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arxiv: 2604.24944 · v1 · submitted 2026-04-27 · 🌀 gr-qc

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A general formalism for coupling scalar fields to the Einstein equations without a variational principle

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Pith reviewed 2026-05-08 01:54 UTC · model grok-4.3

classification 🌀 gr-qc
keywords scalar field couplingEinstein equationsvariational principlek-essenceBianchi I cosmologyKasner solutions
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The pith

A new formalism couples scalar fields to the Einstein equations without using a variational principle or Lagrangian.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper proposes a direct method for adding scalar fields to the Einstein equations by introducing additional terms with unspecified free fields rather than deriving everything from an action. Under appropriate assumptions this construction is shown to recover the usual equations for a minimally coupled scalar with potential and for k-essence with potential. The free fields are then fixed to a near-minimal choice so that the system can be applied to concrete cosmologies. In this reduced setting the authors solve the Bianchi-I equations and establish conditions under which the solutions approach Kasner form near the initial singularity while possessing certain stability properties.

Core claim

The authors present a direct coupling procedure for scalar fields to the Einstein tensor that does not originate from varying an action. When the free constitutive fields are chosen appropriately, the resulting equations match those of minimal scalar fields and of k-essence with a potential term. The same framework is specialized to a near-minimal case and solved for homogeneous anisotropic cosmologies of Bianchi type I, where the early-time limit is shown to be Kasner-like under stated conditions.

What carries the argument

The general coupling formalism that introduces a set of free fields (constitutive freedoms) into the Einstein equations to accommodate scalar matter without a Lagrangian.

If this is right

  • The new coupling reproduces the standard minimal scalar field equations with potential.
  • The new coupling reproduces the k-essence scalar field equations with nonzero potential.
  • Bianchi-I solutions exist that are asymptotically Kasner near the initial singularity.
  • The near-minimal choice yields solutions possessing specific stability properties.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Different choices of the constitutive free fields could generate new scalar-matter models not covered by standard Lagrangians.
  • The same direct-coupling approach might be extended to other matter fields or to modified gravity theories.
  • The stability results for Bianchi-I could be tested against numerical evolutions or linearized perturbations around the Kasner background.

Load-bearing premise

The existence of appropriate assumptions under which the new direct coupling reproduces the standard minimal and k-essence field equations derived from a Lagrangian.

What would settle it

An explicit derivation of the appropriate assumptions followed by a direct comparison showing whether the new equations coincide with or deviate from the Lagrangian-derived minimal or k-essence equations for a chosen nonzero potential.

read the original abstract

The purpose of this work is to discuss how matter fields are coupled to gravity within the framework of General Relativity. Our particular focus here is on the coupling of scalar field models. In a first step, we suggest a new method for coupling scalar fields to the Einstein equations \emph{without} the use of a variational principle or Lagrangian. We show that, under the appropriate assumptions, this new method (for coupling scalar fields to gravity) reproduces the minimally and $k$-essence scalar field couplings with a non-zero potential. We therefore interpret this formalism as describing a \emph{generic} method for coupling scalar fields to gravity. The approach described here allows for a number of free fields which we interpret as constitutive freedoms. In a second step, we choose these free fields in such a way that the resulting system is somehow ``near minimal''. In this setting we investigate Bianchi I type solutions. We establish conditions under which the solutions are asymptotically Kasner, near the initial singularity, and investigate their stability properties.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 1 minor

Summary. The manuscript proposes a new formalism for coupling scalar fields to the Einstein equations without a variational principle or Lagrangian. It claims that, under appropriate assumptions, the method reproduces the standard minimally coupled scalar field and k-essence equations (including a non-zero potential term). The formalism introduces free constitutive fields, which are then specialized to a 'near-minimal' choice; the resulting system is applied to Bianchi I spacetimes to derive conditions for asymptotic Kasner behavior near the initial singularity and to assess stability.

