Quantum process capability

Physical processes in the quantum regime possess non-classical properties of quantum mechanics. However, methods for quantitatively identifying such processes are still lacking. Accordingly, in this study, we develop a framework for characterizing and quantifying the ability of processes to cause quantum-mechanical effects on physical systems. We start by introducing a new concept, referred to as quantum process capability, to evaluate the effects of an experimental process upon a prescribed quantum specification. Various methods are then introduced for measuring such a capability. It is shown that the methods are adapted to quantum process tomography for implementation of process capability measure and applicable to all physical processes that can be described using the general theory of quantum operations. The utility of the proposed framework is demonstrated through several examples, including processes of entanglement, coherence, and superposition. The formalism proposed in this study provides a generic approach for the identification of dynamical processes in quantum mechanics and facilitates the general classification of quantum-information processing.

Physical processes in quantum mechanics attract considerable interest on account of their unusual characteristics and potential applications. Investigating how and why these processes cannot be explained using classical physics provides an important insight into the fundamentals of quantum mechanics [1][2][3] . By definition, engineering-oriented procedures are physical processes. Then such purely physical investigation inspires the question as to how quantum-mechanical effects can be harnessed to perform practical tasks 4 . Moreover, feasible techniques for fully exploring the possibilities and limitations of these tasks based on quantum mechanics are still lacking 5 . The effort to address these issues has revolutionized the conventional methods for engineering physical systems and has greatly advanced the development of quantum technology [6][7][8] .
Quantum information processing 9 provides a new paradigm for the emerging generation of quantum technologies, such as quantum computation 10 and quantum communication 11 . The underlying manipulations of quantum systems are all derived from dynamical processes in quantum mechanics, and range from gate operations 10,12 to information storage and protection against the effects of noise 13 , from the creation of entanglement to teleportation 14,15 and entanglement swapping 16 . Identifying the elementary classes of quantum dynamical processes, therefore, is not only significant in its own right, but is also a fundamental goal in uniting work on quantum information theory 9 .
Considerable progress has been made in understanding quantum dynamical processes; in particular, in identifying the quantum properties of the output states [17][18][19][20][21][22][23][24] . However, a fully comprehensive analogue for dynamical processes has yet to be found. Moreover, despite the success of theoretical methods in describing the dynamics of quantum systems, such as the quantum operations formalism 3 , the problem of characterizing the prescribed quantum-mechanical features of dynamical processes in a quantitatively precise manner has yet to be resolved. As a result, it is presently intractable to quantitatively distinguish the different processes in quantum mechanics.
Motivated by this problem, and driven by the desire to ultimately identify all quantum dynamical processes, we present herein a method for quantifying the extent to which a process quantum mechanically behaves and affects a system. We commence by introducing a new concept referred to as the quantum process capability for evaluating the prescribed quantum-mechanical ability of a process. We then introduce two capability measures and a task-oriented capability criterion, which demonstrate that such process evaluation can be quantitatively determined through experimentally feasible means. We show that with the proposed tools, it is possible, for the first time, to quantitatively identify several fundamental types of dynamical process, including processes of entanglement, coherence and superposition.
We begin by systematically characterizing the physical process acting on a system using the quantum operations formalism. In doing so, we assume that the system of interest and its environment are initially in a product 1 2 , then process χ is also incapable, where  denotes the concatenation operator.
(P2) If a process is a linear combination of incapable processes: , then χ is also an incapable process.
These properties imply that manipulating incapable processes inevitably results in another incapable process. Furthermore, if the process χ expt cannot be described by any incapable processes  χ in any way at all, then χ expt must be capable regarding the corresponding quantum-mechanical specification.
To place the basic definitions of capable and incapable processes into a wider context, we now introduce a measurable property of a process called the quantum process capability, which provides a quantitative understanding of how well χ expt might work, and helps identify processes with prescribed quantum process abilities. The proposed property has applications not only for exploiting the quantum effects behind an unknown process, but also for assisting in the evaluation and improvement of primitive operations for task-oriented purposes. (Note that more general features will be described in the later discussion section).
