1 Fibril α-syn induced membrane currents, affected synaptic signaling and altered cellular excitability of neurotransmitter-defined neurons in sleep-controlling brain nuclei
We previously reported that fibril α-synuclein (α-synF) induced excitatory membrane responses in LDT and PPT neurons[30], and in accordance with those results, α-synF induced excitatory membrane responses in all of the LDT neurons examined (n = 10/10; Fig. 2). The average amplitude of the α-synF-induced inward current in LDT neurons was 7.3 ± 0.8 pA (n = 10). Moreover, we saw no statistical differences between the amplitudes of α-synF-elicited current in populations of neurotransmitter defined LDT cells (bNOS+/cholinergic: 7.6 ± 1.3 pA, n = 5; bNOS-/non-cholinergic: 8.3 ± 1.8 pA, n = 2; p = 0.8; Unpaired T-test; Fig. 2C1). Similarly, α-synF induced excitatory membrane responses in 100% of the recorded PPT neurons. The average amplitude of the α-synF –induced inward current in PPT neurons was 9.3 ± 1.9 pA (n = 8/8). We also found no significant differences between the current amplitudes between cholinergic and non-cholinergic PPT neurons (bNOS+: 9.8 ± 3.0 pA, n = 3; bNOS-: 8.5 ± 3.2 pA, n = 2; Fig. 2C2). When the current amplitude elicited by α-synF was compared between nuclei from all cells irrespective of phenotype, there wasn’t a significant difference (p = 0.4; Unpaired T-test).
Next, we analyzed whether α-synF had effects on synaptic activity in these two nuclei. Relative to baseline, α-synF induced a significant increase (8%) in the amplitude of the spontaneous excitatory postsynaptic currents (sEPSCs) in LDT neurons (control: 10.7 ± 2.1 pA; α-synF: 11.6 ± 2.1 pA; n = 4; p = 0.04; Paired T-test; Fig. 3), which was comparable to α-synF-mediated increases in sEPSC amplitudes in PPT neurons (8% increase from baseline; control: 11.3 ± 3.6 pA; α-synF: 12.2 ± 3.7 pA; n = 4; p = 0.02; Paired T-test). No significant changes were induced by α-synF in the frequency of sEPSCs within the LDT (control: 11.0 ± 3.8 Hz; α-synF: 12.8 ± 5.2 Hz, n = 4, p = 0.3; Paired T-test) or PPT (control: 8.4 ± 3.1 Hz; α-synF: 8.2 ± 2.8 Hz, n = 4, p = 0.5; Paired T-test).
The alterations induced by α-synF in membrane currents and synaptic activity of neurons in the LDT and PPT could result in modulation of neuronal excitability. Therefore, we examined directly whether this was the case and found that α-synF significantly increased the firing frequency of LDT neurons by 37.5% (control: 0.4 ± 0.1 Hz; α-synF: 0.55 ± 0.1 Hz; n = 3; p = 0.04; Paired T-test; Fig. 3C), and the firing frequency of PPT neurons was significantly increased by 39.5% (control: 0.43 ± 0.1 Hz; α-synF: 0.6 ± 0.1 Hz; n = 3; p = 0.03; Paired T-test).
2 Oligomeric α-syn induced effects on membrane currents, altered synaptic activity and heightened excitability in sleep-controlling nuclei.
The oligomeric form of α-syn (α-synO) also induced excitatory currents in the majority of recorded neurons in both the LDT (n = 7/7) and the PPT (n = 4/4). In contrast to what was seen for the fibril form in which there were no differences between the amplitudes elicited in LDT and PPT neurons, the amplitude of the current in PPT neurons induced by α-synO was significantly smaller than the amplitude induced by the same form of the protein in LDT neurons (LDT: 6.0 ± 1.5 pA; n = 4; PPT: 3.5 ± 1.2 pA; n = 4; p = 0.04; Unpaired T-test; Fig. 4). While recovery was low, the population of recorded cells included both cholinergic and non-cholinergic neurons, and there did not appear to be a difference between amplitudes across phenotypes within each nuclei (LDT bNOS+: 6.5 ± 4.9 pA, n = 2; bNOS-: 5.5 ± 2.1 pA, n = 2; p = 0.9; Unpaired T-test; PPT bNOS+: 3.7 ± 1.8 pA, n = 2; bNOS-: 5.0 pA, n = 1; data not shown).
