Gauge-invariant cosmological perturbations in Type 3 New General Relativity and background-hierarchy bounds
Pith reviewed 2026-05-19 20:57 UTC · model grok-4.3
pith:VVEX5KL2 Add to your LaTeX paper
What is a Pith Number?\usepackage{pith}
\pithnumber{VVEX5KL2}
Prints a linked pith:VVEX5KL2 badge after your title and writes the identifier into PDF metadata. Compiles on arXiv with no extra files. Learn more
The pith
Type 3 New General Relativity permits consistent linear cosmological perturbations only within specific parameter bounds.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We derive the background-hierarchy bounds for the scalar, transverse-vector, and tensor modes around a flat FLRW background, and identify the region of parameter space in which the linear perturbation theory of Type 3 remains viable for cosmological applications. The propagating modes are correctly identified even when the perturbed Lagrangian is not written solely in terms of gauge-invariant variables, after reviewing preferable gauge choices for metric-affine theories with Weitzenbock connection.
What carries the argument
Background-hierarchy bounds obtained by comparing background spacetime evolution contributions to quadratic kinetic terms in the perturbed Lagrangian.
If this is right
- Linear perturbation theory of Type 3 remains viable for cosmological applications inside the derived parameter region for scalar, transverse-vector, and tensor modes.
- Propagating modes stay correctly identified in the perturbative analysis without needing the Lagrangian written only in gauge-invariant variables.
- Preferred gauge choices respect symmetries in both the Dirac-Bergmann analysis and linear perturbation theory for metric-affine theories with Weitzenbock connection.
Where Pith is reading between the lines
- The derived bounds could be used to select parameter values when comparing Type 3 predictions to cosmic microwave background or large-scale structure data.
- Similar hierarchy comparisons might apply to perturbation analyses in other New General Relativity types or teleparallel gravity models.
- Violation of the bounds would require moving to nonlinear perturbation orders or including interaction terms to model the theory's behavior accurately.
Load-bearing premise
The bounds assume background spacetime evolution contributions always exceed quadratic kinetic terms from perturbations; if other higher-order or interaction terms become comparable at the same scale, the viability region no longer guarantees a consistent linear theory.
What would settle it
A concrete calculation showing the quadratic kinetic term dominating the background contribution for any mode inside the claimed viable parameter region would falsify the bounds.
Figures
read the original abstract
In this paper, we investigate background-hierarchy bounds in Type~3 of New General Relativity (NGR). These bounds arise when the contribution associated with the evolution of the background spacetime exceeds that of the quadratic kinetic term in the perturbed Lagrangian. Type~3 of NGR has two free parameters and preserves diffeomorphism invariance and spatial rotations, while breaking Lorentz-boost invariance. We first review Type~3 and identify preferable gauge choices for metric-affine gauge theories of gravity with Weitzenb\"ock connection, including NGR, from the viewpoint of symmetry in both Dirac--Bergmann analysis and linear perturbation theory. We then revisit the perturbative analysis of Type~3 and show that the propagating modes are correctly identified even when the perturbed Lagrangian is not written solely in terms of gauge-invariant variables. Finally, we derive the background-hierarchy bounds for the scalar, transverse-vector, and tensor modes around a flat FLRW background, and identify the region of parameter space in which the linear perturbation theory of Type~3 remains viable for cosmological applications.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper reviews Type 3 New General Relativity, identifies suitable gauge choices for metric-affine theories with Weitzenböck connection, confirms that propagating modes (scalar, transverse-vector, tensor) are correctly identified in the linear perturbation analysis around flat FLRW even without exclusive use of gauge-invariant variables, and derives background-hierarchy bounds by requiring that the background spacetime evolution term exceeds the quadratic kinetic term in the perturbed Lagrangian. It then maps the resulting viable region in the two-parameter space for which linear cosmological perturbation theory remains applicable.
