Abstract
Developing neurons must regulate morphology, intrinsic excitability, and synaptogenesis to form neural circuits. When these processes go awry, disorders, including autism spectrum disorder (ASD) or epilepsy, may result. The phosphatase Pten is mutated in some patients having ASD and seizures, suggesting that its mutation disrupts neurological function in part through increasing neuronal activity. Supporting this idea, neuronal knock-out of Pten in mice can cause macrocephaly, behavioral changes similar to ASD, and seizures. However, the mechanisms through which excitability is enhanced following Pten depletion are unclear. Previous studies have separately shown that Pten-depleted neurons can drive seizures, receive elevated excitatory synaptic input, and have abnormal dendrites. We therefore tested the hypothesis that developing Pten-depleted neurons are hyperactive due to increased excitatory synaptogenesis using electrophysiology, calcium imaging, morphological analyses, and modeling. This was accomplished by coinjecting retroviruses to either “birthdate” or birthdate and knock-out Pten in granule neurons of the murine neonatal dentate gyrus. We found that Pten knock-out neurons, despite a rapid onset of hypertrophy, were more active in vivo. Pten knock-out neurons fired at more hyperpolarized membrane potentials, displayed greater peak spike rates, and were more sensitive to depolarizing synaptic input. The increased sensitivity of Pten knock-out neurons was due, in part, to a higher density of synapses located more proximal to the soma. We determined that increased synaptic drive was sufficient to drive hypertrophic Pten knock-out neurons beyond their altered action potential threshold. Thus, our work contributes a developmental mechanism for the increased activity of Pten-depleted neurons.
Introduction
The biology underlying the proper formation and function of neural circuits is of central interest in neuroscience. Genetic mutations found in patients with neurodevelopmental disorders give experimental inroads to, and highlight the clinical importance of, understanding these processes. Mutations in the dual-specificity lipid and protein phosphatase, Phosphatase and Tensin Homolog on Chromosome Ten (PTEN), exist in some patients having autism spectrum disorder (ASD) with macrocephaly (Goffin et al., 2001; Butler et al., 2005; Buxbaum et al., 2007; Orrico et al., 2009; Varga et al., 2009; McBride et al., 2010; Stein et al., 2010; Conti et al., 2012; Klein et al., 2013; Hobert et al., 2014). Pten normally functions to oppose the PI3K-Akt-mTor pathway by catalyzing the reverse reaction of PI3K: degrading phosphatidylinositol 3,4,5-trisphosphate to phosphatidylinositol (4,5)-biphosphate. Further, Pten likely has important scaffolding and protein-phosphatase roles in regulating neuronal cell biology. Through mechanisms not yet elucidated, ASD-associated point mutations are thought to lead to protein dysfunction in one or more of these cellular roles, ultimately causing pathological changes in neurophysiology.
Seizures and ASD are present in ∼30% of patients with either disorder (Tuchman et al., 2010), and PTEN mutations are documented in patients with epilepsy and ASD (Rudolph et al., 2011; Marchese et al., 2014). This suggests that loss of Pten protein function is sufficient to increase neuronal activity to pathological levels and that this increased neuronal activity may be etiological in the associated forms of ASD or epilepsy. Supporting this idea, Cre/Lox strategies in mice have been used to uncover how loss of Pten produces changes in neuronal form and function, but the varied developmental stages at which Pten has been depleted, and the variable times over which phenotypes have been studied, has produced seemingly conflicting data and interpretations regarding the relationship between morphological changes and physiology (Backman et al., 2001; Kwon et al., 2001, 2006; Ogawa et al., 2007; Zhou et al., 2009; Amiri et al., 2012; Sperow et al., 2012; Lugo et al., 2014). Consequently, the mechanisms connecting the loss of function of Pten to altered neuronal excitability have remained unresolved. Interestingly, it has been found that, when Pten is depleted from developing neurons, this results in increased excitatory afferent input (Luikart et al., 2011a; Xiong et al., 2012) and can lead to seizures (Amiri et al., 2012; Pun et al., 2012). Thus, we tested the hypothesis that loss of Pten function increases neuronal excitability through increased developmental excitatory synaptogenesis.
We coinjected retroviruses that encoded a fluorescent protein only with retroviruses that encoded a distinct fluorescent protein and Cre into the dentate gyrus of neonatal Pten-floxed mice. This allowed us to birthdate, label, and manipulate Pten in newborn granule neurons. By comparing Pten knock-out (KO) neurons to control (control) neurons of the same age within the same animal, we measured cell-autonomous changes caused by Pten KO. We found that increased developmental dendrite arborization and recruitment of excess excitatory inputs explain the increased synaptic drive underlying the excessive activity of Pten KO neurons.
Materials and Methods
Animals.
Procedures were approved by the Dartmouth Institutional Animal Care and Use Committee and conformed to federal, state, local, and Association for Assessment and Accreditation of Laboratory Animal Care standards. The animals used in these experiments were mice of either gender, supplied by The Jackson Laboratory. The two strains utilized were C57BL/6J (control) and B6.129S4-Pten<tm1hwu>/J homozygous (“Pten Floxed”) mice, which were also on the C57BL/6J genetic background, of either gender (Kwon et al., 2006; Luikart et al., 2008). Animals were on a 12 h light/dark cycle with chow and water provided ad libitum.
Surgery and slice preparation.
Under isoflurane anesthesia, 2 μl bilateral injections of replication-defective retroviruses based on pRubi were made into the dentate gyrus at postnatal day 7, at a rate of at 0.3 μl/min (Bayer and Altman, 1974; Luikart et al., 2011b). At varying days postinjection (DPI), animals were anesthetized by intraperitoneal injection of 2% tribromoethanol and were transcardially perfused for immunohistochemistry or for electrophysiology and multiphoton microscopy. Slices were generated at 7.5, 12.5, 16.5, 20.5, and 24.5 DPI (±1 d at each DPI) using published methods (Luikart et al., 2011a).
Replication-defective retroviruses.
Methods for production of replication-defective retroviruses based on pRubi have been previously published (Luikart et al., 2011b); briefly, viral particles expressed either a fluorescent reporter alone or both a fluorescent reporter and Cre recombinase via a T2A motif (Donnelly et al., 2001).
To generate pRubi-mCherry-T2A-Cre, we used PCR to amplify and add a 5′ BsrG1 and a 3′ EcoR1 site to Cre recombinase. The PCR product was then ligated into a cloning plasmid. Using annealed oligos with BsrG1-compatible overhangs and BsrG1 digestion, we introduced a T2A element upstream of Cre. The T2A-Cre was excised from the cloning plasmid and introduced into FUGW or FUCW via EcoR1 and BsrG1 digestion to create FUeGFP-T2A-Cre and FUmCherry-T2A-Cre, respectively. To generate retroviral constructs, SacII sites were used to excise a fragment encoding the ubiquitin promoter, fluorescent protein-T2A-Cre, and WRE elements from lentivirus plasmids, which were ligated into pRubi that had also been SacII digested.
