CC BY
38
УЧЕНЫЕ ЗАПИСКИ КАЗАНСКОГО УНИВЕРСИТЕТА
Физико-математические пауки
UDK 514.7
THE PETROV CLASSIFICATION AND VACUUM DARK FLUID
I. Dymnikova
Abstract
The Pet.rov classification of stress-energy tensors makes it possible to introduce a unified description of dark energy and dark matter as a vacuum dark fluid based on the space-time symmetry. In this approach a vacuum dark energy is described by a variable cosmological term whose symmetry is reduced as compared with the Einstein cosmological term which allows a vacuum energy to be evolving and clustering. The relevant class of solutions to the Einstein equations implies also the existence of compact vacuum objects generically related to a dark energy: regular black holes, their remnants and self-gravitating vacuum solit.ons with de Sitter vacuum interior which can be responsible for observational effects typically related to a dark matter. The mass of objects with de Sitter interior is generically related to vacuum dark energy and to breaking of space-time symmetry.
Key words: dark energy, dark matter, regular black holes and solit.ons with de Sitter core.
Introduction
Quantum field theory in curved space-time does not contain a unique specification for the quantum state of a system, and the symmetry of a vacuum expectation value of a stress-energy tensor does not always coincide with the symmetry of a background space-time [1]. In the case of the de Sitter space the renormalized expectation value of (TMV} for a scalar field with an arbitrary mass m and curvature coupling £ is proved to have a fixed point attract or behavior at late times ( fl] and references therein) approaching, dependency on m and £, or the Bunch - Davies de Sitter-invariant vacuum either, for the massless minimally coupled case (m = £ = 0) the de Sitter invariant Allen Folacci vacuum. The last case is peculiar since the de Sitter invariant two-point function is infrared divergent, and the vacuum states, free of this divergence, are 0(4)-invariant Fock vacua: the vacuum energy density in the 0(4)-invariant case is not the same (larger) than in de Sitter-invariant case [2].
The Petrov classification of stress-energy tensors provides opportunity to consider vacuum in a model-independent way, as a medium specified by the algebraic structure of its stress-energy tensor [3-5]. The Einstein cosmological term AgMV corresponds to the de Sitter vacuum presented by the stress-energy tensor of maximal symmetry, with all three spacelike eigenvalues equal to the timelike eigenvalue. As a result it has an infinite set of co-moving reference frames, so that an observer cannot in principle measure his velocity with respect to it [3]. The maximal symmetry of a vacuum stress-energy tensor can be reduced to the case when less than three spacelike eigenvalues are equal to the timelike eigenvalue [4, 5]. This leads inevitably (by the Bianchi identities) to dynamical vacuum energy represented by anisotropic vacuum dark fluid which can both be distributed and form compact objects [6]. It generates regular space-time with the de Sitter interior whose existence follows from requirements of regularity and certain energy conditions on a source term in the Einstein equations [7].
Vacuum dark fluid provides a unified description of dark energy and dark matter. The key point is that astronomical data testify in favor of a cosmological vacuum dark energy described by the Einstein cosmological term (see [8] and references therein). The problem is that density of de Sitter vacuum must be constant by the contracted Bianchi identities, while the inflationary paradigm requires its much bigger value for the earliest stage of the Universe evolution. Vacuum dark fluid represents a cosmological vacuum by a variable spherically symmetric cosmological term which connects smoothly two de Sitter vacua at r ^ 0 Mid r ^ <x>. Its symmetry is reduced as compared with the Einstein cosmological term which allows a vacuum energy to be evolving and clustering. Time-evolving and space-inhomogeneons cosmological term [5] describes regular cosmological models dominated by vacuum dark energy [9].
The relevant class of solutions to the Einstein equations implies the existence of compact vacuum objects generically related to a dark energy through their de Sitter vacuum interiors: regular black holes [4. 10]. their remnants [11, 12] and self-gravitating vacuum solitons [7, 11, 13], which can be responsible for observational effects typically-related to a dark matter [6].