Next, we examined whether α-synO affected synaptic activity in both nuclei. α-synO induced a 11.8% increase from baseline in the amplitude of sEPSCs in the LDT which was significant (control: 8.5 ± 1.1 pA; α-synO: 9.5 ± 1.0 pA; n = 3; p = 0.02; Paired T-test), as well as a 8.4% increase from baseline within the PPT that was significant (control: 10.3 ± 5.0 pA; α-synO: 11.1 ± 5.0pA; n = 3; p = 0.01; Paired T-test). No significant change in the frequency of sEPSCs was seen in the analyzed neurons within the LDT (control: 13.9 ± 1.7 Hz; α-synO: 13.0 ± 1.2 Hz p = 0.08; Paired T-test) or the PPT (control: 5.8 ± 1.8 Hz α-synO: 4.4 ± 0.8 Hz; p = 0.6; Paired T-test; Fig. 4).
We also investigated potential effects of α-synO on excitability in neurons within these two nuclei. In the LDT, α-synO induced an increase of 52% from baseline in the firing frequency which was significant (control: 0.63 ± 0.2 Hz; α-synO: 0.96 ± 0.3 Hz; n = 3; p = 0.03; Paired T-test). Similarly, a significant increase in the firing frequency of 50% over baseline was induced in PPT neurons (control: 0.82 ± 0.3 Hz; α-synO: 1.2 ± 0.4 Hz; n = 4; p = 0.03; Paired T-test). We found no significant differences between the relative change from baseline in the α-synO-induced firing frequency when comparing this effect between the two nuclei (p > 0.9; Unpaired T-test; Fig. 4).
3 Monomeric α-syn induced membrane currents, altered synaptic activity and heightened excitability in both sleep-controlling nuclei
In our previous report[30], we showed that the monomeric form of α-syn (α-synM) evoked an excitatory membrane response in all of the neurons examined in the LDT irrespective of phenotype (n = 35/35), which exhibited an average amplitude of 7.0 ± 2.7 pA (n = 35). In agreement with our earlier report[30], in this study, all tested PPT cells exhibited an excitatory membrane response which was also phenotype independent. While a greater average amplitude of current was elicited in PPT neurons (8.9 ± 2.5 pA, n = 9), this did not constitute a significant difference from the amplitude evoked in the LDT (p = 0.32; Unpaired T-test; Fig. 5).
Next, we determined effects of α-synM on sEPSCs and found that this form of the protein induced a significant increase of 18.7% over baseline in the amplitude of the sEPSCs in LDT neurons (control: 8.0 ± 0.8 pA; α-synM: 9.5 ± 0.9 pA; n = 6; p = 0.01; Paired T-test; Fig. 5). A significant sEPSCs amplitude increase of 16% was noted in PPT cells (control: 5.1 ± 0.5 pA; α-synM: 6.0 ± 0.5 pA; n = 4; p = 0.008; Paired T-test). In contrast to what was seen for the other forms of the protein, α-synM also induced a significant increase in the frequency of sEPSCs in the LDT (23.3%) (control: 6.0 ± 1.8pA; α-synM: 7.4 ± 2.2 pA; n = 6; p = 0.04; Paired T-test), which was not an effect we observed in the PPT (control: 5.0 ± 1.8 pA; α-synM: 4.5 ± 1.2 pA; n = 4 ; p = 0.2; Paired T-test; Fig. 5).
When we investigated excitability changes induced by α-synM, we found an increase of 15% in the firing frequency of LDT neurons, which was a significant change (control: 0.31 ± 0.03 Hz; α-synM: 0.36 ± 0.01 Hz; n = 4; p = 0.03; Paired T-test). In contrast, while the firing rate was relatively higher following α-synM, the increase was not significant in the examined PPT neurons (control: 1.2 ± 0.8 Hz; α-syn: 1.7 ± 1.3 Hz; n = 3; p = 0.35; Paired T-test; Fig. 5).
