP amplitude (P= 0.03, Pearson product moment correlation, Fig. 5F), indicating that endogenous adenosine causes an activity-dependent increase in mAHP amplitude by an action on the mAHP itself rather than on the concomitant ADP.
Endogenous adenosine does not alter ADP amplitude
In five neurones, we used 1 μm apamin (which we estimated to be ∼5–10 times greater than the IC50 for apamin against the mAHP in this preparation (Kirkpatrick & Bourque, 1996)) to reduce mAHP amplitude (from −4.0 ± 0.9 mV to −0.8 ± 0.4 mV, P= 0.03, one-way repeated measures ANOVA followed by Student–Newman–Keuls test) and tested the effects of 10 μm CPT on ADP amplitude (Fig. 6A). In the continued presence of 1 μm apamin, 10 μm CPT did not further alter mAHP amplitude (P= 0.70) and did not affect ADP amplitude (P= 0.40, Fig. 6B), confirming that endogenous adenosine does not increase mAHP amplitude via actions on the ADP.
We have previously demonstrated that endogenous activation of κ-opioid receptors causes activity-dependent inhibition of the ADP in supraoptic nucleus neurones (Brown & Bourque, 2004). To determine whether endogenous adenosine modulates activity-dependent inhibition of ADP amplitude, we evoked pairs of ADPs 9 s apart every 60 s and interposed a 25-spike conditioning train between the pairs of ADPs (Fig. 6C); this protocol elicits activity-dependent inhibition of the ADP, without altering mAHP amplitude (Brown & Bourque, 2004). CPT (10 μm) reduced mAHP amplitude (Fig. 6D) but did not alter activity-dependent ADP inhibition (Fig. 6E), indicating that endogenous adenosine does not contribute to activity-dependent inhibition of ADP amplitude evoked in this protocol.
Endogenous adenosine does not alter spike parameters
To determine whether CPT affects spikes, we measured spike amplitude and half-width, and fast AHP (fAHP) amplitude (Fig. 7A), as well as activity-dependent spike broadening (Fig. 7C) in data used to generate the mAHP and ADP (all n= 15); none of these parameters was altered by superfusion of 10 μm CPT (Fig. 7B and D).
Endogenous adenosine does not alter the slow AHP
To determine whether CPT affects the slow AHP (sAHP), we measured the amplitude of sAHPs that followed a 50-spike train (Fig. 8A); superfusion of 10 μm CPT did not alter peak sAHP amplitude (−0.4 ± 0.7 mV change; n= 4, P= 0.86, Wilcoxon signed rank test) or the amplitude of the sAHP measured between 1 and 2 s after the end of the spike train (−0.2 ± 0.5 mV change; n= 4, P= 0.86, Wilcoxon signed rank test; Fig. 8B), when potential confounding effects of the much faster mAHP would not be observed.
Discussion
Here, we used intracellular sharp electrode recordings from supraoptic nucleus neurones in hypothalamic explants to show that antagonism of A1 receptors reduced the amplitude of evoked mAHPs in these neurones and decreased spike frequency adaptation during spontaneous phasic bursts. Endogenous adenosine enhancement of the mAHP was not mediated by actions on the ADP because the amplitude of the ADP was not affected by CPT when the mAHP was reduced by apamin. In the presence of CsCl to block the ADP, CPT appeared marginally less effective at inhibiting the mAHP after lower frequency spike trains. CsCl also blocks the hyperpolarization-activated inward current (IH) and the leakage K+ current in supraoptic nucleus neurones (Ghamari-Langroudi & Bourque, 2001), which might account for the reduced effectiveness of CPT in the presence of CsCl.
Antagonism of A1 receptors also increased the duration of spontaneous phasic bursts and this was associated with increased post-spike excitability during bursts. Taken together, our results indicate that endogenous adenosine increases mAHP amplitude to enhance spike frequency adaptation and reduce the probability of spike firing during spontaneous phasic bursts in vasopressin neurones.
Generation of endogenous adenosine from somato-dendritic ATP release
As the effects of CPT on both spontaneous phasic spike discharge and the mAHP were activity dependent, the simplest explanation for the effects of CPT is that endogenous adenosine accumulates in an activity-dependent manner during burst firing. ATP and adenosine triphosphatase are contained within vasopressin neurosecretory vesicles (Poisner & Douglas, 1968) and so will be released with vasopressin into the supraoptic nucleus during somato-dendritic exocytosis of vasopressin (Ludwig, 1998; Ludwig & Leng, 2006). Thus the main source of extracellular adenosine might be the vasopressin neurones themselves, via a combination of adenosine secretion and the rapid catabolism of exocytosed ATP (Song & Sladek, 2005).