The question of the origin of dark matter still remains open [14]. The most popular hypothesis is that dark matter consists of neutral weakly interacting particles created in the hot early Universe. However, recently gathered results lead to the conclusions that known elementary particles can not account for a dark matter, at least in the frame of the Standard Model [15]. Dark energy particles as quanta of the cosmological constant A (considered as the fundamental constant) were proposed in [16] for a wide range of masses up to 1055 g including thus also observable Universe. In models of a unified dark finid with scalar fields, a dark energy is treated as a remnant density of a complex scalar field and dark matter as particles of this field [17], although the form of the scalar field potential can not be directly derived from high energy theories.
Vacuum dark fluid provides a model-independent dark energy-dark matter unification based on the space-time symmetry. Vacuum gravitational solitons called G-lnmps [7] (they are bounded by their own gravity balanced at the surface where the strong energy condition is violated) can be responsible for local effects related to a dark
A
Black holes (especially primordial) are recognized as good dark matter candidates [18]. Black hole remnants (final products of Hawking evaporation) have been considered as a source of dark matter for more than two decades [19] (for a review see [14]). The open question discussed in the literature concerns the existence of remnants: In the case of a singular black hole it would be a Planck size black hole: however, no evident symmetry or quantum number exists which would prevent complete evaporation. Character and scale of uncertainty concerning an endpoint of the Hawking evaporation of a singular black hole are clearly evident in the case of a nmltihorizon space-time [20]. The fate of a regular black hole is unambiguous: it leaves tliermodynamically stable donble-horizon remnant with the positive specific heat [11, 12].
Mass of objects is related to interior de Sitter vacuum and breaking of space-time symmetry from the de Sitter group at the origin [7]. This has been tested by evaluating the gravito-electroweak unification scale from the measured mass-sqnarcd differences for solar and atmospheric neutrinos [21]. Nonlinear electrodynamics coupled to gravity-provides a non-trivial example of a matter object with dark energy interior [22, 23] which we discuss in Section 2. In Section 1 we present the vacuum dark fluid in general setting, and in Section 2 we show how it can provide a unified description of dark energy-arid dark matter.
1. Vacuum dark fluid
The Einstein cosmological term AgMV with A = const, corresponds to a vacuum stress-energy tensor of the maximal symmetry
ASVV = 8nGTVaC- (1)
In the Petrov classification, stress-energy tensors are classified on the basis of their algebraic structure. When eigenvalues of TVV are real, the eigenvectors of TVV are non-isotropic and form a comoving reference frame with a timelike eigenvector representing a velocity.
In this classification an anisotropic fluid is specified by fllll] and [11(H)], and an isotropic fluid by [I(III)]. The first symbol denotes the eigenvalue related to the timelike eigenvector. Parentheses combine degenerate eigenvalues. A comoving reference frame is defined uniquely if and only if none of spacelike eigenvalues Ak (k = 1,2, 3) coincides with a timelike eigenvalue A0. Otherwise there exists an infinite set of comoving reference frames.
The maximally symmetric de Sitter vacuum (1), specified by [(IIII)] in the Petrov classification scheme (all eigenvalues equal, all reference frames comoving), represents the isotropic vacuum fluid. The high symmetry of a vacuum stress-energy tensor (1) can be reduced to the case when one (or two) of the spacelike eigenvalues of TVV coincides with its timelike eigenvalue
Pk = -P. (2)
A vacuum stress-energy tensor with a reduced symmetry is invariant under Lorentz k
reference frame and thus fix the velocity with respect to a vacuum fluid which is intrinsic property of a vacuum [24].
A vacuum defined by the symmetry of its stress-energy tensor must be evidently anisotropic (except the maximally symmetric de Sitter vacuum (1)). The Petrov classification scheme suggests three types of anisotropic vacuum fluid: f(II)(II)]. [(11)11]. [(III)I] [6].
A spherically symmetric vacuum fluid corresponds to [(II)(II)] and is specified by [4]
Tt = t;. (3)
It satisfies the equation of state (following from TVV = 0) for anisotropic perfect fluid
rdP !A\
Pr = -P, =
and generates space-time with the de Sitter center whose existence follows from requirements of regularity and the weak energy condition on a source term in the Einstein equations [7].