4 α-syn alters intracellular calcium in sleep-controlling nuclei
The neuronal effect induced by α-syn in its different structural conformations could impact intracellular calcium levels differentially, which could then substantially impact neuronal functioning. To investigate whether calcium is altered by α-syn in a structurally dependent manner, we applied α-synF, and α-synO, or α-synM and assessed changes in intracellular calcium levels using a fluorescent calcium indicator.
4.1 Fibril α-syn: Similar to findings in our previous study[30], α-synF elicited changes in intracellular calcium dynamics in the LDT and PPT neurons that were comparable for the two nuclei (Fig. 6). Within the LDT, 97% and in PPT, 93% of the cells responded to α-synF with changes in fluorescence indicative of changes in calcium (LDT: n = 60/62, PPT: n = 56/60; Fig. 6C). Responses elicited were categorized into two types: an increase or a decrease in fluorescence corresponding to increases or decreases in intracellular calcium, respectively. In both nuclei, α-synF elicited an increase in calcium in the majority of cells (LDT: 71.6%, n = 43/60; PPT: 60.7%, n = 34/56; Fig. 6C). The proportion of cells responding to α-synF was not significantly different in LDT and PPT (p = 0.5, Fisher’s exact test), and the proportion of responding cells exhibiting an increase in intracellular calcium did not differ between these two nuclei (p = 0.6; Fisher’s exact test).
4.2 Oligomeric α-syn: α-synO induced a change in fluorescence indicative of an alteration in intracellular calcium in 76.0% (n = 35/46) of the cells within the LDT, and in 92.0% of the cells within the PPT (n = 23/25). In both nuclei, the majority of cells responded with an increase in calcium (LDT: 82.8%, n = 29/35; PPT: 86.9%, n = 20/23; Fig. 6C). The proportion of examined cells responding to α-synO was not significantly different between the two sleep-related nuclei (p = 0.06; Fisher's exact test), and there were no nucleus-based differences in the proportion of directionality of the response (p = 0.9; Fisher's exact test). Taken together, this suggests that α-synO exerts similar effects on intracellular calcium in the LDT and PPT.
4.3 Monomeric α-syn: Similar to the effects of the other two α-syn conformations, α-synM exposure lead to alterations in intracellular calcium in the majority of cells in the sleep-controlling nuclei (LDT: 88.0%, n = 94/107; PPT: 83.0%, n = 45/54), which we had also observed in our previous study[30]. In both nuclei, the majority of responding cells exhibited increases in calcium (LDT: 64.3%, n = 60/94; PPT: 65.6%, n = 29/45; Fig. 6). There were no significant differences in the proportion of cells responding, or the proportion of responding cells which exhibited an increase or decrease in fluorescence between nuclei (p = 0.4; Fisher's exact test). Taken together, this suggests that the effects of the protein on intracellular calcium are similar in cells within LDT and PPT.
5 Effects on membrane currents, synaptic events, firing rate, and calcium levels in sleep-controlling nuclei are independent of the structural complexity of α-syn
Table 1
Comparison of the membrane current, EPSCs, firing rate and intracellular calcium changes induced by 3 different forms of -syn in sleep-controlling nuclei.