Significance. If the bounds hold and the linear truncation is self-consistent, the work supplies concrete parameter constraints that delineate where Type 3 NGR can be reliably used for cosmological applications. The explicit discussion of gauge choices and the demonstration that mode counting remains correct without full gauge-invariant reduction are useful technical contributions to the literature on metric-affine gravity.
major comments (1)
- The central viability claim rests on the background term dominating the quadratic kinetic term for each mode class. However, the manuscript does not supply an estimate showing that cubic or higher interaction terms remain parametrically smaller throughout the claimed region; if any such term becomes comparable near the boundary, the truncation to linear order would lose self-consistency. This assumption is load-bearing for the final statement that the identified parameter space supports reliable cosmological applications.
minor comments (1)
- The abstract and introduction would benefit from a brief statement of the explicit form of the two free parameters and the precise definition of the background-hierarchy ratio used to obtain the bounds.
Simulated Author's Rebuttal
We thank the referee for the positive evaluation of the manuscript and for the constructive major comment. We address the point below and will revise the manuscript to strengthen the discussion of truncation self-consistency.
read point-by-point responses
-
Referee: The central viability claim rests on the background term dominating the quadratic kinetic term for each mode class. However, the manuscript does not supply an estimate showing that cubic or higher interaction terms remain parametrically smaller throughout the claimed region; if any such term becomes comparable near the boundary, the truncation to linear order would lose self-consistency. This assumption is load-bearing for the final statement that the identified parameter space supports reliable cosmological applications.
Authors: We agree that a complete justification of the linear truncation's validity would benefit from an explicit estimate of higher-order terms. The manuscript derives the background-hierarchy bounds by requiring that the background evolution term exceeds the quadratic kinetic contributions in the perturbed Lagrangian, thereby ensuring the linear equations remain a controlled approximation around flat FLRW. In the revised version we will add a short scaling argument in the discussion section (following the presentation of the bounds) showing that cubic interaction terms are suppressed by an additional factor of the dimensionless perturbation amplitude, which is assumed small (≪1) throughout the linear regime. Near the boundary of the viable parameter region this suppression factor remains intact, so the cubic terms stay parametrically smaller than the retained quadratic terms. A full nonlinear analysis lies beyond the present scope, which is limited to linear cosmological perturbations; we will note this limitation explicitly. We believe the added discussion will make the viability claim more robust without altering the central results. revision: yes
Circularity Check
No significant circularity; bounds derived by direct term comparison in perturbed Lagrangian
full rationale
The paper derives background-hierarchy bounds through explicit comparison of the background spacetime evolution term against the quadratic kinetic term in the perturbed Lagrangian for scalar, vector, and tensor modes around flat FLRW. This is a straightforward algebraic inequality obtained from the action expansion and does not reduce to any fitted parameter, self-referential definition, or load-bearing self-citation chain. Prior work on Type 3 NGR is reviewed for context and gauge choices, but the central viability region follows independently from the mode-by-mode term ordering without invoking uniqueness theorems or ansatze from the authors' own prior papers as the sole justification.
Axiom & Free-Parameter Ledger
free parameters (1)
- two free parameters of Type 3 NGR
axioms (2)
- domain assumption Flat FLRW background spacetime
- domain assumption Preservation of diffeomorphism invariance and spatial rotations
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
We derive the background-hierarchy bounds for the scalar, transverse-vector, and tensor modes around a flat FLRW background, and identify the region of parameter space in which the linear perturbation theory of Type 3 remains viable
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
background-hierarchy bound is estimated as δhij ∼ sqrt(-1 + 3c3/2c2)
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
second-order terms of perturbation fields are included in the torsion and metric tensor,
-
[2]
Our results in the previous work are summarized in Table I
the gauge choice is performed in a manner consistent with the symmetry inherent in NGR, as clarified by the DB analysis. Our results in the previous work are summarized in Table I. The first point has already been addressed in our previous work [23]. However, the second point requires further investigation, setting it for the first purpose of this paper. ...
-
[3]
A first-class constraint disappears, giving rise to one new DOF
Pattern I. A first-class constraint disappears, giving rise to one new DOF
-
[4]
Pattern II. Two first-class constraints become second-class, giving rise to one new DOF; Patterns I and II occur in modifications or extensions of an original theory, and these two patterns are directly related to the emergence of new DOFs in NGR. We mention two important representations of symmetry in MAG theories. The first is diffeomorphism symmetry, w...