To generate a retrovirus expressing the ultrasensitive calcium indicator GCaMP6s, we procured pGP-CMV-GCaMP6s (Addgene: pGP-CMV-GCaMP6s, Douglas Kim) (Chen et al., 2013), from which we amplified GCaMP6s, adding EcoR1 sites at each end by PCR. The amplification product was purified and ligated into a cloning plasmid. From pRubi, eGFP was excised by Xba1. Then, GCaMP6s was ligated into (pRubi minus eGFP) after both had been EcoR1 digested. All plasmids were confirmed by sequencing.
Immunohistochemistry.
Methods for eGFP, mCherry, Pten, and relative phosphorylated ribosomal S6 (p-S6) immunolabeling, and methods for neuronal soma size analysis, have been previously published (Fricano et al., 2014). For c-Fos measurements, rabbit polyclonal anti-c-Fos (Oncogene Science/Nuclea Diagnostics) was used; intensity measurement normalization was done as for p-S6. Antibodies against synaptobrevin 2 (1:1000, 104–211) and against Shank2 (1:400, 162–202) were from Synaptic Systems and were used on tissue that had undergone pH 6.0 sodium citrate heat-mediated antigen retrieval. Reconstructions were accomplished by manual tracing in Neurolucida (MBF Bioscience).
Electrophysiology.
The electrophysiological methods used here have been previously published (Luikart et al., 2011a; Rudolph et al., 2011). Tribromoethanol-anesthetized mice were perfused and hippocampal slices made in ice-cold solution containing the following (in mm): 110 choline-Cl, 10 d-glucose, 7 MgCl2, 2.5 KCl, 1.25 NaH2PO4 · 2H2O, 0.5 CaCl2, 1.3 Na-ascorbate, and 25 NaHCO3, bubbled with 95% O2-5% CO2. Slices were stored at room temperature, and recordings were performed at 37°C in aCSF as follows (in mm): 125 NaCl, 25 NaHCO3, 2.5 KCl, 1.25 NaH2PO4, 2.0 CaCl2, 1.0 MgCl2, and 25 d-glucose, bubbled with 95% O2-5% CO2. Intrinsic properties and current-clamp recordings were performed using a K-gluconate internal solution as follows (in mm): 115 K-gluconate, 10 HEPES, 2 EGTA, 20 KCl, 2 MgATP, 10 Na-phosphocreatine, and 0.3 Na3GTP. Synaptic currents were recorded using Cs-gluconate internal solution containing the following (in mm): 113 Cs gluconate, 10 HEPES, 10 EGTA, 17.5 CsCl, 8 NaCl, 2 MgATP, 0.3 NaGTP, 10 Na-phosphocreatine, pH 7.3, 295 mOsm. Recordings in strontium-containing extracellular solution replaced Ca using 2 mm Mg and 3 mm Sr. Series resistance was monitored before and after recordings; data were discarded if it increased by >10 mΩ. Recordings were sampled at 80 kHz (Multiclamp 700B; Molecular Devices). Action potentials were detected using a template (Axograph X) and reviewed manually. Spike threshold was defined as the membrane potential at which the first derivative of the voltage trace reached 10% of its peak. Analysis of spike amplitude, rise time, and half-width was performed on action potentials evoked by 500 ms current injection, which were temporally isolated by at least 20 ms from any other spikes in the train. For determination of the afterhyperpolarization, only the first spike was analyzed, and the temporal window was 20 ms. All other spike characteristics were measured by Axograph X. Asynchronous EPSCs (aEPSCs) were detected using template matching in Axograph X. The template rise time was 1 ms, decay time 6 ms, baseline 10 ms, length 30 ms, and had a threshold of 3. All captured events were then manually reviewed. The miniature EPSC (mEPSC) recordings were made in the presence of 1 μm TTX and 10 μm SR95531 (Gabazine), using the potassium gluconate internal solution and a holding current of −90 mV. For processing, mEPSC events were filtered at 2 Hz and the template kinetics were the same as used for aEPSCs.
Multiphoton microscopy.
Morphology of granule neuron dendritic protrusions/spines in the territory of the outer molecular layer was captured by multiphoton microscopy (Ultima In Vivo, Prairie Technologies/Bruker). Slices were superfused with aCSF bubbled with 95% O2, 5% CO2, at 37°C. Stimulation of fluorescence was at 920 nm using a Chameleon tunable laser (Coherent). Control neurons were those expressing only eGFP in non–Pten-floxed mice of the same genetic background (C57BL/6J, “wild-type”, control) or Pten-floxed mice; Pten KO neurons were those expressing eGFP-T2A-Cre in Pten-floxed mice.
Morphology measurements.
Image series were analyzed using ImageJ. After performing the “Smooth” function, a maximum intensity Z-projection was generated for each time point using the Group Z Projector plug-in. Small degrees of drift were corrected by the StackReg plug-in using the “Rigid Body” option.
A segmented line ROI was used to define dendrite length. ROI width was increased to encompass the dendrite shaft. From the area of the dendrite shaft ROI, dendrite width was calculated. For each apparent protrusion/spine, coordinates at the base of the protrusion were recorded. The number of protrusions divided by the length of the dendritic segment gave apparent protrusion density. For each protrusion, the Manual Tracking plug-in was used to plot coordinates of the spine tip at each time point. The length of each protrusion was approximated as the mean shortest distance between the coordinates of the protrusion base and the protrusion tip across each of the 10 time points of the imaging epoch.
Dendritic protrusions were classified by reviewers blinded to DPI and Pten status. Reviewers indicated type: thin/filopodial (longer than wide with no obvious head), stubby (wider than long with no obvious head), mushroom (discernibly wider head and thinner neck), or atypical (if it could not be clearly categorized as another morphological type). It was noted when a protrusion acquired a mushroom morphology over the imaging epoch. For these metrics, the count per dendritic segment was divided by the length of that dendritic segment to calculate the density. Densities were averaged between reviewers and used for final analyses.
Modeling.