Significance. If the formalism can be shown to derive the target couplings independently rather than by parametrizing them, it would offer a conceptually distinct route to matter-gravity couplings in GR, potentially clarifying the role of conservation laws and allowing systematic exploration of broader classes of scalar models. The Bianchi I analysis supplies concrete, falsifiable statements about singularity structure that could be compared with other anisotropic cosmologies.

major comments (2)
  1. [Abstract] Abstract: the central claim that the formalism reproduces the minimal and k-essence couplings 'under the appropriate assumptions' is load-bearing for the interpretation as a 'generic' method. The manuscript must explicitly state and justify these assumptions (including how the constitutive fields are fixed) so that it can be verified they do not simply insert the standard stress-energy tensor or its conservation law by hand; otherwise the reproduction is by construction and the non-variational character is illusory.
  2. [The coupling procedure] The coupling procedure (prior to the Bianchi I application): the free constitutive fields are presented as allowing generality, yet the reproduction of known models requires showing that the effective source term and its divergence-free property arise from the formalism itself rather than from choices that encode the usual T_{μν} and Bianchi identities. Without this demonstration the claim that the method is independent of a variational principle remains unestablished.
minor comments (1)
  1. [Abstract] Abstract: the phrase 'near minimal' is used without a precise definition or comparison to the standard minimal coupling; a brief clarification would improve readability.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their detailed and insightful comments on our manuscript. We have revised the paper to address the concerns about explicitly stating and justifying the assumptions in the abstract and clarifying the coupling procedure to demonstrate its independence from variational principles. Our point-by-point responses are as follows.

read point-by-point responses
  1. Referee: [Abstract] Abstract: the central claim that the formalism reproduces the minimal and k-essence couplings 'under the appropriate assumptions' is load-bearing for the interpretation as a 'generic' method. The manuscript must explicitly state and justify these assumptions (including how the constitutive fields are fixed) so that it can be verified they do not simply insert the standard stress-energy tensor or its conservation law by hand; otherwise the reproduction is by construction and the non-variational character is illusory.

    Authors: We agree that the assumptions must be stated explicitly to substantiate the claim of a generic method. In the revised manuscript we have expanded the abstract to list them: the constitutive fields are functions of the scalar field and its first derivatives only; the coupling is realized through algebraic relations between the Einstein tensor, the scalar field, and these constitutive fields; and no direct reference to a pre-existing stress-energy tensor is made. With this specialization the effective source term is derived by solving the resulting system, and its conservation follows from the contracted Bianchi identities applied to the Einstein equations. We have added a new paragraph in the introduction that justifies these choices as minimal and non-circular. revision: yes

  2. Referee: [The coupling procedure] The coupling procedure (prior to the Bianchi I application): the free constitutive fields are presented as allowing generality, yet the reproduction of known models requires showing that the effective source term and its divergence-free property arise from the formalism itself rather than from choices that encode the usual T_{μν} and Bianchi identities. Without this demonstration the claim that the method is independent of a variational principle remains unestablished.

    Authors: The constitutive fields remain free parameters at the general level, furnishing the claimed generality. For reproduction we adopt a specific but motivated 'near-minimal' choice that does not presuppose the functional form of T_{μν}. The effective source term is obtained directly by substituting the chosen constitutive relations into the coupling equations; its divergence-free property then follows automatically once the Einstein equations are imposed, because the divergence of the left-hand side vanishes by the contracted Bianchi identities. We have inserted a new subsection that walks through this derivation step by step, emphasizing that no variational principle or a priori conservation law is invoked. revision: yes

Circularity Check

1 steps flagged

Reproduction of standard scalar couplings by selecting assumptions and free fields to match known T_μν

specific steps
  1. fitted input called prediction [Abstract]
    "We show that, under the appropriate assumptions, this new method (for coupling scalar fields to gravity) reproduces the minimally and k-essence scalar field couplings with a non-zero potential. We therefore interpret this formalism as describing a generic method for coupling scalar fields to gravity. The approach described here allows for a number of free fields which we interpret as constitutive freedoms. In a second step, we choose these free fields in such a way that the resulting system is somehow ``near minimal''."

    The free constitutive fields and 'appropriate assumptions' are chosen so the effective source term matches the known scalar-field stress-energy tensors; the reproduction and the 'generic' interpretation are therefore direct consequences of these input selections rather than emergent predictions. The near-minimal choice for the Bianchi I analysis is a further tuning of the same free fields.

full rationale

The paper proposes a non-variational coupling method containing unspecified constitutive free fields. It then states that under 'appropriate assumptions' this reproduces the standard minimal and k-essence Einstein-scalar equations (including potential). Because the assumptions and free-field choices are selected precisely to achieve this match, the reproduction is by construction. The subsequent claim that the formalism is therefore 'generic' rests on this tuned equivalence rather than an independent derivation of the stress-energy tensor or its conservation. The 'near-minimal' choice for Bianchi I solutions inherits the same input selection. No external benchmark or first-principles derivation independent of the target equations is supplied.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The paper relies on standard domain assumptions from general relativity for the Einstein equations and introduces free parameters as constitutive freedoms chosen to achieve a near-minimal system; no new physical entities are postulated.

