Advances in High Energy Physics

Volume 2018, Article ID 7080232, 8 pages

https://doi.org/10.1155/2018/7080232

## From Quantum Unstable Systems to the Decaying Dark Energy: Cosmological Implications

^{1}Astronomical Observatory, Jagiellonian University, Orla 171, 30-244 Kraków, Poland^{2}Mark Kac Complex Systems Research Centre, Jagiellonian University, Łojasiewicza 11, 30-348 Kraków, Poland^{3}Institute of Physics, University of Zielona Góra, Prof. Z. Szafrana 4a, 65-516 Zielona Góra, Poland

Correspondence should be addressed to Marek Szydłowski; lp.ude.ju@ikswoldyzs.keram

Received 9 April 2018; Revised 25 June 2018; Accepted 31 July 2018; Published 19 August 2018

Academic Editor: Ricardo G. Felipe

Copyright © 2018 Aleksander Stachowski et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. The publication of this article was funded by SCOAP^{3}.

#### Abstract

We consider a cosmology with decaying metastable dark energy and assume that a decay process of this metastable dark energy is a quantum decay process. Such an assumption implies among others that the evolution of the Universe is irreversible and violates the time reversal symmetry. We show that if we replace the cosmological time appearing in the equation describing the evolution of the Universe by the Hubble cosmological scale time, then we obtain time dependent in the form of the series of even powers of the Hubble parameter : . Our special attention is focused on radioactive-like exponential form of the decay process of the dark energy and on the consequences of this type decay.

#### 1. Introduction

In the explanation of the Universe, we encounter the old problem of the cosmological constant, which is related to understanding why the measured value of the vacuum energy is so small in comparison with the value calculated using quantum field theory methods [1]. Because of a cosmological origin of the cosmological constant one must also address another problem. Namely, it is connected with our understanding, with a question of not only why the vacuum energy is not only small, but also, as current Type Ia supernova observations to indicate, why the present mass density of the Universe has the same order of magnitude [2].

Both mentioned cosmological constant problems can be considered in the framework of the extension of the standard cosmological CDM model in which the cosmological constant (naturally interpreted as related to the vacuum energy density) is running and its value is changing during the cosmic evolution.

Results of many recent observations lead to the conclusion that our Universe is in an accelerated expansion phase [3]. This acceleration can be explained as a result of a presence of dark energy. A detailed analysis of results of recent observations shows that there is a tension between local and primordial measurements of cosmological parameters [3]. It appears that this tension may be connected with dark energy evolving in time [4]. This paper is a contribution to the discussion of the nature of the dark energy. We consider the hypothesis that dark energy depends on time, , and it is metastable: We assume that it decays with the increasing time to : as . The idea that vacuum energy decays was considered in many papers (see, e.g., [5, 6]). Shafieloo et al. [7] assumed that decays according to the radioactive exponential decay law. Unfortunately, such an assumption is not able to reflect all the subtleties of evolution in the time of the dark energy and its decay process. It is because the creation of the Universe is a quantum process. Hence the metastable dark energy can be considered as the value of the scalar field at the false vacuum state and therefore the decay of the dark energy should be considered as a quantum decay process. The radioactive exponential decay law does not reflect correctly all phases of the quantum decay process. In general, analysing quantum decay processes one can distinguish the following phases [8, 9]: (i) the early time initial phase, (ii) the canonical or exponential phase (when the decay law has the exponential form), and (iii) the late time nonexponential phase. The first phase and the third one are missed when one considers the radioactive decay law only. Simply they are invisible to the radioactive exponential decay law. For example, the theoretical analysis of quantum decay processes shows that at late times the survival probability of the system considered in its initial state (i.e., the decay law) should tend to zero as much more slowly than any exponential function of time and that as a function of time it has the inverse power-like form at this regime of time [8, 10, 11]. So, all implications of the assumption that the decay process of the dark energy is a quantum decay process can be found only if we apply a quantum decay law to describe decaying metastable dark energy. This idea was used in [12], where the assumption made in [7] that decays according to the radioactive exponential decay law was improved by replacing that radioactive decay law by the survival probability , that is, by the decay law derived assuming that the decay process is a quantum process.