Morphologies for control and Pten KO neurons were reconstructed into multicompartment models in Neurolucida and imported as multicompartment models into NEURON (version 7.3). Axial resistivity and specific membrane capacitance were set to 100 Ωcm and 1 μF/cm2, respectively. Increased surface areas in dendrites generated by protrusions were calculated from measurements for protrusion densities, protrusion lengths, and dendritic diameters observed in control and Pten KO neurons (Tables 3 and 4; data from 20.5 to 24.5 DPI) with protrusions assumed to have a mean diameter of 0.25 μm and with protrusion densities observed in Z-projections expected to detect 33% of the total protrusions along dendrites. Specific membrane capacitance and specific membrane conductance of dendritic compartments was then multiplied by the resulting “spine factor” (1.54 for control, 1.89 for Pten KO), and specific membrane resistivity was adjusted to replicate the experimentally determined mean RNs for 20.5 and 24.5 DPI control (RM = 17,850 Ωcm2; mean RN = 555 mΩ) and Pten KO (RM = 13,160 Ωcm2; mean RN = 143 mΩ) neurons. The leak conductance was set to reverse at −93 mV. Synaptic inputs were simulated as AMPA-like conductance changes having exponential rise (tau = 0.2 ms) and decay (tau = 2 ms), a maximum conductance of 350 pS (chosen to match mean aEPSC amplitudes in control neurons), and reversal potentials of 0 mV. Synapses were individually activated at 1 μm intervals along all dendritic segments, and responses were recorded with a simulated somatic single-electrode voltage clamp. All simulated synaptic responses in a given neuron were averaged to generate a mean EPSC, from which the population mean EPSC (± 2 SEM), was generated (see Fig. 9).
Statistics.
Toward ensuring that our studies had adequate statistical power, sample size was guided by our previously published research that used similar immunohistochemical and electrophysiological techniques (Luikart et al., 2011a; Fricano et al., 2014). Where absence of a statistically significant difference was biologically relevant to data interpretation, we explicitly analyzed power post hoc test using GraphPad StatMate 2.0. To compare Pten KO versus control neurons across time points, two-way ANOVA with Bonferroni's multiple-comparisons test was used. For electrophysiological studies comparing control versus Pten KO neuron responses to increasing levels of afferent stimulation or for immunohistochemical studies comparing control versus Pten KO neurons within the same animal, two-way repeated-measures ANOVA with Bonferroni's multiple-comparison test was used. Where control versus Pten KO neurons were compared at a single time point, Student's t tests were used with Welch's correction where appropriate.
Results
Retroviral Pten deletion causes hypertrophy and increases markers of activity in developing neurons
To investigate the development of Pten KO neurons, we generated retroviruses in which Cre was downstream of a fluorescent protein via a T2A motif (Donnelly et al., 2001). We then coinjected retroviruses encoding only a fluorescent protein with retroviruses encoding a distinct fluorescent protein-T2A-Cre, into the dentate gyrus of P7 Pten flx/flx animals (Lesche et al., 2002) (Fig. 1A). Immunohistochemistry confirmed that newborn neurons in Pten-floxed mice infected with retroviruses expressing eGFP only (control) retained Pten immunoreactivity, whereas neurons in the same animal infected with a retrovirus expressing mCherry-T2A-Cre lacked Pten immunoreactivity (Pten KO, Fig. 1B, yellow asterisks). To analyze the emergence of hypertrophy after Pten KO, we compared the soma size in control versus Pten KO neurons within individual animals at several time points (DPI). Soma size was greater in Pten KO neurons by 7.5 DPI and at every time point thereafter (Fig. 1C: effects, age, p < 0.0001; Pten KO, p < 0.0001; by two-way repeated measures ANOVA with Bonferroni's post test, two-way repeated-measures ANOVA, neurons from 16 animals). In contrast, in a control experiment, Cre expression in non–Pten-floxed (i.e., “wild-type”) C57BL/6J mice did not cause somatic hypertrophy (115.0 ± 2.7 vs 115.6 ± 1.4 μm2 in control versus Cre-expressing neurons from 3 animals, p = 0.806 by paired t test).
Having validated that our system allowed the longitudinal examination of developing Pten KO neurons, we examined whether Pten deletion resulted in increased neuronal activity in vivo. In addition to inducing hypertrophy, Pten KO increases expression of the activity marker p-S6 (Pun et al., 2012). Indeed, in our system, we found that immunoreactivity for p-S6 was elevated in Pten KO neurons versus controls (24.5 DPI; Fig. 1D). Immunoreactivity of p-S6 was elevated in Pten KO neurons (p < 0.0001), and this effect was significant at time points from 12.5 DPI onward (Fig. 1E; two-way repeated-measures ANOVA, neurons from 15 animals).
Although p-S6 is increased by activity, its levels are also increased in nonexcitable cells by Pten loss through disinhibition of the PI3K/AKT/mTOR/S6 kinase pathway; therefore, we examined levels of c-Fos, which also reports high levels of neuronal activity (Douglas et al., 1988; Knight et al., 2012). In Figure 1F, a Pten KO neuron (marked with **) is c-Fos-immunoreactive, whereas the control (marked *) is not (16.5 DPI). Compared with controls, overall c-Fos immunoreactivity in Pten KO neurons was significantly elevated (p = 0.0036), although for post hoc analyses of individual time points, this increase was significant only at 16.5 DPI (Fig. 1G; two-way repeated-measures ANOVA, neurons from 12 animals). Thus, expression levels of two activity markers provided evidence that developing Pten KO neurons were more active in vivo.
Developing Pten KO neurons have altered electrophysiological properties
Toward investigating the basis of increased activity in Pten KO cells, we tested how Pten altered the intrinsic properties of developing neurons. In whole-cell recordings, Pten KO was found to alter input resistance and membrane capacitance in response to a small voltage step (40 ms, 10 mV; holding potential −70 mV) (Fig. 2A). Capacitance increased with neuron age (p < 0.0001) but was higher in Pten KO cells (p < 0.0001), and this effect was significant at each DPI (Fig. 2B; two-way ANOVA, changes illustrated by Gaussian fit lines; 44 control, 37 KO neurons). We found that, whereas input resistance normally decreased with age (p < 0.0001), Pten KO further reduced input resistance (p < 0.0001), and this effect was significant at all DPIs (Fig. 2C; two-way ANOVA, Gaussian fit lines; 43 control, 39 KO neurons).