The Einstein equations with a source term specified by (3) admit the class of regular solutions asymptotically de Sitter as r ^ ^d r ^ to [5, 7]
(8nG)-1ASV TV (8nG)-1ASV (5)
with A < A. The metric of a space-time is given by
ds2 =g(r)dt2 -^f-- r2dtt2
g(r)
g(r)
Fig. 1. Metric function in the case of three horizons
with the metric function [10]
r
g(r) = 1
2GM{r) _ Л о r 3 '
M(r) = 4n / p(x)x2 dx,
I
(7)
0
which evolves from the de Sitter metric function g(r) = 1 — (Л + A)r2/3 as r ^ 0, to the Kottler - Trefftz metric function g(r) = 1 — rg/r — Ar2/3, rg = 2GM Дог r С r* where r* = (r2rg)1/^th r" = 3/Л, is the characteristic length scale in geometry with de Sitter center ([4] and references therein). The mass parameter (gravitational mass)
is related to interior de Sitter vacuum and breaking of space-time symmetry from the de Sitter group at the origin [7]. Space-time can have not more than three horizons [9]. the cosmological horizon rc, the black bole horizon rb < rc, and the internal horizon ra < rb (see Fig. 1).
The internal horizon r = ra is the cosmological horizon for a static observer in the fi-region 0 < r < ra. A static observer in the fi-region rb < r < rc observes T-ra < r < rb mass is limited within
Mcr1 < M < Mcr2. The value M = Mcri corresponds to a double-horizon (ra = rb) state which appears as an end-point of the Hawking evaporation. For M < Mcr1 the metric (6) describes a G-lump in asymptotically de Sitter space (the upper curve in
Mcr2 rb = rc
represents a regular modification of the Nariai solution.
This behavior is generic for the class of regular solutions specified by (3) and satisfying the weak energy condition [7. 9]. The pictures are plotted with the density-profile [4]
p(r) =Po exP( —'"3/''"o'rs); ro = y/Z/8*Gpo; p0 = p(r 0) = (SttG^A- rg = 2GM (9)
which describes vacuum polarization effects leading to de Sitter interior in the simple semi-classical model for vacuum polarization in the gravitational field [11].
2. Regular cosmologies with vacuum dark energy
In the coordinates of comoving observers, the metric (C) describes regular vacuum dominated cosmologies (vacuum density evolves smoothly from a big initial value to
(8)
0
Fig. 2. Metric function for double-liorizon and one-horizon configurations
g(r)=1-Rrn. 3r2
Lemaitre observer
r = 0
r = 0
Fig. 3. Spherically symmetric vacuum space-time wit.li one horizon
a small value) of the Lemaitre class arid Ivantowski Sachs type whose dynamics depends on the number of horizons.
In the vacuum cosmologies of the Lemaitre class, evolution starts from a nonsingular non-simultaneous de Sitter bang followed by an anisotropic stage at which most of the mass is produced [25]. For cosmologies of Ivantowski Sachs type, evolution starts with a null bang from a horizon, but information about pre-bang history is available for KS observes [9].
Two simplest cases of one-horizon configurations are shown in Fig. 3: the global structure of space-time is the same as for de Sitter geometry but with dynamical vacuum dark energy.
In the Lemaitre coordinates this configuration represents vacuum anisotropic models of the Lemaitre class, in which evolution starts with a nonsingular non-simultaneous de Sitter bang from the regular time-like surface r(R, t) = 0 for the model with zero and negative spatial curvature, and from r = r for the models with the positive spatial curvature [9].