This is the place where one has to emphasize that the use of the assumption that dark energy depends on time and is decaying during time evolution leads to the conclusion that such a process is irreversible and violates a time reversal symmetry. (Consequences of this effect will be analysed in next sections of this paper) Note that the picture of the evolving Universe, which results from the solutions of the Einstein equations completed with quantum corrections appearing as the effect of treating the false vacuum decay as a quantum decay process, is consistent with the observational data. The evolution starts from the early time epoch with the running and then it goes to the final accelerating phase expansion of the Universe. In such a scenario the standard cosmological CDM model emerges from the quantum false vacuum state of the Universe.

The paper is organised as follows: In Section 2 one finds a short introduction of formalism necessary for considering decaying dark energy as a quantum decay process. Cosmological implications of a decaying dark energy are considered in Section 3. Section 4 contains conclusions.

#### 2. Decay of a Dark Energy as a Quantum Decay Process

In the quantum decay theory of unstable systems, properties of the survival amplitudesare usually analysed. Here a vector represents the unstable state of the system considered and is the solution of the Schrödinger equationThe initial condition for (2) in the case considered is usually assumed to beor equivalentlyIn (2) denotes the complete (full), self-adjoint Hamiltonian of the system. We have . It is not difficult to see that this property and hermiticity of imply thatTherefore, the decay probability of an unstable state (usually called the decay law), i.e., the probability for a quantum system to remain at time in its initial state ,must be an even function of time [8]:

This last property suggests that, in the case of the unstable states prepared at some instant , say , initial condition (3) for evolution equation (2) should be formulated more precisely. Namely, from (7), it follows that the probabilities of finding the system in the decaying state at the instant, say , and at the instant are the same. Of course, this can never occur. In almost all experiments in which the decay law of a given unstable subsystem system is investigated this particle is created at some instant of time, say , and this instant of time is usually considered as the initial instant for the problem. From property (7) it follows that the instantaneous creation of the unstable subsystem system (e.g., a particle or an excited quantum level and so on) is practically impossible. For the observer, the creation of this object (i.e., the preparation of the state, , representing the decaying subsystem system) is practically instantaneous. What is more, using suitable detectors he/she is usually able to prove that it did not exist at times . Therefore, if one looks for the solutions of Schrödinger equation (2) describing properties of the unstable states prepared at some initial instant in the system and if one requires these solutions to reflect situations described above, one should complete initial conditions (3), (4) for (2) by assuming additionally thatEquivalently, within the problem considered, one can use initial conditions (3), (4) and assume that time may vary from to only, that is, that .

Note that canonical (that is a classical radioactive) decay law (where is a lifetime) does not satisfy property (7), which is valid only for the quantum decay law . What is more, from (5) and (6) it follows that at very early times, i.e., at the Zeno times (see [8, 13]),which implies thatSo at the Zeno time region the quantum decay process is much slower than any decay process described by the canonical (or classical) decay law .

Now let us focus the attention on the survival amplitude . An unstable state can be modeled as wave packets using solutions of the following eigenvalue equation , where , and denotes a continuum spectrum of . Eigenvectors are normalized as usual: . Using vectors we can model an unstable state as the following wave-packet:where expansion coefficients are functions of the energy and is the lower bound of the spectrum of . The state is normalized , which means that it has to be . Now using the definition of the survival amplitude and the expansion (11) we can find , which takes the following form within the formalism considered:where and is the probability to find the energy of the system in the state between and + . The last relation (12) means that the survival amplitude is a Fourier transform of an absolute integrable function . If we apply the Riemann-Lebesgue Lemma to integral (12) then one concludes that there must be as . This property and relation (12) are an essence of the Fock–Krylov theory of unstable states [14, 15].

As it is seen from (12), the amplitude and thus the decay law of the unstable state are completely determined by the density of the energy distribution for the system in this state [14, 15] (see also [8, 10, 11, 16–21]).