-
[5]
Gauge choice I.φ ′ = 0,B ′ = 0,C ′ i = 0 (spatially flat gauge)
-
[6]
Gauge choice II.α ′ = 0,B ′ = 0,C ′ i = 0. Here, each gauge choice is expressed in terms of perturbation fields rather than the gauge parametersξ 0,ξ, andξ (v) i . Finally, we establish a criterion for selecting an appropriate gauge choice from the list given above. To this end, we restrict our attention to theories of gravity that satisfy diffeomorphism ...
-
[7]
The perturbed theory of gravity contains only a kinetic term ofα ′
Case A. The perturbed theory of gravity contains only a kinetic term ofα ′
-
[8]
Case B. The perturbed theory of gravity contains not only a kinematic term ofα ′ but also a quadratic term composed ofψ ′ and/or a time derivative ofψ ′. In Case A, we can count the kinetic term ofα ′ as a propagating scalar mode, since ˙α′ ˙α′ contains only the kinetic term of the gauge-invariant variableγ ′,i.e., (aH) −2 ˙γ′ ˙γ′ ∈ ˙α′ ˙α′. Cases B is mo...
-
[9]
The perturbed theory of gravity contains only the kinetic term ofφ ′
Case A. The perturbed theory of gravity contains only the kinetic term ofφ ′
-
[10]
The perturbed theory of gravity contains the kinetic terms not only ofφ ′ but also ofψ ′
Case B. The perturbed theory of gravity contains the kinetic terms not only ofφ ′ but also ofψ ′. In Case A, the diffeomorphism invariance prohibits this mode from propagating; this case cannot be realized under this invariance. In Case B, the term ˙ψ′ ˙ψ′ contains two kinetic terms proportional to ˙β′ ˙β′ and ˙γ′ ˙γ′, respectively, and no higher-order ti...
-
[11]
Riemann-geometrie mit aufrechterhaltung des begriffes des fernparallelismus,
A. Einstein, “Riemann-geometrie mit aufrechterhaltung des begriffes des fernparallelismus,” Preussische Akademie der Wissenschaften, Phys.Math. Klasse, Sitzungsberichte. (1928) 217
work page 1928
-
[12]
Measurements of Omega and Lambda from 42 High-Redshift Supernovae
K. Hayashi and T. Shirafuji, “New general relativity.,” Phys. Rev. D19(1979) 3524–3553. [Addendum: Phys.Rev.D 24, 3312–3314 (1982)]. [3]Supernova Cosmology ProjectCollaboration, S. Perlmutter et al., “Measurements of Ω and Λ from 42 High Redshift Supernovae,” Astrophys. J.517(1999) 565–586,arXiv:astro-ph/9812133. [4]Supernova Search TeamCollaboration, A. ...
work page internal anchor Pith review Pith/arXiv arXiv 1979
-
[13]
K. Freese, “Review of Observational Evidence for Dark Matter in the Universe and in upcoming searches for Dark Stars,” EAS Publ. Ser.36(2009) 113–126,arXiv:0812.4005 [astro-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2009
-
[14]
Direct detection of dark matter—APPEC committee report*,
J. Billard et al., “Direct detection of dark matter—APPEC committee report*,” Rept. Prog. Phys.85(2022) no. 5, 056201,arXiv:2104.07634 [hep-ex]. [8]PlanckCollaboration, N. Aghanim et al., “Planck 2018 results. VI. Cosmological parameters,” Astron. Astrophys.641 (2020) A6,arXiv:1807.06209 [astro-ph.CO]. [Erratum: Astron.Astrophys. 652, C4 (2021)]. [9]H0LiC...
-
[15]
BAO+BBN revisited — growing the Hubble tension with a 0.7 km/s/Mpc constraint,
N. Sch¨ oneberg, L. Verde, H. Gil-Mar´ ın, and S. Brieden, “BAO+BBN revisited — growing the Hubble tension with a 0.7 km/s/Mpc constraint,” JCAP11(2022) 039,arXiv:2209.14330 [astro-ph.CO]
-
[16]
A. G. Riess, S. Casertano, W. Yuan, L. M. Macri, and D. Scolnic, “Large Magellanic Cloud Cepheid Standards Provide a 1% Foundation for the Determination of the Hubble Constant and Stronger Evidence for Physics beyond ΛCDM,” Astrophys. J.876(2019) no. 1, 85,arXiv:1903.07603 [astro-ph.CO]. [12]ACTCollaboration, M. S. Madhavacheril et al., “The Atacama Cosmo...