In the Ivantowski Sachs region it corresponds to the class of regular homogeneous T-models with vacuum dark energy [26] .Typical features of homogeneous regular T-models are: the existence of a Killing horizon: beginning of the cosmological evolution from a null bang at the horizon: the existence of a regular static pre-bang region visible to cosmological observers: creation of matter from anisotropic vacuum, accompanied by very rapid isotropization. Detailed calculations of the spherically symmetric regular T
T
constraints [26].
r = oo
In quantum cosmology it is possible, in frame of the minisnperspace model, to adapt cosmological constant A for description of a vacuum dark energy density jumping from the big initial valne to the small valne suggested by observations [27]. The gange-non-invariance of quantum cosmology leads to a connection between a choice of the gange and quantum spectrum for a certain physical quantity which can be specified in the framework of the minisnperspace model. There exists a particular gange in which the
AA one can find its small valne with the biggest probability, while at the beginning of the evolution, the biggest probability corresponds to its biggest valne. Transitions between
A
to several scales of symmetry breaking [27].
3. Dark matter candidates
3.1. Regular black hole remnants. The quantum temperature of a horizon rh determined by its surface gravity Kh is given by the Gibbons - Hawking formula:
kTh = ^-Kh = -£-\g'(rh)\. (10)
In space-time with three horizons, an observer in the fi-region rb < r < rc can detect the Hawking radiation from a black hole horizon rb and from a cosmological horizon rc, and an observer in the fl-region 0 < r < ra can detect radiation from the cosmological horizon ra.
Thermodynamics is studied by applying the Padmanabhan approach relevant for a mnltihorizon space with non-zero pressure and based on a canonical ensemble of metrics (6) at the constant temperature of the horizon determined by the periodicity of the Euclidean time in the Euclidean continuation of the Einstein action [28]. With this approach we find temperature Th, thermodynamical energy Eh, entropy Sh, free energy Fh, and specific heat written below in the units c = G = h =1 [12]:
on black hoi horizon
kTb = ^ ~ 8Kp(rb)rb^j ; Eb =
(11)
on internal and cosmological horizons
j- (8?Tp(rh)rh + ,n , , -n -
V 3 vh) 2
Sh = 4nrh; Fh = Eh - ThSh; (13)
kTh = U*p{rh)rh + Eh = -\rh; (12)
on any horizon
Ch — dEh/dTh] Ch '
1
27T
8Tvp'(rh)rh+8Tvp(rh)+X+^
(14)
Dependence of temperature on the black hole horizon radius is shown in Fig. 4.
Fig. 4 is plotted with the density profile (9), but this enrve is generic. Independent of a particular form of the density profile p(r), Tb ^ 0 as ra ^ rb, and as rc ^ rb, since surface gravity vanishes in the extrema of the metric function g(r). Hence the temperature curve should have a maximum, Tb(rm) = Tb max. It follows that specific heat on the black hole horizon Cb is negative for r > rm and positive for r < rm. At the maximum C-1 = 0, hence a specific heat is broken and changes its sign in the course of quantum evaporation [11, 12]. For the case of the density profile (9), maximal
Tb(r)
05
3.0
2.5
20
1.5
1.0
r
0.2
0.3
0.4
0.5
Fig. 4. Temperature of a regular black hole in do Sitter space
temperature corresponding to the phase transition is Tb max = Ttr — 0.2Tpi \Jpo/ppi ■ For po = pgut and Mgut - 1015 GeV it gives Tir - 0.2 • 1011GeV.
The answer to the question what is an endpoint of evaporation, depends on where move horizons. For a metric function (7) with de Sitter asymptotics at the center and Kottler - Trefftz asymptotics for r ^ r* = (r2 rg )1/3, a density profile involves scaling r/r*, and for zeros of a metric function (7) we obtain drb/dM > 0, dra/dM < 0, drc/dM < 0. In the region 0 < r < ra, which is the whole manifold for a static observer, dra > 0 by the second law of thermodynamics for horizons. The horizon ra moves outwards and dra/dM < 0, hence M decreases; since drb/dM > 0, a black hole horizon rb shrinks. Specific heat Ca is positive near the double horizon, dTa/dEa > 0 and dTa/dra < 0, hence Ta decreases with increasing ra. With dTa/dM > 0 and dTa/dra < 0 this leads to monotonic de creasing M and Ta unti 1 Ta vanishes on the double horizon ra = rb = rd where Cd > 0 [12].