The quantum process capability of a process can be quantitatively evaluated using different tools according to the type of specification or subsequently used experimental process. The following discussions propose two methods for evaluating the quantum process capability, namely the capability measures and the task-oriented capability criterion. capability measure. We desire to have a tool that can faithfully reflect the features of capable and incapable processes, respectively, and reliably show how the quantum process capability of χ expt changes after applying additional operations to the system. Let the capability measure be defined as a function of the process matrix, χ C( ), which has the following three properties: (MP1) χ = C( ) 0 if and only if χ is incapable. (MP2) Since incapable processes consist of only incapable ingredients by definition [see (P1) and (P2)], one cannot increase the capability of a process by incorporating additional incapable ones. In other words, it follows that (2a) The capability measure of χ monotonically decreases with an incorporated incapable process, i.e., The capability measure reflects the non-increasing capability of a process under stochastic incapable operations: To show how the quantum process capability can be concretely quantified, we now introduce two different types of capability measure, which both satisfy properties (MP1)-(MP3) defined above (see Methods section).
M1. Capability composition α. A process matrix, χ expt , can be represented as a linear combination of capable and incapable processes, i.e., where ≥ a 0. The capability composition of χ expt is then defined as which specifies the minimum amount of capable process that can be found in the experimental process.
In the practical examples presented later in this study, α is obtained by minimizing the following quantity via semi-definite programming (SDP) with MATLAB 28,29 Note that the solution is obtained under a set of specified conditions for the incapable process, Here, χ   and  χ  are both unnormalized process matrices with a a tr( ) tr( ) , respectively. Rephrasing the process matrices in terms of unnormalized matrices reduces the number of variables to make the problem solvable using SDP. The number of variables is determined by the number of elements in a process matrix. For example, there are at least 16 variables that need to be solved in a single qubit system. For different capabilities, it may need more variables to describe the constraints χ  D( )  . See Methods. χ  D( )  places constraints on the process matrix construction of the incapable process in the process tomography algorithm, which specifies how the input and output states for the process tomography behave under an incapable process.
M2. Capability robustness β. An experimental process, χ expt , can become incapable by mixing with noise, i.e., where ≥ b 0 and χ′ is the noise process. The capability robustness of χ expt can be defined as the minimum amount of noise which must be added such that χ expt becomes  χ , i.e., β ≡ . χ′ b min (4) In practical cases, β can be obtained by using SDP to solve β , which ensure that β ≥ 0 and χ′ is positive semi-definite, respectively.
Quantum criterion. When χ expt is created with respect to a target process, χ target , that is defined as capable for engineering-oriented purposes 9-11 , the process fidelity, χ χ ≡ F tr( ) expt expt target , enables us to examine the similarity between them. In particular, χ expt is judged to have a capability close to that of the target process if it goes beyond the best mimicry by incapable processes to χ target , i.e., expt target    meaning that χ expt is a faithful operation which cannot be simulated by any incapable processes. Note that F  in (5) can be evaluated by performing the following maximization task with SDP:  Moreover, from a reasonable engineering-oriented perspective, we consider χ target capable and to be the default, i.e.,  < F 1. Note that the criterion (5) does not satisfy (MP1)-(MP3). If the process fidelity under the criterion (5) is used to serve as a capability measure, say  , this fidelity measure will not be necessarily equal to zero when the χ expt is an incapable process. The reason is that F  is the optimal value for all incapable processes, which means that the fidelity criterion (5) does not satisfy (MP1). Since Capability examples. Let the following capable processes be used to demonstrate the formalism described above: E1. Non-classical dynamics. As defined in ref. 30 , a non-classical dynamics is a dynamical process that cannot be explained using a classical picture: the initial system is considered a physical object with properties satisfying the assumption of classical realism, and the system thus evolves according to classical stochastic theory.
Non-classical dynamics can be quantified and used as the requirement for the non-classical manipulation of a system 30 , e.g., the fusion of entangled photon pairs 31 . In the present context of quantum process capability, non-classical dynamics is capable of going beyond the generic model of classical dynamics, compared to incapable classical processes. The quantifications of non-classical processes introduced in ref. 30 reveal the capability of non-classical dynamics, and include the capability composition α (2), the capability robustness β (4) and the capability criterion (5).
E2. Entanglement generation. Creating entanglement is a crucial dynamical process in both quantum mechanics and quantum-information processing 9,10 . However, the means to quantify the ability of a process to generate the entanglement of two qubits remains unclear.