Somato-dendritic release of vasopressin is activity dependent (Brown et al. 2004) and capacitance measurements from isolated somata suggest that exocytosis can be evoked by a single spike (de Kock et al. 2003). Consistent with this observation, enhancement of the mAHP by endogenous adenosine was revealed by CPT after only the second spike of a 20-spike train in our current experiments (e.g. Fig. 4A and B), indicating that a single spike might be adequate to generate sufficient adenosine to enhance mAHP amplitude. However, in the presence of CsCl to block the ADP, greater numbers of spikes at higher frequencies were required to reveal the effect of CPT on the mAHP. As CsCl also blocks IH and the leakage K+ current (Ghamari-Langroudi & Bourque, 2001), it is possible that the effects of CPT at lower frequencies might result from interactions with these other targets of CsCl. Calculation of the rate of somato-dendritic secretion required to maintain an effective concentration of vasopressin within the hypothalamus in vivo indicates that (on average) each vasopressin neurone is required to release less than one vesicle every second under basal conditions (Brown et al. 2007), suggesting that high firing rates might be required to provoke an increase in somato-dendritic exocytosis. We have previously suggested that endogenous adenosine might be constitutively present in the extracellular space, but that its effects might not be exposed until after activity-dependent activation of the mAHP (Bull et al. 2006). The molar ratio of vasopressin to ATP is 20: 1 in vasopressin neurosecretory vesicles (Poisner & Douglas, 1968), which might be able to constitutively maintain an effective concentration of adenosine within the extracellular space of the supraoptic nucleus that requires spike discharge for its effects to be exposed. Alternatively, the more rapid effects of endogenous adenosine might result from kiss-and-run exocytotic events because these would not be expected to release vasopressin and dynorphin from the dense core vesicles but might release ATP, which could then be converted to adenosine. However, the adenosine triphosphatase within the neurosecretory vesicles would presumably require full exocytosis for release and so such a mechanism would require ambient adenosine triphosphatase in the extracellular environment.
Vasopressin neurones are not the only potential source of adenosine within the supraoptic nucleus. Noradrenaline (norepinephrine) triggers release of glial ATP to increase postsynaptic efficacy (Gordon et al. 2005) and dendritically released vasopressin facilitates noradrenaline release into the supraoptic nucleus (Ludwig et al. 2000). Hence, it is possible that somato-dendritic vasopressin release also increases the concentration of noradrenaline within the supraoptic nucleus, which in turn releases glial ATP that upon conversion to adenosine then activates A1 receptors on the vasopressin neurones to enhance mAHP amplitude. The effects of endogenous vasopressin on vasopressin neurones are constitutively present in vivo (Brown et al. 2004) and so neighbouring glia are likely to be continuously bathed in vasopressin. Hence, adenosine generated from glia would be expected to be constitutively present in the extracellular space, again requiring spike discharge for its effects to be exposed.
Implications of endogenous A1 receptor activation for spontaneous phasic activity
Phasic bursting in vasopressin neurones involves both extrinsic and intrinsic processes. Bursts are initiated by extrinsic inputs to vasopressin neurones, when summation of synaptic potentials causes membrane potential to cross the threshold for spike generation. Once firing is initiated, both extrinsic and intrinsic mechanisms are required to maintain further firing. When consecutive spikes occur close enough together, their associated non-synaptic ADPs summate to generate a persistent plateau potential that sustains further firing by bringing the membrane potential closer to threshold for spike initiation (Andrew & Dudek, 1983), which increases the probability that on-going synaptic potentials will reach threshold and generate further spikes (Brown & Bourque, 2006; Brown et al. 2006). During bursts, the fAHP increases spike discharge via activation of IH (Ghamari-Langroudi & Bourque, 2000), the mAHP induces spike frequency adaptation over the course of bursts (Kirkpatrick & Bourque, 1996; Greffrath et al. 2004) and the sAHP gradually decreases plateau potential amplitude (Greffrath et al. 1998; Ghamari-Langroudi & Bourque, 2004). In addition, activity-dependent inhibition of ADPs (Brown & Bourque, 2004) reduces the probability of spontaneous spikes firing as bursts progress to increase the probability of burst termination (Brown et al. 2006). Thus, in a spontaneous burst, the firing rate settles to a stable level that reflects a dynamic equilibrium between activity-dependent depolarizing mechanisms and hyperpolarizing influences.
