Appendix 1. Haldane relation
Here we will see an elementary derivation of the Haldane relation. Enzymes help chemical reactions proceed under conditions of microscopic reversibility (Onsager 1931). A kinetic model that violates this thermodynamic principle would be able to generate chemical work without an adequate source of energy.
Haldane (1930) seems to be the first scientist to publish the kinetic equation for a reversible enzymatic chemical reaction,
\(S\,\,\,\overset {} \rightleftharpoons \,\,\,P.\)
In cellular environments, this reaction cannot usually proceed without the presence of an enzyme (same letters are used to designate chemical species concentrations). The enzyme E creates an intermediate complex X.
\(E + S\,\,\underset{{k_{ - 1} }}{\overset{{k_{1} }}{\rightleftharpoons}}\,\,\,X\,\,\,\underset{{k_{ - 2} }}{\overset{{k_{2} }}{\rightleftharpoons}}\,\,\,E + P,\)
where \(k_{i\,} {\text{and}}\,k_{ - i} ,i = 1,2\) are the forward and backward kinetic constants. In an experimental closed system, this reaction ends at equilibrium. In open cellular environments, the substrate is injected– usually as a product of other reactions–and the product P joins in other parallel reaction paths, thus making the whole process practically irreversible.
This equation from Haldane (1930) was derived assuming the steady state of complex X. The rate v of product changes (\(v = {\text{d}}P/{\text{d}}t\)) is written as
$$v = \frac{{k_{1\,} k_{2\,} S\, - \,k_{ - 1\,} k_{ - 2} \,P}}{{k_{ - 1} + k_{2} + k_{1} \,S + k_{ - 2} \,P}}\,\,E_{{{\text{T}}\,}} = \frac{{V_{1} \left( {S/K_{1} } \right) - V_{2} \left( {P/K_{2} } \right)}}{{1 + \left( {S/K_{1} } \right) + \left( {P/K_{2} } \right)}}.$$
with \(V_{1} = k_{2} E_{T} S\), \(V_{2} = k_{ - 1} E_{T} P\), \(K_{1} = \left( {k_{ - 1} + k_{2} } \right)/k_{1}\) and \(K_{2} = \left( {k_{ - 1} + k_{2} } \right)/k_{ - 2}\).
The total concentration of enzyme is \(E_{{{\text{T}}\,}}\) and S, and P are the concentrations of substrate and product. At equilibrium, v = 0, and the kinetic constants obey microscopic reversibility,
\(K_{{{\text{eq}}}} = \left( {\tfrac{P}{S}} \right)_{{{\text{eq}}}} = \frac{{k_{1\,\,\,\,} k_{2} }}{{k_{ - 1\,} k_{ - 2} }}\), and consequently, we have \(K_{{{\text{eq}}}} = \frac{{V_{1} \,K_{2} }}{{V_{2} \,K_{1} }}\).
This last beautiful expression is known as the "Haldane relation," and it is a strong argument to show the thermodynamic consistency of enzymatic catalysis.