We tested the developmental impact of Pten KO on firing threshold by measuring the current necessary to evoke action potentials (“rheobase”; 10 ms current step). Pten KO cells required much more current injection to reach spike threshold than did controls (Fig. 2D). In both control and Pten KO neurons, rheobase increased as cells matured (p < 0.0001) but was even greater in Pten KO cells (p < 0.0001), and this effect was significant at DPI ≥ 12.5 (Fig. 2E; two-way ANOVA; 42 control, 39 KO neurons; Gaussian fit). We used current-clamp recordings to measure action potential threshold (Vm at 10% of the peak of the first derivative of the spike waveform). Newborn granule neurons fired at increasingly more hyperpolarized membrane potentials as they matured (p < 0.0001), but action potential threshold in Pten KO neurons was at yet more hyperpolarized membrane voltages than in controls (p < 0.0001), and this effect was significant by 24.5 DPI (Fig. 2F; two-way ANOVA; 42 control, 39 KO neurons; Gaussian fit). Thus, although much more current was required to elicit action potentials in Pten KO neurons, they were initiated at lower membrane potentials.
In addition to these single-spike studies, we examined the current necessary to evoke multiple action potentials. In response to longer (500 ms) current steps, multiple-spike rheobase in Pten KO neurons was greater than for controls (Fig. 2G). We found that, although the current required to generate the peak spike frequency for each neuron rose with age (p < 0.0001), it was even higher in Pten KO neurons (p < 0.0001), and this effect was significant at DPI ≥ 12.5 (Fig. 2H; two-way ANOVA; 32 control, 37 KO neurons; quadratic fit). Thus, as for single spike threshold, Pten KO cells required much greater current injection to reach peak firing rate. However, we also examined Pten KO neurons, which were more active in terms of their spike rate, independent of the current injection necessary to evoke that spiking. Peak spike rate normally rose with age (p < 0.0001), but this indicator of excitability was yet higher in Pten KO neurons (p < 0.0228) (two-way ANOVA; 32 control, 37 KO neurons; quadratic fit lines). Thus, although Pten KO neurons required greater current injection to fire, they fired at slightly more hyperpolarized membrane voltages and reached higher peak frequencies.
Having found that the firing rate of Pten KO cells was altered, we investigated whether the waveform of action potentials (as stimulated by the 500 ms current pulse) was also affected by Pten KO. Peak spike amplitude was found to rise with age (Tables 1 and 2; p = 0.0015), but spike amplitude was consistently greater in Pten KO neurons (Tables 1 and 2; p = 0.0009); likewise, whereas action potentials had more rapid rise times (10%–90%) with increasing developmental age (p = 0.0004), rise time was more rapid in Pten KO cells (p < 0.0001). Whereas action potential half-width normally decreased with developmental age (p < 0.0001), it was longer in Pten KO cells (p = 0.0193). The integral of the afterhyperpolarization (mV*ms) similarly decreased with developmental age of the neurons (p < 0.0001), but the afterhyperpolarization was diminished in Pten KO cells (p = 0.0193).
Pten KO increases sensitivity to afferent stimulation
Although intrinsic electrophysiological properties were altered by Pten KO, the increased activity of Pten KO neurons in vivo could also be due to altered responsiveness to synaptic drive. We therefore tested whether Pten KO caused developing granule neurons to be more active in response to stimulation of the presynaptic perforant path. In example traces (20.5 DPI; Fig. 3A), although the Pten KO neuron required much more direct current injection to reach threshold than did a control (as in Fig. 2), the Pten KO neuron fired more, and at lower intensities of perforant path stimulation than did the neighboring control cell. This suggested that Pten KO cells required more current to charge their larger membrane surface area but were nonetheless more sensitive to depolarizing synaptic input. With cells from 20.5 to 24.5 DPI, we found (as expected) for all cells spike probability rose with increased levels of afferent stimulation intensity (p < 0.0001), but that Pten KO cells exhibited higher spike probabilities than did controls (p = 0.0004), and this effect was significant at afferent stimulation intensities ≥0.150 mA (Fig. 3B; two-way repeated-measures ANOVA; 15 control, 12 KO neurons; cumulative Gaussian line).
Because our electrophysiology suggested that one mechanism increasing activity in Pten KO neurons was an increased sensitivity to depolarizing synaptic input, we used calcium imaging to confirm this finding. We generated a novel retrovirus expressing GCaMP6s (Chen et al., 2013) and coinjected this with our mCherry-T2A-Cre retrovirus to make a subset of GCaMP6s cells also Pten KOs (Fig. 3C). Using multiphoton microscopy, we distinguished controls expressing GCaMP6s only (*) from Pten KO cells expressing GCaMP6s and mCherry-T2A-Cre (**) (Fig. 3D; 20.5 DPI). At 20.5–24.5 DPI, using epifluorescence, we measured somatic GCaMP6s in control and Pten KO cells at 30 frames per second while stimulating the perforant path (3×, every 13 s: 1 ms pulses at 20 Hz for 500 ms). An image montage and associated plots of somatic intensity changes (Fig. 3E, top) demonstrate that Pten KO neurons had greater GCaMP6s transients for any given perforant path stimulation intensity than did controls (Fig. 3E, bottom). As with spike probability, background-corrected relative increases in GCaMP6s intensity (Peak ΔFReal/F0) (Chen et al., 2013) increased with stimulation intensity for all cells (p < 0.0001), but Pten KO further increased evoked Peak ΔFReal/F0 (p = 0.0263), and this effect was significant at stimulation intensities ≥0.200 mA (Fig. 3F; two-way repeated-measures ANOVA; 10 control, 11 KO neurons; quadratic curves). Thus, both calcium imaging and whole-cell recordings showed that Pten KO neurons fired more readily than did controls in response to equivalent afferent stimulation.
Developing Pten KO neurons have increased dendritic outgrowth and protrusions
Why were Pten KO neurons more responsive to afferent input, even though they required more inward current to fire? One possibility is that increased synaptogenesis in Pten KO neurons leads to greater synaptic drive. Using live multiphoton microscopy of Pten KO and control neurons in acute hippocampal slices, we quantified dendritic protrusions in the outer molecular layer, the territory of lateral perforant path inputs, between 12.5 and 24.5 DPI. Because rapid photobleaching of mCherry made it impractical for imaging protrusions, we visualized protrusions using eGFP. Control neurons (30, from 11 animals) were those expressing only eGFP in wild-type or Pten-floxed mice. Pten KO neurons (42, from 13 animals) were those expressing eGFP-T2A-Cre in Pten-floxed mice (Fig. 4A). During development, the density of dendritic protrusions increased (p = 0.0011), but Pten KO further increased protrusion density (p < 0.0001), and this effect was significant at each DPI (Fig. 4B; two-way ANOVA; 30 control, 42 KO neurons). We found that, in addition to being more numerous, the dendritic protrusions in these same cells had a greater mean length with Pten KO (p < 0.0001, two-way ANOVA; Table 3 and 4). Furthermore, although dendrite caliber normally increased with age (p = 0.0115), this too was increased further by Pten KO (p < 0.0001, two-way ANOVA; Table 3 and 4).