The specific heat C-1 can be written as
This formula tells unambiguously that an extreme state with a double horizon (g' = 0) is thermodynamically stable when it appears in a minimum of the metric function g(r), and thermodynamically unstable when it appears in its maximum [12]. We conclude that a regular black hole leaves behind a thermodynamically stable double-horizon remnant. For the case of the density profile (9), its mass
is Mremnant - 0.3Mpi \/pPl/p0.
3.2. Vacuum gravitational soiitons — G-lumps. This name is owing to Coleman's lumps which are non-singular non-dissipative solutions of finite energy holding themselves together by their own self-interaction [29]. The idea of lumps can be traced back to the Einstein idea to describe an elementary particle by a regular solution of nonlinear field equations as a ''bunched field" located in the confined region where field and energy are particularly high [30]. Vacuum soliton G-lump was proposed in 1996 in a model-independent way as a regular solution to the Einstein equations with the de Sitter interior without horizons [11]. In terms of the proposed in 2001 gravastar model
G
continuous density and pressures.
G
(15)
r(p± + p)' < P + (p± + p)
is satisfied for a wide class of density profiles.
Fig. 5. Potential VY(r) for G-lump with rg/r0 = 1.5 (L = 4)
In the field of G-lump and of the double-horizon remnant, there exist nontrivial geodesic orbits [32] which can be used in search for their observational signatures as dark matter candidates. Geodesies are described by
/dr\2 /L2\ T2
(^J +Vu>n)(r)=E2; + V7(r) = -g(r), (17)
where a is the afiine parameter along geodesic, Vp is the potential for time-like geodesies, and VY for the null geodesies. For a G-lump and extreme black hole the potential curves differ essentially from that for a black hole and evidently depend on the mass M. Potentials Vp have, in a certain range of masses, three extrema and, hence, two branches of stable circular orbits separated by a gap. Potential VY shown in Fig. 5
G
stable bound photon orbits including circular orbits!
3.3. Electromagnetic soliton. Nonlinear electrodynamics coupled to gravity is described by the action
s=ihJ d4x^(R -LF = FikF'lk (18)
with an arbitrary gauge invariant lagrangian L(F) with the Maxwellian asymptotics in the weak field regime. A stress-energy tensor of a spherically symmetric electromagnetic field has the symmetry (3). For a field satisfying the weak energy condition a spherically symmetric electrically charged electrovacuum structure has obligatory de Sitter center in which the electric field vanishes while the energy density of electromagnetic vacuum achieves its maximal value [22]. By the Gurses-Gursey algorithm based on the Trautman Newman technique [33], spherically symmetric electrovacuum solution is transformed into a spinning electrovacuum solution asymptotically Kerr Newman for a distant observer. De Sitter center becomes de Sitter equatorial disk which has both perfect conductor and ideal diamagnetic properties and displays superconducting behavior within a single spinning soliton. This behavior is generic for the class of regular spinning solutions describing electrovacuum black holes and solitons [23]. De Sitter vacuum supplies a particle with the finite positive electromagnetic mass related to breaking of space-time symmetry. These results apply to the cases when the energy-scale is less than the Planck scale. Recently they found a certain confirmation in the existence of minimal length scale (''closest approach" of particles) in the annihilation reaction e+e- ^ 77(7), which can be explained by the existence of the characteristic
surface at which electromagnetic attraction is balanced by the gravitational repulsion due to de Sitter interior [34].
This work was supported by the Polish Ministry of Science and Education for the research project ''Globally regular configurations in General Relativity including classical and quantum cosmological models, black holes and particle-like structures (solitons)" in the frame of the ''Polish-Russian Agreement for collaboration in the Field of Science and Technology."
