Heterogeneous organization of the locus coeruleus projections to prefrontal and motor cortices - PubMed (original) (raw)

Heterogeneous organization of the locus coeruleus projections to prefrontal and motor cortices

Daniel J Chandler et al. Proc Natl Acad Sci U S A. 2014.

Abstract

The brainstem nucleus locus coeruleus (LC) is the primary source of norepinephrine (NE) to the mammalian neocortex. It is believed to operate as a homogeneous syncytium of transmitter-specific cells that regulate brain function and behavior via an extensive network of axonal projections and global transmitter-mediated modulatory influences on a diverse assembly of neural targets within the CNS. The data presented here challenge this longstanding notion and argue instead for segregated operation of the LC-NE system with respect to the functions of the circuits within its efferent domain. Anatomical, molecular, and electrophysiological approaches were used in conjunction with a rat model to show that LC cells innervating discrete cortical regions are biochemically and electrophysiologically distinct from one another so as to elicit greater release of norepinephrine in prefrontal versus motor cortex. These findings challenge the consensus view of LC as a relatively homogeneous modulator of forebrain activity and have important implications for understanding the impact of the system on the generation and maintenance of adaptive and maladaptive behaviors.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Fig. 1.

Fig. 1.

LC cells innervating M1 are distinct from those innervating OFC, mPFC, and ACC. (A_–_C) Representative photomicrographs of pairs of injection sites (Left) and LC through merged fluorescence filters to detect retrograde tracers (second from Left) and DBH immunofluorescence (third from Left) following injections into OFC and M1 (A), mPFC and M1 (B), and ACC and M1 (C). Arrowheads and Roman numerals indicate the locations of cells shown in high power images in the Right panels. Columns show individual neuron(s) through fluorescein (OFC, mPFC, or ACC), rhodamine (M1), and merged fluorescence filters, thus identifying single labeled cells with different terminal fields. (_A_′–_C_′) Histograms show mean cell counts per animal ± SEM projecting to each possible combination of terminal fields (n = 5 rats per experiment).

Fig. 2.

Fig. 2.

LC cells projecting to OFC and mPFC contain enriched mRNA transcripts coding for markers of excitability and release. Mean ± SEM of relative quantities of mRNAs that were shown to differ significantly from M1 projection cells according to terminal field by a Kruskal–Wallis H test (*P < 0.05). DBH is shown in the far right as a representation of protein whose mRNA expression was highly consistent between populations.

Fig. 3.

Fig. 3.

EPSC size and frequency vary according to LC neuronal terminal field. Representative traces of AMPA-mediated sEPSCs, mEPSCs, and NMDA-mediated sEPSCs are shown in A, D, and G. Mean frequencies and amplitudes of these events are shown in B, E, and H, and C, F, and I, respectively. Cells projecting to mPFC were characterized by significantly larger AMPA-mediated sEPSCs and more frequent mEPSCs than those projecting to M1, and cells projecting to OFC were characterized by significantly larger NMDA-mediated sEPSCs than M1 projection cells. Values were generated by using an automated search protocol in ClampFit software to identify all sEPSC events recorded from each cell and calculate a single mean sEPSC size for each cell. Any event smaller than twice the SD of the baseline of the recording was discarded. These data were then used to generate mean ± SEM amplitude values on a cell by cell basis. *Significantly different from M1 projection cells (P < 0.05).

Fig. 4.

Fig. 4.

LC cells projecting to mPFC are more spontaneously active and have a smaller AHP than those projecting to M1. (A) Representative traces of individual action potentials from an mPFC and M1 projection cell showing the magnitude of afterhyperpolarization as measured from action potential threshold to its most hyperpolarized state (dashed lines and arrows). Mean ± SEM afterhyperpolarization amplitudes are shown in B. (C) Representative traces of spontaneous action potentials from all populations of LC projection cells (OFC, n = 18; mPFC, n = 19; ACC, n = 18; M1, n = 17). Mean ± SEM of spontaneous discharge values are shown in D. *Significantly different from M1 projection cells (P < 0.05).

Fig. 5.

Fig. 5.

LC cells projecting to mPFC are more excitable than those projecting to M1. (A) Patched cells were injected with a −0.1-nA current step to measure input resistance, followed by a series of progressively increasing current steps (−3.0 to +4.0 nA, 0.5-nA interval). Representative traces of discharge in response to a 1-s injection of 4.0 nA are shown in B. Action potentials were truncated 5 mV above firing threshold. (C) Input resistance was significantly greater in cells projecting to OFC and ACC than M1. (Inset) The responses to the current injection from representative traces shown in B superimposed on one another. Note that the larger deflections in voltage are from ACC and OFC projection cells whereas the smaller two are from M1 and mPFC projection cells (P < 0.05). A plot of the mean ± SEM of the number of action potentials fired in response to all levels of current injected into each of the populations of LC neurons is shown in D. *Significantly different from M1 projection cells (P < 0.05).

Fig. 6.

Fig. 6.

Cells projecting to PFC and M1 segregate from one another in principal-component space. Principal-component analysis was used to construct composite variables from several current-clamp parameters measured independently. Regression scores were calculated in IBM SPSS Statistics version 20. Scores for PC1 versus PC2 are plotted for all cells in all groups. Note that cells projecting to OFC and ACC differ from M1 projection cells primarily in PC2 (membrane properties) whereas cells projecting to mPFC differ mostly from cells projecting to M1 in PC1 (action potential properties). Individual weights of each of the current-clamp measures to each principal component are shown in

Table S6

. The quality of cluster separation was evaluated using the Davies–Bouldin index (45). Computations were performed in the R language (46) using the clusterSim package according to Walesiak and Dudek (47), with cluster dispersion assessed as the SD of distances from points to the cluster centroid, and separation between clusters assessed as the Euclidean distance. Davies–Bouldin index values for comparisons between M1 and OFC, mPFC, and ACC were 1.47, 1.13, and 1.40, respectively.

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