Having found that there was a higher density of protrusions per dendrite in Pten KO neurons, we next measured how Pten KO altered overall dendrite morphology using Neurolucida reconstructions of tissue from 20.5 to 24.5 DPI. Pten KO caused somatic hypertrophy and dendritic outgrowth (representative reconstructions; Fig. 4C; 8 neurons were reconstructed for control, 8 for Pten KO). Pten KO increased the number of primary dendrites originating from the soma (dendrites, p = 0.0008), the number of dendritic branching points (nodes, p < 0.0001), the number of distal dendrite branches (ends, p = 0.0002), the total dendritic length (p < 0.0001), the total dendrite surface area (p = 0.0001), and the total dendrite volume (p = 0.0016) (Fig. 4D; t tests; 8 control, 8 KO neurons). Thus, in addition to increasing the density of dendritic protrusions, Pten KO increased the total number and territory of primary dendrites.
The increases in total dendritic protrusions could contribute to Pten KO cell's increased sensitivity to synaptic input if the protrusions are functional synapses. We therefore performed immunohistochemistry on control neurons (expressing GFP only; pRubi) and on Pten KO neurons (expressing GFP and Cre; pRubi-GFP-T2A-Cre), both in Pten-floxed mice, at 24.5 DPI. Immunoreactivity for GFP defined infected neurons (α-GFP; Fig. 5A,C, left panels). Immunoreactivity for the glutamatergic postsynaptic density scaffolding protein, SH3 and multiple ankyrin repeat domains protein 2 (α-Shank2; Fig. 5A,C, second panels) was used to identify postsynaptic sites. Presynaptic sites were labeled using an antibody against the vesicle associated membrane protein, synaptobrevin 2 (α-SynB; Fig. 5A,C, third panels). Images were thresholded to the α-GFP signal, delimiting the dendrite and dendritic protrusions of the infected neurons. Using this region of interest, immunoreactivity for SynB and Shank2 could be colocalized to the infected neurons (Fig. 5B,D). Under these conditions, we could clearly detect both the presynaptic and postsynaptic markers either adjacent to, or colocalized at, the dendritic protrusions of both control and Pten KO neurons (mushroom-type spines; Fig. 5B,D, insets). These results suggested that the dendritic protrusions of both control and Pten KO neurons are functional synapses; we therefore investigated whether Pten KO neurons developed increased synaptic input.
Pten KO neurons have increased excitatory synaptic currents
More dendrites, greater surface area, and increased density of dendritic protrusions could be a physical substrate and, thus, the mechanism for, the increased sensitivity to afferent path stimulation of Pten KO neurons. We therefore compared evoked synaptic currents (5 stimulations, 1 every 13 s: 0.1 ms, 0.2 mA) in control versus Pten KO neurons. Mixed AMPA and GABAA postsynaptic currents were recorded at −90 mV. The contribution of AMPA-mediated excitatory currents was determined by subtracting the SR95531 (Gabazine, 10 μm)-sensitive GABAA, IPSC component (Fig. 6A). We found that Pten KO did not affect GABAA current amplitude (Fig. 6B; p = 0.419; two-way ANOVA; 24 control, 33 KO neurons). In contrast, Pten KO increased EPSC amplitude (Fig. 6C; p = 0.0003; two-way ANOVA; 24 control, 33 KO neurons). This suggested that Pten KO disproportionately increased synaptic excitation. Quantifying this, we found that, whereas the EPSC/IPSC amplitude ratio increased as neurons matured (p = 0.0043), Pten KO further increased the EPSC to IPSC amplitude ratio (p = 0.0018), and this effect was significant by 24.5 DPI (Fig. 6D; two-way ANOVA; 24 control, 33 KO neurons). Therefore, in developing Pten KO neurons, the excitatory postsynaptic responses were greater than they were in control cells.
We next determined whether the increased EPSC amplitude in Pten KO cells was due to a greater number of synaptic contacts or was due to stronger individual synapses. Replacement of extracellular calcium with strontium desynchronizes presynaptic vesicle release, generating aEPSCs that resemble quantal events (Bekkers and Clements, 1999; Rudolph et al., 2011). We did not find a significant difference in the degree to which the amplitude of the synchronous component of the evoked release was decreased after the addition of strontium-containing external solution. As in our previous experiments, in extracellular calcium, 20.4–24.5 DPI Pten KO neurons had larger evoked EPSCs (eEPSCs) than did controls (Fig. 6E, Ca2+ traces). These events were smaller and desynchronized in a calcium-free, strontium-containing solution (Fig. 6E, Sr2+ traces), and we were able to detect aEPSCs (Fig. 6F, arrowheads). Mean aEPSC amplitude was larger in Pten KO neurons (Fig. 6G, averaged traces; 6I, histogram), but their kinetic properties were similar to controls (peak-scaled, Fig. 6H), suggesting that the amount but not the type of depolarizing input was altered by Pten KO. As before, the aggregate eEPSC amplitudes in Pten KO neurons was much greater than in controls (∼4.532-fold, p = 0.0259; Fig. 6J; t test; 6 control, 6 KO neurons). In contrast, quantal-like aEPSC amplitude in these same neurons was only 1.343-fold greater in Pten KO neurons (p = 0.0209, Fig. 6K; t test; 6 control, 6 KO neurons). This suggested that the increased EPSC in Pten KO neurons was mostly due to an increased number of synaptic contacts onto Pten KO neurons and was modestly due to stronger individual synapses.
To quantify the increased synaptic drive, we estimated the number of quantal events (synaptic inputs) contributing to the evoked (0.2 mA stimulation) EPSC by dividing the amplitude of the eEPSC (in Ca2+) by the amplitude of the average aEPSCs (in Sr2+) for each neuron. We determined that there were, on average, 12.3 synaptic events per eESPC in controls, whereas there were 44.7 synaptic events per eEPSC in Pten KO neurons (3.63-fold increase, p = 0.0322; Fig. 6L; t test; 6 control, 6 KO neurons). If an increased release probability was principally responsible for the increased eEPSC, it might be expected that paired pulse ratio would be increased by a degree similar to the 3.63-fold increase in eEPSC. In post hoc analysis, we calculated that we had 99% power to detect as small as a 0.79-fold change by two-tailed t test using a significance level of 0.01. Therefore, the increased eEPSC amplitude was likely a cell-autonomous effect because: it paralleled changes in dendritic protrusion density, the presynaptic cell was not genetically manipulated, and the paired pulse ratio was not different between control and Pten KO neurons (p = 0.9193; Fig. 6M; t test; 6 control, 6 KO neurons).