α
|
|
|
α-synF
|
α-synO
|
α-synM
|
pvalue
|
|
ΔIM
|
-7.3 ± 0.8
|
-6.0 ± 1.5
|
-7.0 ± 2.7
|
0.6
|
|
ΔsEPSCs -Amp
|
↑ 8.0%
|
↑ 11.8%
|
↑ 18.7%
|
0.4
|
LDT
|
ΔsEPSCs – Freq
|
↑16.3%
|
6.4%
|
↑ 23.3%
|
0.08
|
|
ΔAP – Freq
|
↑ 37.5%
|
↑ 52.0%
|
↑ 15.0%
|
0.2
|
|
ΔDF/F
|
97.0%
|
#76.0%
|
88.0%
|
0.004
|
|
Increase in DF/F
|
71.6%
|
82.8%
|
64.3%
|
0.2
|
|
ΔIM
|
-9.3 ± 1.9
|
-3.5 ± 1.2
|
-8.9 ± 2.5
|
0.2
|
|
ΔsEPSCs - Amp
|
↑ 8.0%
|
↑ 8.4%
|
↑ 16.0%
|
0.5
|
PPT
|
ΔsEPSCs – Freq
|
2.3%
|
24.0%
|
10.0%
|
0.5
|
|
ΔAP – Freq
|
↑ 39.5%
|
↑ 50%
|
↑41.6%
|
0.3
|
|
ΔDF/F
|
93.0%
|
92.0%
|
83.0%
|
0.2
|
|
Increase in DF/F
|
60.7%
|
86.9%
|
65.6%
|
0.1
|
IM: membrane current, α-syn: α-synuclein (M: monomers; F: fibril, O: oligomers), Amp: Amplitude, Freq: Frequency, AP: action potential; p value column calculated with either a one-way ANOVA or a Chi-square test. Significance in post hoc testing with the Fisher’s exact test is indicated by #.
5.1 LDT: All 3 conformations of α-syn depolarized the membrane of both cholinergic and non-cholinergic LDT neurons, and no significant differences between the current amplitudes were observed (Table 1). Similarly, there were no differences between the different structures when comparing the α-syn effect of increasing the amplitude of sEPSCs; however, only α-synM also enhanced the frequency of sEPSCs within the nucleus. An increase in firing frequency was induced by all 3 forms of α-syn. In the majority of LDT cells examined, the 3 conformations of α-syn induced changes in fluorescence indicative of alterations in intracellular calcium. However, in terms of frequency of response, some variation was found when comparing actions of α-synF, α-synO, and α-synM on alterations in calcium levels. A significantly greater proportion of examined LDT cells responded to α-synF when compared to the proportion responding to α-synO. However, the proportion of responding cells which exhibited an increase in intracellular calcium was not significantly different for these two protein forms, and the amplitude of the rise was not significantly different between all three proteins forms. When taken together, we conclude that overall alterations of membrane currents, synaptic events, excitability and increases in intracellular calcium were not structure dependent in neurons of the LDT as effects of α-synM, α-synO, α-synF on these parameters did not vary greatly.
5.2 PPT: Similar to actions seen in the LDT, we observed that the 3 conformations of α-syn altered the membrane current in 100% of the PPT neurons tested, and the amplitude of the evoked currents did not vary significantly when comparing α-synM, α-synO, or α-synF (Table 1). The α-syn-elicited increase of the amplitude of the sEPSCs did not vary significantly between the distinct protein structures, and none were found to enhance the frequency of sEPSC within this nucleus. The firing rate of PPT neurons was significantly altered by α-synO and α-synF. However, there were no significant differences in the proportion of cells responding with changes in intracellular calcium or in the proportion of responding cells exhibiting calcium increases following exposure to the 3 different protein forms.
When taken together, with the exception that α-synM did not induce changes in frequency of firing or EPSCs within the PPT, we conclude that findings in the PPT were similar to those seen in the LDT in that all three forms of α-syn altered membrane currents, synaptic events, excitability and intracellular calcium.