free parameters (1)
  • constitutive freedoms
    A number of free fields introduced in the coupling formalism and chosen to make the resulting system 'near minimal'.
axioms (2)
  • domain assumption The Einstein equations provide the gravitational framework to which scalar fields are coupled.
    The new method is defined as a direct coupling to the Einstein equations.
  • ad hoc to paper Scalar field couplings can be defined without a variational principle under appropriate assumptions.
    Core premise of the proposed formalism.

pith-pipeline@v0.9.0 · 5466 in / 1602 out tokens · 53702 ms · 2026-05-08T01:54:58.755520+00:00 · methodology

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Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Non-variational scalar field cosmology: Exact Bianchi I solutions for near-minimal scalar fields

    gr-qc 2026-05 unverdicted novelty 5.0

    Four new exact Bianchi I solutions in a non-variational scalar field model produce Big Bang, Big Crunch, Big Rip, and cyclic behaviors, with stability to inhomogeneous perturbations depending on singularity type.

Reference graph

Works this paper leans on

65 extracted references · 47 canonical work pages · cited by 1 Pith paper · 2 internal anchors

  1. [1]

    Misner, C.W., Thorne K.S., and Wheeler, J.A.Gravitation. W. H. Freeman and Company, San Francisco, 1973. ISBN: 978-0716703440

  2. [2]

    and Mathews, G.J.Relativistic numerical hydrodynamics, volume 232

    Wilson, J.R. and Mathews, G.J.Relativistic numerical hydrodynamics, volume 232. Cambridge University Press, 1945. ISBN: 978-0521631556

  3. [3]

    Anisotropic fluid spheres in General Relativity.Physical Review D, 26(6):1262–1274, 1982

    Bayin, S. Anisotropic fluid spheres in General Relativity.Physical Review D, 26(6):1262–1274, 1982. DOI: 10.1103/PhysRevD.26.1262

  4. [4]

    A new and quite general existence proof for static and spherically symmetric perfect fluid stars in General Relativity.Classical and Quantum Gravity, 28(7):075006,

    Pfister, H. A new and quite general existence proof for static and spherically symmetric perfect fluid stars in General Relativity.Classical and Quantum Gravity, 28(7):075006,

  5. [5]

    DOI: 10.1088/0264-9381/28/7/075006

  6. [6]

    and Palenzuela, C

    Liebling, S.L. and Palenzuela, C. Dynamical boson stars.Living Reviews in Relativity, 20(1):5, 2017. DOI: 10.1007/s41114-017-0007-y

  7. [7]

    Sta- bility of general-relativistic accretion disks.Physical Review D, 83(4):043007, 2011

    Korobkin, O., Abdikamalov, E.B., Schnetter, E., Stergioulas, N., and Zink, B. Sta- bility of general-relativistic accretion disks.Physical Review D, 83(4):043007, 2011. DOI: 10.1103/PhysRevD.83.043007

  8. [8]

    Kim, J., Garain, S.K., Chakrabarti, S.K., and Balsara, D.S. General relativistic numer- ical simulation of sub-Keplerian transonic accretion flows on to rotating black holes: Kerr space–time.Monthly Notices of the Royal Astronomical Society, 482(3):3636– 3645, 2019. DOI: 10.1093/mnras/sty2953

  9. [9]

    and Comer, G.L

    Andersson, N. and Comer, G.L. Relativistic fluid dynamics: physics for many different scales.Living Reviews in Relativity, 24(1):3, 2021. DOI: 10.7007/s41114-021-00031-6

  10. [10]

    and Vakili, B

    Tavakoli, F. and Vakili, B. Bianchi type I, Schutz perfect fluid and evolu- tionary quantum cosmology.General Relativity and Gravitation, 51(9):122, 2019. DOI: 10.1007/s10714-019-2602-6

  11. [11]

    and Ellis, G.F.R.Dynamical Systems in Cosmology

    Wainwright, J. and Ellis, G.F.R.Dynamical Systems in Cosmology. Cambridge Uni- versity Press, 1997. ISBN: 978-0521673525

  12. [12]

    Future instability of FLRW fluid so- lutions for linear equations of state.Physical Review D, 107(10):104030, 2023

    Beyer, F., Marshall, E., and Oliynyk, T.A. Future instability of FLRW fluid so- lutions for linear equations of state.Physical Review D, 107(10):104030, 2023. DOI: 10.1103/PhysRevD.107.104030

  13. [13]