Note that K1 and K2 can be expressed in terms of the association constants KS and KP, on which the recognition of ligands S and P by the receptor sites depends. The respective equations are:
$$K_{1} = \frac{{k_{ - 1} + k_{2} }}{{k_{1} }} = \frac{1}{{K_{{\text{S}}} }} + \frac{{k_{2} }}{{k_{1} }},$$
$$K_{2} = \frac{{k_{ - 1} + k_{2} }}{{k_{ - 2} }} = \frac{1}{{K_{P} }} + \frac{{k_{ - 1} }}{{k_{ - 2} }}.$$
Very far from equilibrium, \(S \gg P\), rate v becomes the classical Michaelis–Menten equation,
$$v \approx V_{1\,} \,S/\left( {K_{1} + S} \right).$$
Appendix 2. Survival modes
Here we want to discuss an interesting point related to the physical effects of the presence of the iCat. Let us imagine that the emission energy of the light signal is in both situations \(\varepsilon_{{\text{E}}}\). Suppose that formatting the emission of that light to transfer the information in Morse requires an additional energy \(\varepsilon_{{\text{F}}}\). Finally suppose that the prisoner's decoding the Morse code has consumed an energy \(\varepsilon_{{\text{L}}}\). Then, the conditions associated with the code that allow the prisoner to open the combination box, access the food and save his life have a total energy cost \(\varepsilon_{{\text{T}}}\) given by
$$\varepsilon_{{\text{T}}} = \varepsilon_{{\text{E}}} + \varepsilon_{{\text{F}}} + \varepsilon_{{\text{L}}} .$$
Let us now expand the experiment to Q isolated prisoners, trapped in their cells and released at age \(m_{i}\), i = 1, …, Q. Suppose everyone knows Morse code, gets saved and continues their lives. If these i individuals live a total of \(n_{i}\) years, each one of them will carry out a total consumption of free energy given by
$$F_{i} \left( {m,n} \right) = \int\limits_{{m_{i} }}^{{n_{i} }} {W_{i} (a)\,{\text{d}}a} ,$$
where \(W_{i} (a)\) is the instantaneous power expressed in units of age. It is expected that in general for each pair of individuals j, k, it will be \(F_{j} (m,n) \ne F_{k} (m,n)\). This implies that the information associated with a relatively small amount of energy, \(\varepsilon_{T}\), generates different amounts of dissipation of free energy \(F\left( {m,n} \right)\). It is also expected to be \(F(m,n) \gg \varepsilon_{{\text{T}}}\) and that both amounts are not correlated.
Appendix 3. Toward a formal representation of Information Catalysis
The information catalyst iCat is built from two systems of pattern recognition, the operators \(\Im_{{{\text{input}}}}\) and \(\Im_{{{\text{output}}}}\). As we previously pointed out, the semantic information processed by an iCat is located (or, we could also consider, "defined") in the structure of its filters \(\Im_{{{\text{input}}}}\) and \(\Im_{{{\text{output}}}}\).
Let us start by describing the way these iCats work. In a transition between an initial state \(Y_{ \downarrow }^{{({\text{in}})}}\) and a final state \(Z_{ \uparrow }^{{({\text{fin}})}}\)(represented by \(Y_{ \downarrow }^{{({\text{in}})}} \mathop{\longrightarrow}\limits^{{}}Z_{ \uparrow }^{{({\text{fin}})}}\)) with very low probability \(p_{0}^{{({\text{in,fin}})}} \approx 0\) of occurrence, a catalyst iCat guides the same transformation \(Y_{ \downarrow }^{{\text{(in)}}} \mathop{\longrightarrow}\limits^{{{\text{iCat}}}}Z_{ \uparrow }^{{({\text{fin}})}}\), with a transition probability \(p_{{{\text{iCat}}}}^{{({\text{in,fin}})}} \gg p_{0}^{{({\text{in,fin}})}}\). The subscripts \(\downarrow\) and \(\uparrow\) mean non-filtered and filtered, respectively. After the transition is completed, the catalyst recovers its ability to initiate a new cycle. It is important to remark that iCat, instead of enhancing rates as it happens in chemical catalysis, drastically increase the probabilities of occurrences of the involved events.
The states Y and Z have a very variable inner structure depending on the patterns involved. We can assume the following symbolic representation of the action of the filters of iCat:
$$Y_{ \downarrow }^{{{\text{(in}})}} \mathop{\longrightarrow}\limits^{{\Im_{{{\text{input}}}} }}Y_{ \uparrow }^{{({\text{in}})}} \,{\text{and}}\,Z_{ \downarrow }^{{({\text{fin}})}} \mathop{\longrightarrow}\limits^{{\Im_{{{\text{output}}}} }}Z_{ \uparrow }^{{({\text{fin}})}}$$
Consequently, a large set of potential states \(Y_{ \downarrow }^{{({\text{in}})}}\) is filtered to a selected subset of actual states \(Y_{ \uparrow }^{{{\text{(in}})}}\) (e.g., the selection of a particular ordered set of substrates of an enzyme form the large set of potential substrates), and a large set of potential states \(Z_{ \downarrow }^{{({\text{fin}})}}\) is filtered to a selected subset \(Z_{ \uparrow }^{{({\text{fin}})}}\) that gives the final outcome (e.g., for the case of an enzyme, and the filter reduced the set of potential products to a set of actual products).