6 Mechanisms of action of α-syn M on membrane currents, synaptic transmission and calcium responses in sleep-controlling nuclei
6.1 Cell Death
In our earlier work, we were the first to report that α-synM has actions on membrane currents in mammalian neurons in ex vivo studies in the LDT and PPT. Further, we were the first to show that these actions, as well as rises in calcium, were associated with cell death, which we postulated were related. In the present study, we confirmed α-synM-mediated heightened cell death and extended our findings by showing that α-synF also leads to increased cell death by exposing one half of an LDT slice to control solution and the other half to either α-synF or α-synM and comparing cell death. When exposed to α-synF the proportion of cell death was 13 ± 8.1% over control (n = 5) in the LDT and when exposed to α-synM, 12 ± 3.6% cell death over control was detected (data not shown). There were no significant differences between the relative degree of cell death induced by α-synM and α-synF (p = 0.9; Unpaired T-test; data not shown). These results indicate that α-syn induced a toxic effect in a structure-independent manner. Calcium alterations have been shown to be induced by α-synM in hippocampal and cortical brain slices, however, these alterations did not result in toxicity in cultured neurons[34], which suggests that different mechanisms may be involved in α-synM-mediated effects across different nuclei. Therefore, we continued our investigations with a focus on examination of the mechanisms by which α-synM which is the form of α-syn that can alter to other conformations, affects the current of the membrane, synaptic transmission, and intracellular calcium in SD nuclei, and as these investigations were extensive, we focused on the LDT.
6.2 α-synM associates with the membrane of LDT neurons
We first ascertained whether α-synM was affecting LDT neuronal cell function by association with structures at the membrane surface or with internal structures suggestive of subcellular effect subsequent to internalization. Therefore, we used a recently developed and reported α-syn monoclonal antibody conjugated to Alexa Fluor 647 (α-syn/AF647) that allowed live-cell, particle tracking[40]. Using fluorescent imaging, we monitored the kinetics of movement and associations of the peptide within the slice once it entered the bath (Fig. 7). Baseline fluorescence was obtained by recording fluorescent intensity for 30s before bath perfusion of α-syn/AF647. We observed that within 1–2 min of entering the bath, α-syn/AF647 was located opposed to the membrane of cells. We verified that it remained stationary at the membrane during the subsequent 20 mins of recording (n = 3), suggesting that α-syn/AF647 was associated with structures at the surface of the membrane (Fig. 7A).
As α-syn/AF647 can be immobilized in brain slices by exposure to a crosslinking agent (paraformaldehyde) and retain its fluorescent properties, we performed immunohistochemistry on slices in which α-syn/AF647 had been fixated in order to identify bNOS + neurons and examine the relationship of α-syn/AF647 to neuronal phenotypes within the LDT. We observed that α-syn/AF647 was located at the surface of the membrane in 68% of the bNOS + cells (n = 23/28) and was not apparent near the remaining 32% of the bNOS + neurons (Fig. 7B). While it was not possible to visualize non-bNOS + cells, these data provide support for our hypothesis that the membrane of cholinergic sleep-controlling neurons within LDT is one target for α-synM actions.
6.3 Membrane perforations are not induced by α-synM
The live-cell imaging and fixed tissue fluorescence indicated an association with the membrane and raised the possibility that α-synM could be creating pores which could allow the passage of ions, including calcium across the cell membrane. This mechanism had been suggested previously when it was noted that the presence of 500 nM of α-synO in the pipette induced ruptures of the neuronal membrane following 20 min of exposure in primary cultures of rat hippocampal and dopaminergic neurons from the substantia nigra (SN)[42, 45, 46]. To examine this possibility, we conducted perforated patch recordings following well-established protocols[41] to detect the appearance of pores based on large changes in membrane resistance (Fig. 7C). In a control solution, a stable seal was formed between the membrane and maintained for over 40 min (resistance of the seal at 0min: 1.7 GOhms; at 40 min: 1.5 GOhms). In a separate population of cells, we added α-synM (500 nM) to the patch pipette solution and monitored whether changes in the seal resistance appeared, putatively due to membrane perforations. Results seen in control conditions were very similar to those obtained when α-synM was present in the pipette solution. A stable seal was obtained for over 40 min (resistance of the seal in 0 min: 1.5 ± 0.4 GOhms; 40min: 1.2 ± 0.2 G GOhms; p = 0.1; n = 3) suggesting no ruptures of the membrane under the pipette. Therefore, induction of inward current by α-synM does not appear reliant on pore formation in the membrane of native mouse LDT neurons.