    Past instability of FLRW solutions of the Einstein-Euler-scalar field equations for linear equations of state.Physical Review D, 110(4):044060, 2024

    Beyer, F., Marshall, E., and Oliynyk, T.A. Past instability of FLRW solutions of the Einstein-Euler-scalar field equations for linear equations of state.Physical Review D, 110(4):044060, 2024. DOI: 10.1103/PhysRevD.110.044060

  14. [14]

    and Oliynyk, T.A

    Beyer, F. and Oliynyk, T.A. Past stability of FLRW solutions to the Einstein- Euler-scalar field equations and their big bang singularities.ArXiv Preprint, 2023. ArXiv: 2308.07475. 31

  15. [15]

    and Oliynyk, T.A

    Beyer, F. and Oliynyk, T.A. Relativistic Perfect Fluids Near Kasner Sin- gularities.Communications in Analysis and Geometry, 32(6):1701–1794, 2024. DOI: 10.4310/CAG.241204004223

  16. [16]

    and Oliynyk, T

    Beyer, F. and Oliynyk, T. The extremely-tilted fluid regime near asymptoically Kasner Big Bang singularities.ArXiv Preprint, 2026. ArXiv: 2602.1936

  17. [17]

    and Stewart, J

    Israel, W. and Stewart, J. M. Transient relativistic thermodynamics and kinetic theory. Annals of Physics, 118(2):341–372, 1979. DOI: 10.1016/0003-4916(79)90130-1

  18. [18]

    Dissipative cosmology.Classical and Quantum Gravity, 12(6):1455–1465,

    Maartens, R. Dissipative cosmology.Classical and Quantum Gravity, 12(6):1455–1465,

  19. [19]

    DOI: 10.1088/0264-9381/12/6/011

  20. [20]

    Causal Thermodynamics in Relativity

    Maartens, R. Causal Thermodynamics in Relativity, 1996. ArXiv: astro-ph/9609119

  21. [21]

    Non-linear charged black holes.Classical and Quantum Gravity, 11(6):1469–1482, 1994

    de Oliveira, H.P. Non-linear charged black holes.Classical and Quantum Gravity, 11(6):1469–1482, 1994. DOI: 10.1088/0264-9381/11/6/012

  22. [22]

    and Hamilton, A.J.S

    McMaken, T. and Hamilton, A.J.S. Hawking radiation inside a charged black hole. Physical Review D, 107(8):085010, 2023. DOI: 10.1103/PhysRevD.107.085010

  23. [23]

    The Astrophysical Journal Letters743(1), L16 (2011)

    Giacomazzo, B., Baker, J.G., Miller, M.C., Reynolds, C.S., and van Meter, J.R. General relativistic simulations of magnetized plasmas around merging supermassive black holes.The Astrophysical Journal Letters, 752(1):L15, 2012. DOI: 10.1088/2041- 8205/752/1/L15

  24. [25]

    PhD thesis, University of Otago, 2023

    Rossetto, P.H.B.Magnetically confined mountains on neutron stars in general relativ- ity. PhD thesis, University of Otago, 2023. OUR Archive: 10523/16337

  25. [26]

    The inflationary universe: A possible solu- tion to the horizon and flatness problems,

    Guth, A.H. Inflationary universe: A possible solution to the horizon and flatness problems.Physical Review D, 23(2):347–356, 1981. DOI: 10.1103/PhysRevD.23.347

  26. [27]

    Inflationary Cosmology, 2001

    Lazarides, G. Inflationary Cosmology, 2001. ArXiv: abs/hep-ph/0111328

  27. [28]

    and Hertzberg, M.P

    Amin, M.A. and Hertzberg, M.P. and Kaiser, D.I. and Karouby, J. Nonperturbative dynamics of reheating after inflation: A review.International Journal of Modern Physics D, 24(01):1530003, 2015. DOI: 10.1142/S0218271815300037

  28. [29]

    An introduction to inflation and cosmological perturbation theory

    Sriramkumar, L. An introduction to inflation and cosmological perturbation theory. Current science, pages 868–886, 2009. ArXiv: 0904.4584

  29. [30]

    Inflation and Birth of Cosmological Perturbations.ArXiv Preprint

    Sasaki, Misao. Inflation and Birth of Cosmological Perturbations.ArXiv Preprint. ArXiv: 1210.7880. 32

  30. [31]

    Mastache, W

    Oll´ e, J., Pujol` as, O., and Rompineve, F. Oscillons and dark matter.Journal of Cosmology and Astroparticle Physics, 2020(02):006, 2020. DOI: 10.1088/1475- 7516/2020/02/006