Резюме
И. Дъшиикооа. Классификация Петрова и темная вакуумная жидкость. Классификация Петрова тензоров эпергии-импульса позволяет ввести объединённое описание тёмной энергии и тёмной материи как вакуумной тёмной жидкости па основе симметрии прострапства-времепи. При таком подходе вакуумная тёмная энергия описывается переменным космологическим членом, симметрия которого нарушена по сравнению с космологическим членом Эйнштейна. В случае сферической симметрии инфляционное уравнение состояния выполняется только для радиального давления, в результате плотность энергии и оба давления становятся зависящими от времени и пространственных координат. Уравнения Эйнштейна с правой частью, представленной тензором эпергии-импульса такого типа, допускает также класс решений, описывающих компактные объекты с центром де Ситтера: регулярные чёрные дыры, продукты их испарения и вакуумные гравитационные солитопы, которые могут ответственными за наблюдательные эффекты, свидетельствующие о существовании тёмной материи. Масса объектов с де Ситтеров-ским ядром связана с тёмной энергией и нарушением симметрии прострапства-времепи от группы де Ситтера в центре до группы Пуанкаре па бесконечности для асимптотически плоских пространств или до группы де Ситтера с меньшим значением космологической постоянной для асимптотически де Ситтеровских па бесконечности пространств.
Ключевые слова: тёмная энергия, тёмная материя, регулярные объекты с де Сит-теровским ядром.
References
1. Anderson P.R. Attractor states and infrared scaling in de Sitter space // Phys. Rev. D. -2000. - V. 62, No 12. - P. 124019-1-124019-24.
2. Kirsten K., Garriga J. Massless minimally coupled fields in de Sitter space: O(4)-symmetric states versus de Sitter invariant vacuum // Phys. Rev. D. - 1993. - V. 48, No 2. - P. 567-577.
3. Gliner E.B. Algebraic properties of the energy-momentum tensor and vacuum-like // Sov. Phys. JETP. - 1966. - V. 22, No 2. - P. 378-383.
4. Dymnikova I. Vacuum nonsingular black hole // Gen. Rel. Grav. - 1992. - V. 24, No 3. -P. 235-242.
5. Dymnikova I. The algebraic structure of a cosmological term in spherically symmetric solutions // Phys. Lett. B. - 2000. - V. 472, No 1-2. - P. 33-38.
6. Dymnikova I., Galaktionov E. Vacuum dark fluid // Phys. Lett. B. - 2007. - V. 645, No 4. - P. 358-364.
7. Dymnikova I. The cosmological term as a source of mass // Class. Quant. Grav. - 2002. -V. 19, No 4. - P. 725-739.
8. Copeland E.J. Models of Dark Energy // AIP Conf. Proc. - 2010. - V. 1241. - P. 125-131.
9. Bronnikov K.A., Dobosz A., Dymnikova I. Nonsingular vacuum cosmologies with a variable cosmological term // Class. Quant. Grav. - 2003. - V. 20, No 16. - P. 3797-3814.
10. Dymnikova I., Soltysek B. Spherically Symmetric Space-Time with Two Cosmological Constants // Gen. Rel. Grav. - 1998. - V. 30, No 12. - P. 1775-1793.
11. Dymnikova I. De Sitter - Schwarzschild black hole: its particlelike core and thermody-namical properties // Int. J. Mod. Phys. D. - 1996. - V. 5, No 5. - P. 529-540.
12. Dymnikova I., Korpusik M. Regular black hole remnants in de Sitter space // Phys. Lett. B. - 2010. - V. 685, No 1. - P. 12-18.
13. Dymnikova I., Galaktionov E. Stability of a vacuum non-singular black hole // Class. Quant. Grav. - 2005. - V. 22, No 12. - P. 2331-2357.
14. Bergström L. Dark Matter Candidates // AIP Conf. Proc. - 2010. - V. 1241. - P. 49-63.
15. Olive K.A. Dark Energy and Dark Matter. - arXiv:1001.5014v1 [hep-ph]. - 2010. - 12 p. -URL: http://arxiv.org/pdf/1001.5014v1.pdf.
16. Böhmer C. G., Harko T. Does the cosmological constant imply the existence of a minimum mass? // Phys. Lett. B. - 2005. - V. 630, No 3-4. - P. 73-77.
17. Arbey A. Dark fluid: A complex scalar field to unify dark energy and dark matter // Phys. Rev. D. - 2006. - V. 74, No 4. - P. 043516-1-043516-7.
