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. 2019 Jun 24;9(1):9078.
doi: 10.1038/s41598-019-45011-7.

The logic behind neural control of breathing pattern

Affiliations

The logic behind neural control of breathing pattern

Alona Ben-Tal et al. Sci Rep. .

Abstract

The respiratory rhythm generator is spectacular in its ability to support a wide range of activities and adapt to changing environmental conditions, yet its operating mechanisms remain elusive. We show how selective control of inspiration and expiration times can be achieved in a new representation of the neural system (called a Boolean network). The new framework enables us to predict the behavior of neural networks based on properties of neurons, not their values. Hence, it reveals the logic behind the neural mechanisms that control the breathing pattern. Our network mimics many features seen in the respiratory network such as the transition from a 3-phase to 2-phase to 1-phase rhythm, providing novel insights and new testable predictions.

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Conflict of interest statement

The authors declare no competing interests.

Figures

Figure 1
Figure 1
Examples of Boolean networks and their characteristic response to an input signal C1. An action potential (spike) is represented by “1” and the time that passes between action potentials is signified by a sequence of zeros. Panel (A) shows a network where the memory (represented by S1,S2,···,Sk) is preserved after an action potential has been generated in X1. Panel (B) shows a network with self excitation (depicted by I1) where some of the memory is erased after a spike has been generated (the nodes S1,S2,···,Sm convey the memory that remains). Panel (C) shows the response of Network A and Panel (D) shows the response of Network B to changes in the period of C1. In both networks when the period of C1, p, is low (the spiking frequency is high), X1 exhibits tonic spiking with period 1 (i.e. X1=111···). When p=k/N+1 in Network A, p=m+2 in Network B, bursting appears (for example, X1=11100001110000···). When pk/(N1) in Network A, pk in Network B, X1 exhibits silence (i.e. X1=000···). The number of consecutive “1” within a burst is reduced in Network A as the period of C1 increases but stays constant in Network B (the only exceptions are when p=m+1 and p=k1 where we get different kinds of bursting, see Theorem 5). This characteristic response does not depend on the actual values of k (memory size), m (size of memory that was not erased) and N (threshold of X1 in Network A).
Figure 2
Figure 2
Schematic description of a larger network that provides better control of expiration and inspiration time. The Net A and Net B sub-networks are shown in Fig. 1, Panels (A and B) respectively. Here we only show the output and the first node to which the control input connects (S1i, where i is the sub-network number, this is equivalent to S1 in Fig. 1, see Figs S9, S10 and S11 for more details). This structure can be related to the schematic representation of the respiratory neural network hypothesized in Smith et al.. Sub-network X2, is deliberately missing from our diagram. Unlike Smith et al., we found that this sub-network is not essential for generating and controlling the bursting signal.
Figure 3
Figure 3
Transition from 3- to 2- to 1-phase pattern in the larger network (Fig. 2). In the 3-phase pattern, X1 is active during phase “I” (inspiration), X4 is active during phase “E1” (first phase of expiration) and X3 is active during phase “E2” (second phase of expiration). In the 2-phase pattern, X1 is active during inspiration, X3 is active during expiration and X4 is inactive. In the 1-phase pattern only X1 is bursting. We used the following parameters to generate this figure. For X1 and X3, k=400, N=2, m=100. For X4, k=800, N=3. The 3-phase pattern is shown here when the period of C1=5, the period of C3=110 and the period of C4=32. For the depicted 2-phase pattern, the period of C4 is increased to 1000. The 1-phase pattern is shown here when the period of C4=1000 (same as for the 2-phase pattern), the period of C3=500 and the period of C1=110.
Figure 4
Figure 4
Controlling inspiration and expiration times within the 3-phase pattern. The period of breathing and expiration time can be increased (keeping inspiration time constant) by increasing the period of C3 (RTN, Panel (B)). Expiration time can be decreased and inspiration time increase (keeping the period of breathing constant) by increasing the period of C4 (Pons, Panel (C)). The inverse effect (increasing expiration time and decreasing inspiration time while keeping the period of breathing constant) can be achieved by increasing the period of C1 (NTS, Panel (A)). This figure also shows that there is some variability in the timing of the bursting signals and that this variability increases when the periods of C1 and C4 increase. We used the following parameters to generate the figure. For X1 and X3, k=400, N=2, m=100. For X4, k=800, N=3. When it is not varied the period of C1=5, the period of C3=110 and the period of C4=32.
Figure 5
Figure 5
Controlling inspiration and expiration times within the 2-phase pattern. Increasing the period of C1 (NTS, Panel (A)) results in increasing expiration time (number of “0”) and decreasing inspiration time (number of “1”s) while keeping the period of breathing constant on average. Increasing the period of C3 (RTN, Panel (B)) increases the inspiration time (number of “1”s). The period of bursting is not shown in Panel (B) - its value increases as the period of C3 increases with the same increasing tendency as the inspiration time. The parameters used to generate this figure are as follows: for X1 and X3,k=400,N=2,m=100; for X4,k=800,N=3, and the period of C4=1000. In panel (A) the period of C3=110. In panel (B) the period of C1=5.
Figure 6
Figure 6
Other types of breathing patterns predicted by the model. Panel (A) shows periodic breathing - a dynamic change in inspiration time (marked by I) caused by an increase in the periods of C1, C3 and C4 (decrease in the spiking frequency of NTS, RTN and the Pons respectively). As a result, X3 (Aug-E) is silent and X4 (Post-I) is bursting. X1 (Pre-I) would have been bursting had it been in isolation. In Panel (B), the periodic breathing is suppressed by increasing the spiking frequency of NTS (decreasing the period of C1). This leads to another way by which a 2-phase pattern can be achieved. We used the following parameters to generate this figure. For X1 and X3, k=400, N=2, m=100. For X4, k=800, N=3. The period of C3=500 and the period of C4=350. The period of C1=110 in Panel (A) and the period of C1=50 in Panel (B).
Figure 7
Figure 7
Mechanism of the 3-phase pattern generation. X3 is in a bursting state due to the period of C3. While it is active both X1 and X4 are inactive. When X3 turns itself down (due to its bursting state), both X1 and X4 can be activated by their control signals C1 and C4 respectively. Due to the lower threshold of X1 and the higher frequency of its control signal, X1 is activated first. When X4 is activated, it terminates X1. When X3 becomes active again (due to its bursting state), X4 is terminated.
Figure 8
Figure 8
Creating a periodic signal: (a) C1=(10¯) (period 2); (b) C1=(100¯) (period 3); (c) C1=(1000¯) (period 4).

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