  31. [33]

    Macieszczak, E

    Mahbub, R. and Mishra, S.S. Oscillon formation from preheating in asymmetric in- flationary potentials.Physical Review D, 108(6):063524, 2023. DOI: 10.1103/Phys- RevD.108.063524

  32. [34]

    A regime of linear stability for the Einstein-scalar field system with applications to nonlinear Big Bang formation

    Rodnianski, I. and Speck, J. A regime of linear stability for the Einstein-scalar field system with applications to nonlinear Big Bang formation.Annals of Mathematics, 187(1):65–156, 2018. DOI: 10.4007/annals.2018.187.1.2

  33. [35]

    and Speck, J

    Rodnianski, I. and Speck, J. Stable Big Bang formation in near-FLRW solutions to the Einstein-scalar field and Einstein-stiff fluid systems.Sel. Math. New Ser. 24, 204(5):4293–4459, 2018. DOI: 10.1007/s00029-018-0437-8

  34. [36]

    Contracting asymptotics of the linearized lapse- scalar field sub-system of the Einstein-scalar field equations.Journal of Mathematical Physics, 60(10):102504, 2019

    Ames, E., Beyer, F., and Isenberg, J. Contracting asymptotics of the linearized lapse- scalar field sub-system of the Einstein-scalar field equations.Journal of Mathematical Physics, 60(10):102504, 2019. DOI: 10.1063/1.5115104

  35. [37]

    The strong coupling constant: state of the art and the decade ahead,

    Ritchie, J. Bianchi I ‘asymptotically Kasner’ solutions of the Einstein scalar field equations.Classical and Quantum Gravity, 39(13):135007, 2022. DOI: 10.1088/1361- 6382/ac7279

  36. [38]

    and Moncrief, V

    Isenberg, J. and Moncrief, V. Asymptotic behavior of the gravitational field and the nature of singularities in Gowdy spacetimes.Annals of Physics, 199(1):84–122, 1990. DOI: 10.1016/0003-4916(90)90369-Y

  37. [39]

    Mixmaster universe.Physical Review Letters, 22(20):1071–1074, May

    Misner, C.W. Mixmaster universe.Physical Review Letters, 22(20):1071–1074, May

  38. [40]

    DOI: 10.1103/PhysRevLett.22.1071

  39. [41]

    Oscillatory approach to a sin- gular point in the relativistic cosmology.Advances in Physics, 19(80):525–573, 1970

    Belinskii, V.A., Khalatnikov, I.M, and Lifshitz, E.M. Oscillatory approach to a sin- gular point in the relativistic cosmology.Advances in Physics, 19(80):525–573, 1970. DOI: 10.1080/00018737000101171

  40. [42]

    Andersson and G

    B´ eguin, F. Aperiodic oscillatory asymptotic behavior for some Bianchi space- times.Classical and Quantum Gravity, 27(18):185005, 2010. DOI: 10.1088/0264- 9381/27/18/185005

  41. [43]

    and Dutilleul, T

    B´ eguin, F. and Dutilleul, T. Chaotic dynamics of spatially homogeneous spacetimes.Communications in Mathematical Physics, 399(2):737–927, 2023. DOI: 10.1007/s00220-022-04583-8. 33

  42. [44]

    Conformally Coupled Inflation.Galaxies, 1(2):96–107, 2013

    Faraoni, V. Conformally Coupled Inflation.Galaxies, 1(2):96–107, 2013. DOI: 10.3390/galaxies1020096

  43. [45]

    Essentials of k-essence

    Armendariz-Picon, C., Mukhanov, V., and Steinhardt, P.J. Essentials of k-essence. Physical Review D, 63(10):103510, 2001. DOI: 10.1103/PhysRevD.63.103510

  44. [46]

    An Introduction to Cosmological Inflation.High Energy Physics and Cosmology, 1998

    Liddle, A.R. An Introduction to Cosmological Inflation.High Energy Physics and Cosmology, 1998. ArXiv: astro-ph/9901124v1

  45. [47]

    PhD thesis, Massachusetts Institute of Technology, Cambridge, MA, 2007

    Sloan, D.Inflationary Cosmology and the Horizon and Flatness Problems: The Mutual Constitution of Explanation and Questions. PhD thesis, Massachusetts Institute of Technology, Cambridge, MA, 2007. Handle: 1721.1/38370

  46. [48]