Let entanglement creation be defined as a capable process, χ ent . Any process that merely preserves the separability of a quantum system is therefore said to be incapable, and is denoted by χ ,ent  . The capability measures of χ ent , such as α and β, confirm that χ > C( ) 0 ent . By contrast, the capability measure of  χ ,ent is minimum, i.e., . The concrete set of constraints acting on the incapable process  χ  D( ) ,ent in calculating α, β and  F is given by ,ent in in ,ent in PT in sep where s sep denotes the set of separable states. The first constraint in Eq. (6) ensures that the output states are positive semi-definite for all the input states required in the process tomography algorithm. As will be illustrated below, this condition is necessary for all incapable processes. The second constraint is based on the positive partial transpose (PPT) criterion 32,33 , and guarantees that if the input states are separable states, the output states are separable states as well. In other words, the PPT criterion stipulates that an output state ρ out after partial transposition (PT) is positive semi-definite, i.e., ρ ≥ 0 out PT , if and only if the state ρ out is separable. E3. Coherence creation and preservation. Quantum coherence is one of the main features of quantum systems 18,[21][22][23] , and is the main power behind quantum technology 6,7 . If the density matrix of a d-dimensional system is not diagonal in a given orthonormal basis 1}, then the system is said to possess coherence www.nature.com/scientificreports www.nature.com/scientificreports/ with respect to basis | 〉 j { } 21 . A mixture consisting only of the basis states of the form: , is then said to be an incoherent state.
Coherence creation and preservation are essential in performing state preparation and manipulation in quantum engineering [9][10][11]13 . They represent two different abilities of capable processes, and are denoted hereafter as χ cre and χ pre , respectively. The capability measure of coherence creation shows that χ > C( ) 0 cre . Compared with χ cre , an incapable process, χ ,cre  , cannot create coherence, i.e., incoherent states remain incoherent, and hence the coherence capability measure is minimum, To evaluate α, β and  F , for a process incapable of coherence creation, ,cre in in ,cre in incoh in incoh where  s incoh and s incoh denote the sets of unnormalized incoherent states and incoherent states regarding the basis | 〉 j { }, respectively. In other words, if the input states are incoherent states, then the output states must also be incoherent states.
Regarding the capability of coherence preservation, χ C( ) pre has a positive value for a capable process. By contrast, an incapable process causes the states to decohere, i.e., , for an incapable process is formulated as In other words, all of the output states are incoherent states, regardless of the input state ρ in . It is noted that this is different from the coherence creation case, in which the input states are restricted to incoherent states.
E4. Superposition of quantum states. The superposition principle of quantum mechanics 24,34 describes how any two or more quantum states can be superposed together to form another valid quantum state (and vice versa). The superposition of quantum states therefore generalizes the capability of coherence creation in the orthonormal basis | 〉 j { } to the ability to superpose states in a normalized and linear independent basis j . Superposition states cannot be explained by any mixture of the basis states: , and are hence referred to as superposition free states 24 .
For a capable superposition process, the capability measure has a positive value, χ > C( ) 0 sup . By contrast, for an incapable process, χ ,sup  , i.e., a process which merely preserves the mixture in the superposition free states, the capability measure is given as . The constraints on the incapable process, where  s supf and s supf denote the sets of unnormalized superposition free states and superposition free states under indicates that if ρ in is a superposition free state, then the output state must also be superposition free.
Demonstration of the process capability measures. We now provide an explicit example illustrating how a dynamical process of interest can be identified upon the prescribed quantum specification (i.e., E1-E4). We consider the case of a composite system consisting of two qubits. Let the qubits be coupled via an interaction, equivalent to the quantum Ising model, of the Hamiltonian 35 : , which is an important primitive for creating cluster states in a one-way quantum computer 36 . The composite two-qubit evolution can be represented by an unitary transform can be considered as an implementation of the controlled-Z gate. Moreover, assume that one of the qubits is depolarized at a rate γ. The depolarization of a qubit can be represented in the form where Î is identity matrix. By using the process tomography algorithm, the process matrix of such depolarization is Given γ = 0.02, Fig. 1a,b illustrate the variations of α and β, respectively, for the five different capabilities described above with the qubit interaction time, t. The set of specified conditions for different capabilities for the incapable process,  χ  D( ), used to evaluate α, β, and  F for this example are given in Methods section. Figure 1c compares the process fidelity, F expt , with the four different thresholds F  of the capable processes, with respect to a target process, the controlled-Z gate. When = F 1 expt , it means the χ t ( ) expt arrives at the target process, the controlled-Z gate. There are oscillations of α, β, and F expt in Fig. 1 , the oscillation period will become π in our example. An observation of Fig. 1 yields several important conclusions regarding process identification and classification, as described in the following.