Now, we need to assume the existence of a linkage between the pair \(\left( {Y_{ \uparrow }^{{({\text{in}})}} \wedge Z_{ \downarrow }^{{{\text{(fin}})}} } \right)\). This linkage is imposed by the physical linkage between the operators \(\Im_{{{\text{input}}}} \circ \,\,\Im_{{{\text{output}}}}\). In an enzymatic catalysis, the linkage between variables \(Y_{ \uparrow }^{{({\text{in}})}}\) and \(Z_{ \downarrow }^{{({\text{fin}})}}\) has chemical and thermodynamic constraints, but in the case of neural associative memories, these a priori constraints do not exist (see Sect. 3.2), because they emerge after contingent associative experiences.
Let us exemplify with some details these Y and Z sets based on the examples in Sect. 3. In the case of enzymatic catalysis (Fig. 1), \(Y_{ \downarrow }^{{({\text{in}})}}\) is the set of potential substrates and \(Y_{ \uparrow }^{{({\text{in}})}}\) is the subset of substrates selected by the specificity of the active sites of the enzyme; \(Z_{ \downarrow }^{{({\text{fin}})}}\) is the set of possible thermodynamically and chemically accessible states from \(Y_{ \uparrow }^{{({\text{in}})}}\), and \(Z_{ \uparrow }^{{{\text{(fin}})}}\) is the set of transformations selected by the properties of the catalytic sites of the enzyme. (The chemical and thermodynamic basis of this catalytic process is illustrated in detail in Dixon and Webb 1979.) In the case of a neural system, we will describe the interpretation of the sets based on both Fig. 2 and the prisoner's parable: the set \(Y_{ \downarrow }^{{({\text{in}})}}\) is the set of total signals received by the system (whether they represent noise or a code) and \(Y_{ \uparrow }^{{({\text{in}})}}\) is the subset recognized by the neural module; this \(Y_{ \uparrow }^{{({\text{in}})}}\) subset enters a network that is capable of selecting from a potential set of motor acts \(Z_{ \downarrow }^{{({\text{fin}})}}\), the specific subset \(Z_{ \uparrow }^{{({\text{fin}})}}\) of actions that solve the problem, in the case of the prisoner, the movements that open the safe. (An illustration of how a modular neural system achieves this type of specific response is shown in Mizraji 1989 and Mizraji et al 2009).
Let us assume that a very complex system can be characterized by a large set of potential transformations
$$\Omega^{{{\text{POT}}}} = \left\{ {\,\left[ {Y_{ \downarrow }^{{({\text{in}},r)}} \to Z_{ \uparrow }^{{({\text{fin}},q)}} } \right],\,\,\,(r,q) \in {\mathbb{N}} \times {\mathbb{N}}\,} \right\}.$$
(with low transition probabilities in the absence of a iCat). The set \(\Omega^{{{\text{POT}}}}\) has a high cardinal number. Let \(\Phi = \left\{ {{\text{iCat}}} \right\}\) be the actual set of iCat's that exists inside the system. Let us also assume the existence of a function \(\Upsilon\),
$$\Upsilon :\,\,\Omega^{{{\text{POT}}}} \times \,\,\Phi \,\,\, \to \,\,\,\Omega^{{{\text{ACT}}}} ,$$
that represents the collection of transformations from \(\Omega^{{{\text{POT}}}}\) onto the very much smaller set \(\Omega^{{{\text{ACT}}}} \subset \Omega^{{{\text{POT}}}}\) (the transformations that actually happen), promoted by the set of information catalysts \(\Phi\). This is a formalization of the creation of order by a set of iCat's.