The changes we observed with evoked currents strongly suggested an increase in the number and strength of excitatory synaptic inputs to Pten KO cells. To confirm this, we examined mEPSCs. Using control and Pten KO neurons from the 20.5–24.5 DPI range, cells were held at a potential of −90 mV in the presence of tetrodotoxin and SR-95531 (Gabazine). Spontaneous events were recorded using a potassium gluconate-based internal solution. Under these conditions, we could record quantal glutamatergic inputs as mEPSCs. The frequency and amplitude of individual mEPSCs were increased in Pten KO versus control cells (Fig. 7A, raw trace). The increased mEPSC amplitude was also evident in the average waveform of all mEPSCs recorded from Pten KO versus control neurons (Fig. 7B), although the kinetics were similar once peak scaled (Fig. 7C). Consistent with the increased number of dendritic protrusions and the greater number of aEPSCs per eEPSC, the frequency of mEPSC events was higher in Pten KO versus control cells (p = 0.0265; Fig. 7D; one-tailed t test; n = 9 control, 10 KO neurons). Absent a change in the paired pulse ratio (i.e., Fig. 6M), the increased mEPSC frequency provides further support to the interpretation that there are a greater number of synapses upon Pten KO cells (rather than an increased release probability at the same number of synapses). As with aEPSCs, the peak amplitude of mEPSCs was greater in Pten KO neurons than in controls (p = 0.0271; Fig. 7E; one-tailed t test; n = 9 control, 10 KO neurons). Although the kinetics of the peak-scaled mEPSC were visually similar between control and Pten KO neurons (i.e., Fig. 7B), quantification revealed a small but significantly increased mESPC rise time in Pten KO neurons versus controls (p = 0.0045; Fig. 7F; one-tailed t test; n = 9 control, 10 KO neurons). In contrast, the mEPSC decay time was not significantly increased in Pten KO cells (p = 0.1469; Fig. 7G; one-tailed t test; n = 9 control, 10 KO neurons).
Filopodia precede increased mushroom spine density in Pten KO neurons
Our data suggested that Pten KO cells were more active because they were more sensitive to afferent stimulation and that this increased sensitivity was due to an increase in the number of excitatory synapses Pten KO cells form. We therefore characterized synaptogenesis using live imaging in acute hippocampal slices. Dendritic protrusions in image series from the same neurons in Figure 4A, B were characterized as follows: thin/filopodial, stubby, mushroom, or atypical if not fitting another morphological category (example of classifications: Fig. 8A) (Peters and Kaiserman-Abramof, 1970; Arellano et al., 2007). The density of protrusions for each class was determined across development in control and Pten KO neurons.
We found that, whereas the density of thin/filopodial dendritic protrusions normally decreased with age (p = 0.0027), thin/filopodial density was markedly increased in Pten KO neurons (p < 0.0001), and this effect was significant at every DPI (Fig. 8B; Table 3 and 4; two-way ANOVA; 30 control neurons from 11 animals, 42 Pten KO neurons from 13 animals). Conversely, in these same neurons, although mushroom spine density normally increased with developmental age (p < 0.0001), it was even higher in Pten KO cells (p < 0.0001), and this effect was significant after >12.5 DPI (Fig. 8C; Table 3 and 4 two-way ANOVA). Therefore, a loss of Pten produces developmental increases in thin/filopodial dendritic protrusions that precede the increased density of mushroom spines seen later in Pten KO neurons. We also looked for potential changes in stubby and atypical spine densities: stubby spine densities did not differ with Pten KO (p = 0.0785, Table 3 and 4), although atypical spine densities were higher in Pten KO neurons (p = 0.0081, Table 3 and 4). Together, these morphological data suggest that Pten KO neurons form more mushroom (putatively functional) spines than controls, supporting the electrophysiological findings that indicated an increased number of glutamatergic synaptic sites.
Toward addressing why Pten KO neurons developed more spines, we quantified spine maturation as the frequency of instances in which a filopodial/thin protrusion became a mushroom spine. An example spine maturation is illustrated in Figure 8D wherein a filopodial/thin protrusion (distinguished by a yellow asterisk) adopts a mushroom shape. Because the 20 min session only rarely captured maturation events, we pooled data across DPIs. Spine maturations per a given length of dendrite occurred more frequently in Pten KO neurons (Fig. 8E; p = 0.0182, t test; 30 control, 42 KO neurons). However, because total filopodial protrusion density was also higher in Pten KO neurons (i.e., Fig. 8B), we tested whether the proportion of protrusions that matured differed with Pten KO. We found that the proportion of protrusions that matured was not different between control and Pten KO neurons (Fig. 8F; p = 0.731, t test; 30 control, 42 KO neurons). Post hoc analysis revealed that this experiment had 99% power to detect a proportional difference as small as ∼0.12 between control and Pten KO groups by two-tailed t test at a significance level of 0.01, which is >10-fold more discrete a change than the 1.363-fold increase in spine maturations in Pten KO neurons we observed (i.e., Fig. 8E). Thus, these data suggest that Pten KO neurons have an equivalent ability to stabilize synaptogenic contacts but do so more often because they have more filopodia, ultimately leading to more functional excitatory synapses.
Accounting for elevated excitatory synaptic input to Pten KO neurons
We sought to test whether the morphological changes we observed in Pten KO neurons not only accompanied, but could also explain, the increased excitatory drive they received. By 20.5–24.5 DPI, the eEPSCs in Pten KO neurons were 4.5 ± 1.1-fold that of controls (graphed as eEPSC measured, Fig. 9A; data: Fig. 6J). The increased aggregate eEPSCs could be due to increased dendrite length, spine density, and/or greater synaptic currents at each synapse. We therefore quantified the contribution of each of these changes. Using data from Figure 4D, Pten KO neurons had 1.9 ± 0.1-fold more dendritic length versus controls (graphed as total arbor length, Fig. 9A). Using data from the 20.5–24.5 DPI range of Figure 8C, Pten KO neurons had 1.6 ± 0.07-fold more mushroom spines than did controls (mushroom spine density, Fig. 9A). Last, using data from Figure 6K, aEPSC amplitude (approximating amplitude of quantal events) was 1.3 ± 0.1-fold more in Pten KO neurons (aEPSC amplitude, Fig. 9A). We used aEPSC data, rather than mEPSC data, in our models because, although essentially identical in this study, some evidence suggests postsynaptic responses to vesicles undergoing spontaneous versus evoked released differ (Bekkers and Clements, 1999). Furthermore, the evoked events may be more directly related to the increased glutamatergic input. Individually, none of these factors alone was sufficient to explain the enhanced synaptic drive that Pten KO neurons received. However, the product of the increases in arbor length, mushroom spine density, and aEPSC amplitude did yield the predicted enhancement of the eEPSC in Pten KO neurons: 4.1 ± 0.4-fold greater (eEPSC predicted, Fig. 9A). This predicted elevation of excitatory input was within the experimentally measured range (eEPSC measured, Fig. 9A). Therefore, these data suggest that both the altered dendrite morphology (length and density) and the increased aEPSC amplitude explained the enhanced excitatory drive to Pten KO cells.