First, compared to α, the capability robustness measure β provides a clearer distinction between the various processes under different interaction periods. This distinction can be realized by characterizing how close χ t ( ) expt is to an incapable process in the sense of how large the minimum amount of noise β is required to be to make χ t ( ) expt incapable (see Methods). Second, while the process considered in Fig. 1 has no ability to create coherence, it enables the two qubits to be entangled. Such a result implies that the coherence of the output entangled qubits is not generated by the process χ t ( ) expt itself, but is transformed from the input states. In other words, χ t ( ) expt has 0 02 in the present example. It is worth noting that χ t ( ) expt can serve as a controlled-Z (CZ) gate at a proper interaction time 36 . When setting this gate operation as the target process, the process fidelity F expt varies with time. As indicated in (c), the capability thresholds F  for superposition, entanglement generation, non-classical dynamics, and coherence preservation are: 0.750, 0.500, 0.467 and 0.250, respectively. Since the CZ gate can be described by incapable processes  χ ,cre , and is not a proper target process for coherence creation, such process capability is not considered in (c). Note that, in (a), for coherence preservation, the process is always a capable process, since the depolarization only acts on one of the qubits and another qubit can still preserve coherence of single qubit. According to the definition of the incapable process of coherence preservation (i.e., all the output states must be incoherent states), this process is always capable process of coherence preservation. (2019) 9:20316 | https://doi.org/10.1038/s41598-019-56751-x www.nature.com/scientificreports www.nature.com/scientificreports/ the ability to convert the coherence of the input states into an entanglement of the qubits at specific qubit interaction times. The efficiency of this coherence conversion process can be determined by the capability of entanglement generation, as evaluated by β, for example (see Methods).
Third, superposition can be performed either by purely unitary evolution or by quantum jumps of depolarization. The latter phenomenon can be seen in Fig. 1b can be converted into a superposition of the basis states | 〉 h j . (Note that this fact can be understood in an analogous fashion to that used to understand the conversion of the coherence of the input states into entanglement) (see Methods).

Discussion
The quantum process capability framework introduced above possesses several important features for practical utility and extensions, as described in the following.
(D1) Since constructing the process matrix is experimentally feasible, the process capability can be readily quantified in various present experiments. The quantum operations formalism underlying the process matrix is a general tool for describing the dynamics experienced by closed or open quantum systems in a wide variety of physical scenarios. Our formalism is therefore applicable to all physical processes described by the general theory of quantum operations, including, but not limited to, the fundamental processes postulated in quantum mechanics 2,9 , the dynamics of energy transfer systems 37 , the task-orientated processes associated with quantum information 10,11,31 , and the atomic-physics and quantum-optics experiments on a chip 38 .
(D2) In addition to the capable processes illustrated above (i.e., E1-E4), the present framework can also be used to explore other types of quantum process capability, including the creation of genuine multipartite entanglement 39 , Einstein-Podolsky-Rosen steering 40 , Bell non-locality 20 , and genuine multipartite quantum steering 41,42 .
(D3) Process identification and classification. As distinct process capabilities are given, dynamical processes can be identified and classified accordingly using the capability measures, such as the capability robustness. This is helpful in uniting existing works on quantum information under a given type of quantum process capability, for example, the preservation of quantumness 30 or the coherence of quantum information [9][10][11]13 .
(D4) Benchmark for process engineering. The capability criterion (5) sets a level  F of quantum-mechanical quality that can be used as a standard when comparing other experimental processes for task-oriented purposes 9-11 ; as illustrated in Fig. 1c.
(D5) Insightful description of processes. A given quantum process capability may be linked in some way with other concepts. For example, the capability of non-classical dynamics can be used to reveal the non-Markovianity of dynamical processes 30,43,44 . Alternatively, the capability of entanglement generation also provides an understanding of the efficiency of coherence conversion. The framework proposed herein thus facilitates a more comprehensive understanding of the characteristics of quantum dynamics.