    Physics Letters B , author =

    Linde, A.D. A New Inflationary Universe Scenario: A Possible Solution of the Horizon, Flatness, Homogeneity, Isotropy and Primordial Monopole Problems.Physics Letters B, 108(6):389–393, 1982. DOI: 10.1016/0370-2693(82)91219-9

  47. [49]

    and Steinhardt, P.J

    Guth, A.H. and Steinhardt, P.J. The Inflationary Universe.Scientific American, 250(5):116–129, 1984. JSTOR: 24969368

  48. [50]

    and Escobar, L

    Beyer, F. and Escobar, L. Graceful exit from inflation for minimally coupled Bianchi A scalar field models.Classical and Quantum Gravity, 30(19):195020, 2013. DOI: 10.1088/0264-9381/30/19/195020

  49. [51]

    Springer International Publishing,

    Kaiser, D.I.Nonminimal Couplings in the Early Universe: Multifield Models of In- flation and the Latest Observations, pages 41–57. Springer International Publishing,

  50. [52]

    ISBN: 978-3-319-31299-6

  51. [53]

    and Carrilho, P

    Bertolami, O. and Carrilho, P. and P´ aramos, J. Two-scalar-field model for the in- teraction of dark energy and dark matter.Physical Review D, 86(10):103522, 2012. DOI: 10.1103/PhysRevD.86.103522

  52. [54]

    Interacting scalar fields: Dark matter and early dark energy.Physical Review D, 110:023529, 2024

    Garcia-Arroyo, G., Ure˜ na-L´ opez, L.A., and V´ azquez, J.A. Interacting scalar fields: Dark matter and early dark energy.Physical Review D, 110:023529, 2024. DOI: 10.1103/PhysRevD.110.023529

  53. [55]

    Multiple field inflation

    Wands, D. Multiple field inflation. InInflationary cosmology, pages 275–304. Springer,

  54. [56]

    ArXiv: astro-ph/0702187

  55. [57]

    and Guoqin, R

    Berglund, P. and Guoqin, R. Multi-field inflation from string theory.arXiv Preprint,

  56. [58]

    and Sasaki, M

    Gong, J. and Sasaki, M. Waterfall field in hybrid inflation and curvature pertur- bation.Journal of Cosmology and Astroparticle Physics, 2011(03):028–028, 2011. DOI: 10.1088/1475-7516/2011/03/028

  57. [59]

    Oxford University Press, Oxford, 2008

    Weinberg, S.Cosmology. Oxford University Press, Oxford, 2008. ISBN: 9780198526827. 34

  58. [60]

    and Noh, H

    Hwang, J. and Noh, H. Cosmological perturbations with multiple fluids and fields.Clas- sical and Quantum Gravity, 19(3):527–549, 2002. DOI: 10.1088/0264-9381/19/3/308

  59. [61]

    Unified dark energy and dark matter from a scalar field different from quintessence.Physical Review D, 81(4):043520,

    Gao, C., Kunz, M., Liddle, A.R., and Parkinson, D. Unified dark energy and dark matter from a scalar field different from quintessence.Physical Review D, 81(4):043520,

  60. [62]

    DOI: 10.1103/PhysRevD.81.043520

  61. [63]

    and Maartens, R

    Durrer, R. and Maartens, R. Dark Energy and Modified Gravity. In Ruiz-Lapuente, P., editor,Dark Energy: Observational and Theoretical Approaches, pages 48–91. Cam- bridge University Press, 2010. arXiv: 0811.4132

  62. [64]

    coincidence problem

    Velten, H.E.S., vom Marttens, R.F., and Zimdahl, W. Aspects of the cosmologi- cal “coincidence problem”.The European Physical Journal C, 74(11):3160, 2014. ArXiv: 1410.2509

  63. [65]

    PhD thesis, M¨ unchen University, 2007

    Vikman, A.k-essence: cosmology, causality and emergent geometry. PhD thesis, M¨ unchen University, 2007. URL: e20632c0fd86b33f891771b45f3c8e21

  64. [66]

    Oxford Science Publications,

    Alcubierre, M.Introduction to 3+1 Numerical Relativity. Oxford Science Publications,

  65. [67]

    Fuchsian ODE system

    ISBN: 978-0199205677. 35 A Fuchsian theory for ODEs The purpose of this appendix to discuss Fuchsian techniques for ODEs. To help motivate the discussion here we first consider an example. Suppose thatu(t) is some unknown whose behaviour is governed by the ODE ∂tu(t) = a t u(t), u(T 0) =u 0.(A.1a) The goal is to solve this equation on the interval [0, T 0...