18. Ellis J. Dark matter and dark energy: summary and future directions // Phil. Trans. R. Soc. Lond. A . - 2003. - V. 361. - P. 2607-2627.
19. MacGibbon J.H. Can Planck-mass relics of evaporating black holes close the Universe? // Nature. - 1987. - V. 329. - P. 308-309.
20. Dymnikova I. Regular Black Hole Remnants // AIP Conf. Proc. - 2010. - V. 1241. -P. 361-368.
21. Ahluwalia D.V., Dymnikova I. A theoretical case for negative mass-square for sub-eV particles // Int. J. Mod. Phys. D. - 2003. - V. 12, No 9. - P. 1787-1794.
22. Dymnikova I. Regular electrically charged vacuum structures with de Sitter centre in nonlinear electrodynamics coupled to general relativity // Class. Quant. Grav. - 2004. -V. 21, No 18. - P. 4417-4428.
23. Dymnikova I. Spinning superconducting electrovacuum soliton // Phys. Lett. B. - 2006. -V. 639, No 3-4. - P. 368-372.
24. Landau L.D., Lifshitz E.M. The classical theory of fields. - Oxford: Pergamon Press, 1975. - 402 p.
25. Dymnikova I., Dobosz A., Filchenkov M., Gromov A. Universes inside a black hole // Phys. Lett. B. - 2001. - V. 506, No 3-4. - P. 351-361.
26. Bronnikov K., Dymnikova I. Regular homogeneous T-models with vacuum dark fluid // Class. Quant. Grav. - 2007. - V. 24, No 23. - P. 5803-5817.
27. Dymnikova I., M. Fil'chenkov Gauge-noninvariance of quantum cosmology and vacuum dark energy // Phys. Lett. B. - 2006. - V. 635, No 4. - P. 181-185.
28. Padmanabhan T. Classical and quantum thermodynamics of horizons in spherically symmetric spacetimes // Class. Quant. Grav. - 2002. - V. 19, No 21. - P. 5387-5408.
29. Coleman S. Classical Lumps and Their Quantum Descendants // New Phenomena in Subnuclear Physics / Ed. A. Zichichi. - N. Y.: Plenum Press, 1977. - P. 297-421.
30. Einstein A. On the Generalized Theory of Gravitation // Sci. Amer. - 1952. - V. 182, No 4. - P. 13-17.
31. Mazur P. O., Mottola E. Gravitational Condensate Stars: An Alternative to Black Holes. -arXiv:gr-qc/0109035v5. - 2002. - 4 p. - URL: http://arxiv.org/pdf/gr-qc/0109035v5.pdf.
32. Dymnikova I., Poszwa A., Soltysek B. Geodesic Portrait of de Sitter - Schwarzschild Spacetime // Grav. Cosmol. - 2008. - V. 14, No 3. - P. 262-275.
33. Gurses M., G'iirsey F. Lorentz covariant treatment of the Kerr-Schild geometry // J. Math. Phys. - 1975. - V. 16, No 12. - P. 2385-2390.
34. Dymnikova I., Sakharov A., Ulbricht J. Minimal Length Scale in Annihilation. -arXiv:0907.0629v1 [hep-ph]. - 2009. - 16 p. - URL: http://arxiv.org/pdf/0907.0629v1.pdf.
Поступила в редакцию 22.11.10
Dymnikova, Irina Gavriilovna Doctor of Physics and Mathematics, Professor, Department of Mathematics and Computer Science, University of Warmia and Mazury, Olsztyn, Poland: Professor, Leading Researcher, A.F. Ioffe Pliysico-Technical Institute, Saint Petersburg, Russia.
Дымникова Ирина Гаврииловна доктор физико-математических паук, профессор факультета математики и информатики Вармипско-Мазурского университета, г. Оль-штып, Польша: профессор, ведущий паучпый сотрудник Физико-технического института им. А.Ф. Иоффе, г. Санкт-Петербург, Россия.
E-mail: irinaOuunn.edu.pl