(D6) Maximum extraction of resources from processes. The quantum effects of a process on the system inputs, ρ in , as revealed by the output states, ρ out , are usually considered as quantum resources, such as entanglement 45,46 and coherence 21,22 . The maximum amount of resources that can be extracted from a given process, χ expt , can be quantified in terms of the quantum process capability, χ C( ) expt , using an appropriate capability measure. The reason for this lies in the fact that the quantum process capability provides an optimal description of the prescribed quantum specification in χ expt in the sense that the framework proposed in this study does not depend on any specifics of the states being processed (see Methods section).
In conclusion, we have developed a novel formalism for performing the quantitative identification of quantum dynamical processes. The concept of quantum process capability and its various quantifications have been introduced to evaluate the prescribed quantum-mechanical features of a dynamical process. The ability to quantify the ability of a process in terms of its quantum process capabilities makes it possible to discriminate quantitatively between different dynamical processes. Overall, the rigorous framework of quantum process capability proposed in this study provides the means to go beyond the usual analysis of state characteristics and to approach the goal of uniting work on quantum information theory.
Future studies will aim to improve the performance and scalability of the process tomography 47 underlying the proposed formalism, including scenarios such as where the measurement outcomes are continuous and unbound, e.g., as for nanomechanical resonators 48 . It is anticipated that the enhanced framework will thus facilitate the novel recognition and classification of physical processes with quantum process capability. We consider a process consisting of the experimental process 9,27 , χ expt , and an incapable process, χ  , of the form  (2), the process χ χ  n expt  can be represented as

Methods
Note that, while α is the capability composition of χ expt , i.e., the optimal result for χ expt , it is not necessarily the optimal result for χ χ  n expt  . Since χ n  and χ  are both incapable processes, χ χ  n   must also be an incapable process. For χ χ  n C I , there exists a possibility that the process is not capable, i.e., it contains a certain non-vanished amount of incapable process. Therefore, the minimum amount of capable process that can be found in  χ χ  n expt cannot be greater than α. In other words, it follows that it is possible to find specific capable and incapable processes, denoted by χ ′ n  and χ ′ n  , respectively, which yield the following decomposition: n n n n n expt I C I Since α n is the capability composition of n which implies that Thus, we conclude that the capability composition measure satisfies the property, n n n n , and  α = ∑ a p n n n . Note that a  is not necessarily optimal for χ χ  expt  . Since each process  χ ′ n is an incapable process,  χ ′ is also an incapable process. In accordance with the definition of capability composition, we have α n n n which satisfies the property,  i.e., Here we take the capability composition α of entanglement generation for example to demonstrate the three properties (MP1) -(MP3) for capability measure. Let us consider the instance of coupled qubits discussed in Fig. 1. As shown in the inset of Fig. 1a for time evolution without noise effect, when = t 0, the process χ (0) expt is identity process which has no capability to generate entanglement from separable states. Then χ (0) expt is an incapable process and its χ C( (0)) expt is 0 (MP1). If we incorporate the incapable process χ (0) expt into the capable process χ π ( ) expt , we find that the incapable process does not increase the capability composition α,  www.nature.com/scientificreports www.nature.com/scientificreports/ The properties (MP1)-(MP3) also hold for the time evolution under the noise effect. In Fig. 1a, when π = t 2 , the process χ π (2 ) expt is a process that has no capability to generate entanglement from separable states, so χ π (2 ) expt is an incapable process and its χ π C( (2 )) expt is 0 (MP1). The capability composition of a capable process χ π ( ) expt does not increase by incorporating additional incapable process χ π (2 ) expt , i.e., χ π χ π χ π = . < = .  C C ( ( ) (2 )) 0 742 ( ( )) 0 909, expt expt expt and satisfies property (2a) in (MP2). The example for property (2b) in (MP2) can be known from the case, expt expt together, the mixed process satisfies the property (MP3), χ π χ π χ π χ π χ π χ π χ π χ π Since χ n  and χ  are both incapable processes, χ χ  n   must also be an incapable process. It is worth noting that, while β is the robustness of χ expt , i.e., it is an optimal value for χ expt , it is not necessarily the optimal value for the resulting process, In general, the quantum process capability cannot be increased by applying additional incapable processes. Thus, the minimum amount of noise added to χ χ  n expt  should be equal to (or less than) the minimum amount of noise added to χ expt . In accordance with Eqs. (3) and (4), we define β n as the optimal result for  χ χ  n expt . We now get n from which we conclude that In other words, the capability robustness measure possesses the property, (MP3): The process χ χ  expt  (10) can be expressed as n n n n    , and  β = ∑ b p n n n . From the definition of the capability robustness, we know that β Thus, the capability robustness measure has the property χ χ Comparison between α and β. The idea underlying the capability composition measure highlights whether a process can be described by the model of an incapable process. Such a feature indicates that this measure is unable to reveal the distinction between processes, in general. By contrast, the idea of how close a process is to an incapable process, which underlies the capability robustness measure, makes the difference between processes visible. constraints on incapable processes. In this section, we present the constraint sets  χ  D( ) required in the capability examples presented in the main text, where  χ  is an unnormalized process matrix 9 . To obtain the constraints for the incapable process  χ  D( ), we provide in the following the limitations on both the prepared input states and their corresponding output states, which are used to construct the process matrix 9 .