6.4 α-synM induced depolarization of the membrane due to direct actions on LDT postsynaptic neurons
To further investigate where α-synM exerts effects on the LDT, we evaluated the actions of α-synM on membrane currents during action potential blockade via inhibition of voltage-dependent Na+ channels with TTX. Following determination that α-synM responses could be repeated within cells (p = 0.6; n = 3; Paired T-test), we found that following an initial application of α-synM that induced inward currents, inward currents were still seen upon a second application in presence of TTX (0.5 µM). There were no differences in the frequency of responses (control: 100%, TTX: 100%, n = 4) nor in the amplitude of the inward current when action potentials were blocked (control: 6.3 ± 1.7 pA; α-synM: 6.0 ± 1.7 pA; n = 3; p = 0.9; Paired T-test; Fig. 8A). Examination of current-voltage curves revealed a reversal potential of approximately − 55 mV (-55.3 ± 1.9 mV, n = 3; data not shown). These data indicate that the α-synM-induced change in membrane current involves a mixed cation current and does not require action potential generation in the slice, suggesting that effects are due to actions within the synapse, either at the presynaptic terminals or in the postsynaptic neuron.
6.5 α-syn M induced depolarization is not dependent on IP3-mediated intracellular calcium stores or Voltage-Operated Calcium Channels (VOCCs)
Intracellular calcium stores: In cell culture models, α-syno has been shown to activate SERCA pumps leading to alterations in intracellular calcium signaling[47]. In order to test a role for SERCA pumps, we blocked IP3-mediated intracellular calcium stores with CPA (10 µM). In the presence of CPA, α-synM elicited membrane currents in 100% of the cells which were tested (n = 5). In protocols in which the amplitude elicited by a first application of α-synM was compared in the same cells to that induced by a second application in presence of CPA, the average amplitude of the elicited inward currents did not significantly differ (control: 7.0 ± 1.1 pA; CPA: 6.6 ± 0.8 pA; n = 3; p = 0.5; Paired T-test).
VOCCs: The α-synM-induced membrane current could be carried, at least in part, by calcium, and since α-synM has been shown to activate VOCCs[48], we tested the role of VOCCs in this action by addition of Cd+ 2 (200µM), a non-specific blocker of VOCCs[49] to the external solution. When compared to control, the frequency of responses was not altered when the blocker was present (100% of cells tested; n = 8). Further, in repeated protocols in which first and second applications were applied to the same cells, the amplitude of inward current induced by the second application of α-synM in Cd+ 2 solution was not significantly reduced from that obtained from the first application but was instead significantly greater (control: 9.0 ± 0.5 pA; Cd+ 2: 11.6 ± 0.3 pA, p = 0.04; Paired T-test, n = 4). Therefore, we conclude that α-synM mediated inward currents were independent of the activation of SERCA pump-mediated calcium stores and VOCCs (Fig. 8B). When taken together with our TTX and current-voltage curves, we suggest that inward current responses induced by α-synM are not largely dependent on release from the presynaptic terminal, and involve a mixed cation conductance at the postsynaptic membrane.
6.6 Glutamate and Dopamine Receptor Involvement To investigate whether a membrane-bound receptor is involved in α-synM-induced inward currents, we next examined the effects of selective antagonists of receptor targets of α-syn previously reported in the literature.
Glutamate Receptor Mediated Transmission: As α-synM induced an increase of the amplitude of sEPSCs, this could be mediated by postsynaptic AMPA receptors. This supposition is supported by studies showing that α-synO modulates AMPA/NMDA receptor activation[50]. Therefore, we decided to examine the involvement of glutamatergic receptors in the α-synM-induced inward current. DNQX (15µM) and AP5 (50µM), antagonists of AMPA and NMDA receptors, respectively, were added to the external solution simultaneously. Under these conditions, α-synM induced inward currents in 100% of the neurons tested (n = 5). Moreover, in experiments in which it was possible to compare first and second applications, the amplitude of the currents elicited by α-synM during glutamate receptor antagonism did not differ significantly from the first application when the antagonists were absent (Control: 10.0 ± 4.0 pA; DNQX and AP5: 10.3 ± 14.8 pA; n = 3; p = 0.9; Paired T-test; Fig. 8B), suggesting that the α-synM-induced effect was not reliant on ionotropic glutamatergic signaling via AMPA or NMDA receptors.