Both the synaptic and non-synaptic mechanisms that generate phasic firing are modified by substances released by somata and dendrites of vasopressin neurones. Autocrine feedback by somato-dendritic vasopressin reduces vasopressin neurone firing rate during bursts (Ludwig & Leng, 1997); this vasopressin inhibition is evident from the onset of bursts (Brown et al. 2004), indicating that endogenous vasopressin constitutively inhibits phasic vasopressin neurones, probably by reducing the amplitude of EPSCs (Kombian et al. 2000) and by increasing IPSC frequency (Hermes et al. 2000). Nitric oxide is also generated by vasopressin neurones and inhibits firing (Liu et al. 1997; Srisawat et al. 2000), probably by increasing IPSC frequency and amplitude (Stern & Ludwig, 2001). During phasic bursts, ADPs are progressively inhibited by somato-dendritic dynorphin over tens of seconds to increase the likelihood of burst termination (Brown & Bourque, 2004; Brown et al. 2004, 2006). Here, we have shown that the autocrine somato-dendritic processes that generate phasic spike discharge in vasopressin neurones also include adenosine enhancement of the mAHP to increase spike frequency adaptation over the first few seconds of bursts. Hence, the activity-dependent inhibition of phasic firing via A1 receptors reaches a maximum over a much shorter time-course (several seconds) than activity-dependent inhibition by somato-dendritic dynorphin (several tens of seconds) (Brown et al. 2008).
The increase in burst duration induced by CPT is in marked contrast to the effects of complete blockade of the mAHP with apamin, which greatly increases firing rate, eliminates spike frequency adaptation and shortens bursts in vitro (Kirkpatrick & Bourque, 1996); the greatly increased firing rate in the presence of apamin might induce over-activation of other activity-dependent mechanisms, such as activation of the sAHP (Greffrath et al. 1998; Ghamari-Langroudi & Bourque, 2004) and inhibition of the ADP (Brown & Bourque, 2004) to shorten bursts. The more subtle inhibition of the mAHP by CPT (to cause a more modest increase in firing rate than apamin) might enhance the plateau potential, increasing the degree of ADP inhibition and sAHP activation required to terminate bursts.
The effects of endogenous adenosine are probably more complex than enhancement of the mAHP alone because endogenous adenosine also contributes to activity-dependent inhibition of the amplitude of evoked IPSCs and EPSCs (Oliet & Poulain, 1999). Hence, the more profound inhibitory effects of endogenous adenosine evident in vivo (Bull et al. 2006) probably reflect (at least) a reduced synaptic input strength combined with an enhanced mAHP amplitude.
Mechanisms of adenosine action
The intracellular mechanisms by which adenosine increases mAHP amplitude are unknown but might involve a reduction of calcium entry because A1 receptor activation reduces calcium currents and spike duration in supraoptic nucleus neurones (Noguchi & Yamashita, 2000; Ponzio & Hatton, 2005). However, we found no evidence that antagonism of endogenous activation of A1 receptors alters spike duration (or fAHP amplitude) and other calcium-dependent processes, such as activity-dependent spike broadening (Kirkpatrick & Bourque, 1991), were unaffected by CPT suggesting that endogenous adenosine probably does not alter global intracellular calcium concentrations. In vasopressin neurones, the mAHP is underpinned by an apamin-sensitive, calcium-activated small-conductance potassium current (Kirkpatrick & Bourque, 1996). A1 receptors can couple to Gi/o-proteins to reduce adenylyl cyclase activity as well as to Gq-proteins to activate Ca2+ release from intracellular stores; this latter effect is known to stimulate a variety of effector proteins, including calcium-activated potassium channels (Ralevic & Burnstock, 1998) and so might account for the enhancement of the mAHP by endogenous adenosine activation of A1 receptors.
Concluding remarks
Phasic spike discharge (periods of activity with marked spike frequency adaptation, separated by periods of silence) releases more vasopressin per spike than continuous activity, with the greatest secretion occurring early in bursts (Bicknell & Leng, 1981; Cazalis et al. 1985). Hence, spike frequency adaptation is important for efficient vasopressin release from the posterior pituitary gland. Spike frequency adaptation in vasopressin neurones is mediated by activation of the mAHP (Kirkpatrick & Bourque, 1996) and we show that mAHP amplitude is enhanced by endogenous activity-dependent activation of adenosine A1 receptors. We further show that this endogenous activity-dependent activation of adenosine A1 receptors increases spike frequency adaptation during spontaneous phasic bursts as well as reducing burst duration. Taken together, these observations suggest that, after conversion to adenosine, dendritic ATP release contributes to the termination of spontaneous phasic bursts in vivo by autocrine enhancement of mAHP amplitude to reduce the probability of synaptic potentials reaching spike threshold to trigger further spike firing as bursts progress.
Acknowledgments
This work was supported by a University of Otago Research Grant and the Otago School of Medical Sciences Bequest Fund.
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