In the general case the density possesses properties analogous to the scattering amplitude; i.e., it can be decomposed into a threshold factor, a pole-function with a simple pole, and a smooth form factor . There is , where depends on the angular momentum through [8] (see equation (6.1) in [8]), ) and is a step function: for and for . The simplest choice is to take , , and to assume that has a Breit–Wigner (BW) form of the energy distribution density. (The mentioned Breit–Wigner distribution was found when the cross section of slow neutrons was analysed [22]) It turns out that the decay curves obtained in this simplest case are very similar in form to the curves calculated for the above described more general (see [16] and analysis in [8]). So to find the most typical properties of the decay process it is sufficient to make the relevant calculations for modeled by the Breit–Wigner distribution of the energy density , where is a normalization constant. The parameters and correspond to the energy of the system in the unstable state and its decay rate at the exponential (or canonical) regime of the decay process. is the minimal (the lowest) energy of the system. Inserting into formula (12) for the amplitude and assuming for simplicity that , after some algebra, one finds thatwhereHere , is the lifetime, , and . The integral has the following structure:whereand(The integral can be expressed in terms of the integral-exponential function [23–26] (for a definition, see [27, 28])) The result (15) means that there is a natural decomposition of the survival amplitude into two parts:whereandand is the canonical part of the amplitude describing the pole contribution into and represents the remaining part of .

From decomposition (18) it follows that in the general case within the model considered the survival probability (6) contains the following parts:This last relation is especially useful when one looks for a contribution of late time properties of the quantum unstable system to the survival amplitude.

The late time form of the integral and thus the late time form of the amplitude can be relatively easy to find using analytical expression for in terms of the integral-exponential functions or simply performing the integration by parts in (17). One finds for (or ) that the leading term of the late time asymptotic expansion of the integral has the following form:Thus inserting (22) into (20) one can find late time form of .

As was mentioned we consider the hypothesis that a dark energy depends on time, , and decays with the increasing time to : as . We assume that it is a quantum decay process. The consequence of this assumption is that we should consider (where is the initial instant) as the energy of an excited quantum level (e.g., corresponding to the false vacuum state) and the energy density as the energy corresponding to the true lowest energy state (the true vacuum) of the system considered. Our hypothesis means that as . As it was said we assumed that the decay process of the dark energy is a quantum decay process: From the point of view of the quantum theory of decay processes this means that according to the quantum mechanical decay law. Therefore if we defineour assumption means that the decay law for has the following form (see [12]):where is given by relation (6), or, equivalently, our assumption means that the decay law for has the following form (compare [12]):where and is replaced by (21). Taking into account the standard relation between and the cosmological constant we can write where . Thus within the considered case using definition (6) or relation (21) we can determine changes in time of the dark energy density (or running ) knowing the general properties of survival amplitude .

The above described approach is self-consistent if we identify with the energy of the unstable system divided by the volume (where is the volume of the system at ): and . Here is the vacuum energy density calculated using quantum field theory methods. In such a case(where ), or equivalently .

#### 3. Cosmological Implications of Decaying Vacuum

Let us consider cosmological implications of the parameter with the time parameterized decaying part, derived in the previous section, in the formwhere describes quantum corrections and it is given by a series with respect to ; i.e.,where is the cosmological scale time and the functions and have a reflection symmetry with respect to the cosmological time . The next step in deriving dynamical equations for the evolution of the Universe is to consider this parameter as a source of gravity which contributes to the effective energy density; i.e.,where is identified as the energy density of the quantum decay process of vacuumIn this paper, we assume that . The Einstein field equation for the FRW metric reduces towhere , , or

Szydlowski et al. [12] considered the radioactive-like decay of metastable dark energy. For the late time, this decay process has three consecutive phases: the phase of radioactive decay, the phase of damping oscillations, and finally the phase of power law decaying. When for , dark energy can be described in the following form (see (25) and [12]):where , , and are model parameters. Equation (34) results directly from (25): One only needs to insert (22) into formula for and result (19) instead of into (25). In this paper, we consider the first phase of decay process, in other words, the phase of radioactive (exponential) decay.

The model with the radioactive (exponential) decay of dark energy was investigated by Shafieloo et al. [7]. During the phase of the exponential decay of the vacuumwhere ( is decaying).

The set of equations (33) and (35) constitute a two-dimensional closed autonomous dynamical system in the form

System (36) has the time dependent first integral in the formAt the finite domain, system (36) possesses only one critical point representing the standard cosmological model (the running part of vanishes, i.e., ).

System (36) can be rewritten in variableswhere is the present value of the Hubble function. Thenwhere and are a new reparametrized time. The phase portrait of system (39) is shown in Figure 1.