Dopamine Receptor-mediated transmission: α-syn has been shown to enhance dopamine (DA)-mediated transmission by modulation of DA type 2 receptors (DR2)[51]. To test the hypothesis that α-synM-induced membrane current involved actions at dopamine receptors, we preincubated the slices with a cocktail of the DR2-like and DR1-like receptor antagonists, RAC and SCH-23390, respectively. In the presence of the DR1 and DR2 receptor antagonists, α-synM elicited membrane currents in 100% (n = 8) of the neurons tested. Further, in first and second application matched protocols, the average amplitude when the receptor antagonists were present did not differ significantly from the amplitude seen in the first application (amplitude control: 6.6 ± 1.1 pA; SCH23390 + RAC: 7.2 ± 1.0 pA; n = 7; p = 0.5; Paired T-test). Based on these data, we conclude that the current induced by α-synM was not dependent on activation of DR1-like or DR2-like receptors.
6.7 GPCR-mediated transmission
After exclusion of the most common α-synM membrane targets which have been presented in literature from other laboratories, we decided to examine whether a GPCR was involved in the mediation of the α-synM membrane effect. Therefore, we replaced GTP in the intracellular solution with GDPβS (250 µM), a membrane impermeable, nonspecific inhibitor of GPCR signaling. To ensure that this manipulation was effective in blocking GPCR-involved signaling, we monitored the effect of DA on the membrane, as all reported actions of DA at DA receptors are mediated by G-proteins[52]. In the presence of TTX, DA (30 µM) induced an outward current in a population of LDT neurons (n = 3; Fig. 8C). When GDPβS (250 µM) was included in the pipette, DA failed to induce any noticeable effect on the membrane current of LDT neurons (n = 3). Next, we examined the effects of α-synM on LDT neurons in presence of GDPβS, and we observed that α-synM (100 nM) failed to induce an inward current in 76% of the LDT neurons, which was a significant difference from control conditions (n = 10/13, p = 0.0001; Fisher’s exact test; Fig. 8C). The three cells which did respond with a change in membrane current in presence of GDPβS exhibited an amplitude of 4.8 ± 2.2 pA which was significantly less than in control conditions (n = 3; p = 0.02; Unpaired T-test). To further demonstrate that blockade of the responses was present, we reapplied α-synM to a subset of the same neurons, and α-synM still failed to induce a membrane response (n = 5/5). When combined, these results demonstrate that α-synM induced neuronal responses in the membrane of LDT neurons, which involved activation of GPCRs. While we were able to eliminate a role of many of the GPCRs shown in other studies to mediate actions of α-synM (as above), we were not able to identify the specific GPCR involved in α-synM-mediated inward currents in LDT neurons.
6.8 α-syn M enhance the amplitude and frequency of glutamate release from presynaptic excitatory synapses outside the terminal
Since α-synM increases the amplitude and frequency of sEPSCs in the postsynaptic neuron within the LDT, α-synM could be exerting an effect on presynaptic, excitatory synapses. Therefore, we investigated whether the changes in sEPSC frequency were dependent on action potential generation. When we applied α-synM in the presence of TTX, the frequency of miniature EPSCs (mEPSCs) following exposure to α-synM was not significantly different from baseline (control: 3.8 ± 1.3 Hz; α-synM: 3.5 ± 1.3 Hz; n = 5; p = 0.3; Paired T-test; data not shown). Further, α-synM did not significantly alter the amplitude of mEPSCs (control: 4.5 ± 0.7 pA; α-synM:4.6 ± 0.4 pA; n = 5; p = 0.8; Paired T-test; data not shown). These data suggest that α-synM has actions outside the terminal on excitatory, presynaptic inputs directed to the postsynaptic neuron leading to action potential-dependent alterations in glutamate release from presynaptic terminals. As these glutamatergic terminals could source from glutamate-containing cells in the LDT, these data support the conclusion that the population of bNOS- cells in which we observed α-synM-mediated membrane effects included local glutamate-containing LDT neurons. However, glutamatergic input also sources from projections directed to the LDT, therefore, the population of glutamate cells affected by α-synM remains to be determined.