We investigated whether the increased aEPSC amplitude in Pten KO cells may also have a morphological basis. We first reconstructed the morphologies of 8 control and 8 Pten KO neurons (i.e., data from Fig. 4C,D) as models in the NEURON simulation environment (Hines, 1989). For each neuron subtype, experimentally observed age- and Pten KO-dependent differences in dendritic protrusion density were modeled as reciprocal fold changes in dendritic Cm and Rm in dendrite compartments. Membrane resistivity (Rm) was adjusted so mean input resistance (RN) of the group matched the experimentally determined RN of that population. Simulated AMPA-like synaptic conductances (360 pS) were positioned at 1 μm intervals along dendrites and independently activated while recording the resultant somatic aEPSCs using simulated single-electrode somatic voltage-clamp (−93 mV). When identical synaptic conductances were generated in the simulated neurons, mean somatic aEPSC amplitudes were larger in Pten KO than in control cells (Fig. 9B; p = 0.027), and we found no difference between simulated and electrophysiological approaches (Fig. 9C; p = 0.297; two-way ANOVA; 6 control and 6 KO neurons measured, 8 modeled control and 8 KO neurons). Thus, our simulations could accurately predict the increased aEPSC amplitude found in Pten KO cells, and we could therefore investigate a potential morphological basis for this phenomenon.
Why were the somatic EPSCs, evoked by identical synaptic conductances, larger in Pten KO neurons even though they had lower specific membrane resistivity and had greater dendritic membrane capacitance and conductance? Because somatic capacitance has limited influence on synaptic responses recorded under somatic voltage clamp, the hypertrophy of Pten KO neuron somata was not a factor. However, as reported in Figure 4D, Pten KO neurons had more primary dendrites; therefore, a higher proportion of all simulated Pten KO synaptic compartments (i.e., dendritic locations at 1 μm intervals) were physically closer to the soma than they were in control cells (Fig. 9D; 1.2 ± 0.04-fold closer, p < 0.0001; two-way ANOVA; 8 control, 8 KO neurons). That is, aEPSCs were larger in Pten KO cells because synapses were located, on average, more proximal to the soma. By updating our predicted enchantment of the EPSC in Pten KO cells with this information (i.e., as in Fig. 9A), we determined that the relative contributions of these morphological changes (increased dendritic arbor length, mushroom spine density, and synapse proximity to soma) were sufficient to account for the majority (81%) of the enhanced excitatory synaptic responses observed in Pten KO neurons (Fig. 9E).
Collectively, we found that Pten KO neurons were more active in vivo, had altered intrinsic properties, and had morphological properties that accounted for their increased synaptic responsiveness. We therefore tested whether the altered morphological properties and electrophysiological changes induced by Pten KO could explain their increased firing. Using electrophysiological data from 20.5–24.5 DPI time points (Fig. 2), we found no difference in resting membrane potentials of control versus Pten KO neurons (Fig. 9F; VR; p = 0.229, t test; 23 control, 18 KO neurons). However, the membrane potential of Pten KO neurons was more hyperpolarized at action potential threshold (Fig. 9G; VAP; p = 0.0064, t test; 23 control, 18 KO neurons). Thus, it took less somatic voltage change to induce action potentials in Pten KO neurons (Fig. 9H; VR-VAP; p = 0.0325, t test; 23 control, 18 KO neurons). However, although less depolarization was needed to induce action potentials in Pten KO neurons, their morphological properties (i.e., much greater somatic capacitance) caused each synaptic conductance to produce a much smaller somatic depolarization (aEPSP). Indeed, mean simulated aEPSP amplitudes were 3× lower in Pten KO neurons (Fig. 9I; VaEPSP; p < 0.0001, t test; n = 8 control, 8 KO neurons). We therefore quantified the number of synaptic inputs that would be required to bring control versus Pten KO neurons to threshold from rest (assuming linear integration) (Krueppel et al., 2011) by dividing the difference between resting potential and spike threshold by the aEPSP amplitude. We determined that it would take more synaptic inputs to depolarize a Pten KO neuron from rest to threshold: for controls, ∼27 synaptic inputs would be necessary to reach threshold, whereas ∼68 inputs would be required for Pten KO neurons (a 2.54-fold increase; Fig. 9J; (VR-VAP)/VaEPSP; p < 0.0001, t test; 23 control, 18 KO neurons). Thus, action potential generation in Pten KO neurons requires the activation of more synapses than does action potential generation in control neurons.
We next determined whether the measured increase in the number of quantal events per evoked current would be sufficient to increase the firing of Pten KO neurons. We had found that there was a 3.63-fold increase in quantal-like aEPSCs per eEPSC in Pten KO cells (i.e., data from Fig. 6L, illustrated in Fig. 9K, aEPSC). This 3.63-fold increase in events per presynaptic stimulus was greater than the 2.54-fold increase in depolarizing events that our simulations predicted would be necessary for Pten KO cells to reach threshold (i.e., data from Fig. 9J, illustrated in Fig. 9K, threshold). The increase in evoked synaptic input was sufficient to overcome the increased number of synaptic events necessary to reach threshold (Fig. 9K; p = 0.0143; two-way ANOVA; 6 KO neurons: events per EPSC, 18 KO neurons: events to threshold). Thus, despite being hypertrophic, Pten KO neurons are more synaptically excitable than controls because of their increased dendritic territory, higher spine density, increased synapse proximity, and more hyperpolarized firing threshold.