E1. Non-classical dynamics. To demonstrate the constraint set for the incapable processes of non-classical dynamics χ  D( ) ,ncl  , shown in Fig. 1, we first introduce classical processes 30 for a two qubit system. In general, a classical process can be described by its classical states and their evolution. The classical states of input systems satisfy the assumption of realism and can be represented by the realistic sets ≡ represents the possible measurement outcomes of the ith physical property for the jth classical object. The evolutions of these states are described by transition probabilities, Ω ξμ , from ξ v to a final state μ, which can be reconstructed as a density operator ρ μ by using state tomography. Such an evolution can always be rephrased as the transition from a specific state set ξ v to some final state ρ μ′  with Ω = ξμ′ 1, where ρ μ′  denotes the unnormalized density matrix. The constraint set  χ  D( ) ,ncl for the incapable process of non-classical dynamics is given as which ensures that all the output states ρ μ′  of classical processes are positive semi-definite. The constraint set . Since all of the input states ρ in prepared for process tomography are separable states, the output states, ρ  k l m n , must also be separable states for a process with no ability to generate entangled states. The constraint set for the incapable process of entanglement generation is given by , , . The remaining constraints in (26) ensure that when the input states are an identity matrix Î , the corresponding output states are the same for different decompositions of Î . Such a requirement is used in tomographically characterizing separable output states ρ out of incapable processes, where the outputs of Pauli matrices associated with the identity matrix in the inputs σ σ ⊗ k l should be objectively described, independent of measurement bases. Since the identity matrix Î can be represented as the sum of two eigenstates of the Pauli matrices, i.e., , the output state of Î for χ  ,ent  must be the same no matter how it is decomposed. For the second constraint in Eq. (26), which states that the input of the first qubit is Î , the outputs  χ ⊗ | 〉〈 | Î l l ( ) n n ,ent www.nature.com/scientificreports www.nature.com/scientificreports/ are the same for all decompositions of Î . The third and fourth constraints in Eq. (26) state that the input of the second qubit and the input of both qubits are Î , respectively.
E3. Coherence creation and preservation. To construct the process matrix using process tomography 9 , we first prepare the input states . The above specification is also applicable to superposition.
The constraint set χ  D( ) ,cre  for the incapable process of coherence creation is given by   To determine the process matrix, we need 16 matrices, so there are 196 variables that need to be solved by SDP in two qubit system. This is less than the number of variables for non-classical dynamics, since they have different constraint sets  χ  D( ). For the quantum Ising model shown in Fig. 1   with a depolarizing effect, η π = . ( /2) 0 624 sup and η π = .
1 361, respectively. Notably, depolarization at π = t /2 causes the η π ( /2) sup to increase, but makes the superposition robustness β decrease. As a result, the capability of superposition cannot be used to examine the coherence conversion efficiency. ) /(1 ) out , respectively, where ρ χ ρ ′ = ′( ) in , and  ρ χ ρ = ( ) C in are assumed to possess the prescribed resources. One can consider the minimum values of a and b as the quantities of resources that can be found in ρ out under a given input state ρ in and for all possible  ρ and ρ′. By maximizing the quantity of resources for all incapable input states, we obtain the maximum amount of resources that can be extracted from χ expt . Since the above optimization tasks have been considered in Eqs. (2) and (4), we conclude that α and β can quantify the maximum extraction of resources from a process.