7.0 α-synM induces calcium responses directly in postsynaptic neurons which involve G-protein mediated signaling
α-synM altered intracellular calcium levels. To further characterize the mechanism underlying α-synM effects on intracellular calcium, we evaluated whether effects of α-synM on calcium levels remained after blocking the generation of voltage-operated, Na+-dependent action potentials. To enable direct comparison, we wished to examine this in the same individual cells. Therefore, as a first step, we had to verify that the effects of α-synM on calcium were repeatable. We found that there were no significant differences between the probability of responses between a first and second application of α-synM to the same cells (p = 0.9). However, the amplitude of the change in fluorescence indicative of alteration in calcium (DF/F) elicited by the second application of α-synM was significantly reduced by 18% from that seen with first applications (1st app DF/F: 11.0 ± 1.0%; 2nd app DF/F: 9.0 ± 1.0%; n = 33; p = 0.0001). Therefore, we corrected for this reduction when a comparison was made for TTX absent vs TTX present, as well as for CPA absent vs CPA present conditions in the same cells.
The proportion of cells responding, as well as the proportion exhibiting an increase in DF/F, did not differ when TTX was present (Control: n = 23/23, TTX: n = 22/23, p = 0.9; Fisher’s exact test; Fig. 9). Further, the average amplitude of the increase did not significantly differ between TTX present or TTX absent conditions when a correction for the expected decrement was included (DF/F; Control: 9.0 ± 1.0%, TTX: 8.0 ± 1.0%; n = 22, p = 0.2; Paired T-test; Fig. 9). These data indicate that α-synM-elicited intracellular calcium rises do not require action potential generation, and further, that effects on calcium dynamics are likely due to actions at the synapse.
We investigated the source of calcium by inhibiting the SERCA pump-mediated calcium stores via inclusion of CPA in the external solution. The proportion of responding cells indicating intracellular calcium rises was not significantly different from that observed under CPA-absent conditions (DF/F increase: Control: n = 22/23, CPA: n = 23/23, p = 0.99; Fisher's exact test). The mean DF/F increase amplitude to α-synM in the presence of CPA was significantly higher than baseline (DF/F; Control: 7.0 ± 1.0%, CPA: 21.0 ± 1.0%; n = 22, p = 0.0001; Paired T-test; Fig. 9). When taken together, we conclude that rises in calcium induced by α-synM do not rely on intracellular IP3-mediated calcium stores.
7.1 α-synM induced membrane effect and calcium rise in single-cell via GPCR-mediated mechanism
Since we saw effects of α-synM on the membrane current and calcium levels in distinct populations of LDT cells, we wanted to confirm whether these two physiological phenomena occurred in the same cells. To that end, we conducted single-cell calcium imaging by injecting a cell-impermeant form of the calcium indicator dye, Fura 2, via the recording pipette, and concurrently monitored the current of the membrane following application of high concentration of α-synM (500 nM). In all cases, we observed that α-synM induced an inward current that was greater at this higher concentration than at 100 nM (127.5 ± 12.5pA, n = 6) [30], and the membrane current was accompanied by an increase in fluorescence indicative of rises in intracellular calcium levels in the individual neurons (36.8 ± 10.4%DF/F, n = 6). These findings indicate the likelihood of a common underlying mechanism mediating calcium and membrane responses to α-synM. Therefore, we examined the α-synM-mediated rise of calcium in presence of GDPβS. Relative to baseline, α-synM (500 nM) induced an increase in intracellular calcium which was 50% lower in amplitude than under baseline conditions (18.7 ± 6.4%DF/F, n = 7, p = 0.04, Unpaired T-test; Fig. 9). These results demonstrate that α-synM induces intracellular calcium increases within LDT neurons that involve GPCR-mediated signaling. As the rise in calcium was not eliminated, this suggests that additional mechanisms could be involved, or blockade of GPCR-mediated mechanisms was not complete.