Discussion
The phenotype from Pten KO varies depending on when Pten loss occurs. Constitutive Pten KO is lethal at E7.5 (Di Cristofano et al., 1998). Conditional Pten KO before neuronal differentiation (GFAP-Cre) causes neuronal hypertrophy and seizures in 7-week-old animals, with decreased survival rates after 14 weeks (Backman et al., 2001; Kwon et al., 2001). Inducible Pten KO in postnatal granule neuron progenitors (Gli1-CreERT2) causes seizures, neuronal hypertrophy, and increased dendritic arborization and spine density within 6 weeks (Pun et al., 2012). Pten KO soon after neuronal differentiation (Nse-Cre) also increases both dendritic arborization and spine density and produces seizures (Kwon et al., 2006). However, these changes develop after 8 months (Kwon et al., 2006). In contrast, Pten KO in mature neurons (CaMKII-Cre) does not cause hypertrophy of cell soma or increases in dendritic spine density and only subtly increases dendritic arborization without noted seizure generation (Chow et al., 2009; Sperow et al., 2012). Thus, the severity of somatic hypertrophy, increased spine density, and increased seizure susceptibility varies with the stage at which Pten is deleted. Perhaps because of these varied strategies, there has not been consensus on the mechanisms through which Pten loss alters neuronal physiology.
One consistent finding from previous research and this study is that Pten deletion from developing neurons alters both morphology and physiology. Isolated Pten KO neurons on glial micro-islands display somatic hypertrophy, dendrite overgrowth, and increased evoked EPSCs and mEPSCs (Weston et al., 2014). Pten KO in cortical neurons of young animals increases dendritic spine density, total dendritic length, and responsiveness to distant afferent neurons (Xiong et al., 2012). Furthermore, deletion of Pten from postnatally generated neurons in developing animals produces somatic hypertrophy, increased spine density, and increased net activity, as evidenced by the emergence of seizures (Pun et al., 2012). These findings demonstrate that loss of Pten during neuronal development causes morphological abnormalities and increased excitability. However, these previous studies did not completely address the mechanistic interrelation of these phenomena. In the present study, retroviral gene deletion coupled to precise electrophysiological and morphological measurements allowed us to study the progression of the Pten KO phenotype. We found that there is a tight structure–function relationship in these neurons and that the hyperexcitability of Pten KO neurons is chiefly explained by increased recruitment of excitatory synaptic inputs.
The hyperactivity of hypertrophic Pten KO neurons has been a paradox because large neurons need more current to reach threshold and would therefore be predicted to be less excitable. However, our data showing increased expression of activity markers in Pten KO cells, Pten KO mice developing seizures (Backman et al., 2001; Kwon et al., 2001; Ogawa et al., 2007; Ljungberg et al., 2009; Pun et al., 2012), and epilepsy in patients with PTEN mutations (Conti et al., 2012; Marchese et al., 2014), all strongly suggest that Pten KO neurons can be more active in vivo. While we found that Pten KO neurons required far more intracellular current injection to fire, they fired at lower intensities of afferent stimulation, indicating an increase in depolarizing synaptic drive upon Pten-depleted cells. Our voltage-clamp recordings demonstrated that the increased drive was due to an increase in the number and size of glutamatergic currents. Further, we show that the Pten KO neurons fire at decreased thresholds, have increased action potential amplitudes, decreased afterhyperpolarization, and fire at higher peak frequencies. Thus, we find intrinsic changes that contribute to the hyperactivity of Pten KO neurons as well as large increases in excitatory drive that overcome the increased current necessary to depolarize the larger neurons to firing threshold.
We found that increased synaptic depolarization of Pten KO neurons is due primarily to the increased number of excitatory synaptic sites. An imbalance of excitation to inhibition, as observed here, has been proposed to be a central etiology in neurodevelopmental disorders; and indeed, in animal models, direct alteration of this balance can produce symptoms reminiscent of ASD (Rubenstein and Merzenich, 2003; Yizhar et al., 2011). Mechanistically, we found that Pten KO increased dendritic filopodia density before the increased “mature” mushroom spine density. This finding supports the interpretation that filopodia participate in the formation of excitatory synapses (Fiala et al., 1998; Wierenga et al., 2008). Pten opposes trophic factors that otherwise signal through PI3K activation to increase neuronal filopodial motility and synaptogenesis (Luikart et al., 2008). Further, the phosphatidylinositol 3,4,5-trisphosphate that Pten degrades is critical for the accumulation and maintenance of postsynaptic density proteins and glutamate receptors at nascent spines (Arendt et al., 2010). Thus, the excess excitatory synaptogenesis described here by Pten KO may result from disinhibited synapse formation and/or increased stability of nascent synapses. This idea is supported by studies showing that Pten is an effector for some chemo-repellants (Chadborn et al., 2006; Oinuma et al., 2010; Perdigoto et al., 2011; Henle et al., 2013). An important question for future research is whether the excess synaptic contacts that Pten KO cells make represent an increased number of interactions with appropriate partners or interactions between neurons that would not normally be connected.
Almost all of the increased evoked excitatory current necessary for Pten KO neurons to fire could be accounted for by differences in dendritic architecture. Indeed, the increased total dendritic length, increased dendritic spine density, and increased amplitude of quantal-like aEPSCs (as for mEPSCs) accounted for the increased current necessary to initiate action potentials in Pten KO cells. Furthermore, modeling indicated that the increased aEPSC amplitude was also largely a function of dendritic architecture; the greater number of primary dendrites arising from neuronal soma effectively placed more synapses proximal to the soma in Pten KO cells. However, the amplitude of the recorded quantal events was 10.7% larger than that predicted by the model. Although this was within the calculated error of our measurements, it could also reflect a molecular change that would increase AMPA currents (i.e., more synaptic AMPA receptors). Additionally, we found a decrease in the voltage threshold of Pten KO neurons, which contributed to their increased excitability. In future studies, it could be investigated whether this is due to changes in the Pten-regulated expression or function of voltage-gated ion channels. Our data do not address the relationship of models of plasticity, such as LTP and LTD to morphological changes in Pten neurons (Wang et al., 2006; Fraser et al., 2008; Sperow et al., 2012; Takeuchi et al., 2013). However, our data do demonstrate that the basic physiological and morphological changes elicited by Pten KO are tightly coupled and are mechanistically involved in generating the increased excitability.
Footnotes
This work was supported by National Institutes of Health Grant 5 R01 MH097949 to B.W.L. and Grant 1 R01 MH099054 to A.T.G., Autism Speaks Pilot Grant 7359 to B.W.L., National Science Foundation Grant MRI 0922631 to A.T.G., and the Optical Cellular Imaging Shared Resource and the Norris Cotton Cancer Center at the Geisel School of Medicine at Dartmouth (5 P30 CA023108). We thank Jeonghoon Lee, Derek R. Racine, Grace B. Russo, and Paul W. Frazel for their contributions to data acquisition and analysis.
The authors declare no competing financial interests.
- Correspondence should be addressed to Dr. Bryan W. Luikart, Geisel School of Medicine at Dartmouth, Physiology and Neurobiology, 1 Medical Center Drive, Borwell 708E, Lebanon, NH 03745. Bryan.W.Luikart{at}Dartmouth.edu