work page internal anchor Pith review Pith/arXiv arXiv 2019
-
[17]
P. G. Bergmann, “Non-Linear Field Theories,” Phys. Rev.75(1949) 680–685
work page 1949
-
[18]
Non-linear field theories II. Canonical equations and quantization,
P. G. Bergmann and J. H. M. Brunings, “Non-linear field theories II. Canonical equations and quantization,” Rev.Mod.Phys.21(1949) 480
work page 1949
-
[19]
Generalized Hamiltonian dynamics,
P. A. M. Dirac, “Generalized Hamiltonian dynamics,” Can. J. Math.2(1950) 129–148. 22
work page 1950
-
[20]
The Hamiltonian of the general theory of relativity with electromagnetic field,
P. G. Bergmann, R. Penfield, R. Schiller, and H. Zatzkis, “The Hamiltonian of the general theory of relativity with electromagnetic field,” Phys.Rev.80(1950) 81
work page 1950
-
[21]
Constraints in covariant field theories,
J. L. Anderson and P. G. Bergmann, “Constraints in covariant field theories,” Phys. Rev.83(1951) 1018–1025
work page 1951
-
[22]
Generalized Hamiltonian dynamics,
P. A. M. Dirac, “Generalized Hamiltonian dynamics,” Proc. Roy. Soc. Lond. A246(1958) 326–332
work page 1958
-
[23]
The Theory of gravitation in Hamiltonian form,
P. A. M. Dirac, “The Theory of gravitation in Hamiltonian form,” Proc. Roy. Soc. Lond. A246(1958) 333–343
work page 1958
-
[24]
Hamiltonian and primary constraints of new general relativity
D. Blixt, M. Hohmann, and C. Pfeifer, “Hamiltonian and primary constraints of new general relativity,” Phys. Rev. D99 (2019) no. 8, 084025,arXiv:1811.11137 [gr-qc]
work page internal anchor Pith review Pith/arXiv arXiv 2019
-
[25]
Degrees of freedom of new general relativity: Type 2, type 3, type 5, and type 8,
K. Tomonari and D. Blixt, “Degrees of freedom of new general relativity: Type 2, type 3, type 5, and type 8,” Phys. Rev. D112(2025) no. 8, 084052,arXiv:2410.15056 [gr-qc]
-
[26]
Degrees of freedom of new general relativity: Type 4, type 7, and type 9,
K. Tomonari, “Degrees of freedom of new general relativity: Type 4, type 7, and type 9,” Phys. Lett. B875(2026) 140310,arXiv:2411.11118 [gr-qc]
-
[27]
K. Tomonari, T. Katsuragawa, and S. Nojiri, “Cosmological Perturbation in New General Relativity: Propagating mode from the violation of local Lorentz invariance,”arXiv:2509.18772 [gr-qc]
-
[28]
Conformal transformations and cosmological perturbations in New General Relativity,
A. Golovnev, A. N. Semenova, and V. P. Vandeev, “Conformal transformations and cosmological perturbations in New General Relativity,” JCAP04(2024) 064,arXiv:2312.16021 [gr-qc]
-
[29]
On ghost-free tensor lagrangians and linearized gravitation,
P. Van Nieuwenhuizen, “On ghost-free tensor lagrangians and linearized gravitation,” Nucl. Phys. B60(1973) 478–492
work page 1973
-
[30]
Propagating Modes in Gauge Field Theories of Gravity,
R. Kuhfuss and J. Nitsch, “Propagating Modes in Gauge Field Theories of Gravity,” Gen. Rel. Grav.18(1986) 1207
work page 1986
-
[31]
Gravitational waves in New General Relativity,
A. Golovnev, A. N. Semenova, and V. P. Vandeev, “Gravitational waves in New General Relativity,” JCAP01(2024) 003,arXiv:2309.02853 [gr-qc]
-
[32]
Some simple theories of gravity with propagating torsion,
Y. Mikura, V. Naso, and R. Percacci, “Some simple theories of gravity with propagating torsion,” Phys. Rev. D109 (2024) no. 10, 104071,arXiv:2312.10249 [gr-qc]
-
[33]
Revisiting stability in new general relativity,
S. Bahamonde, A. Hell, D. Blixt, and K. F. Dialektopoulos, “Revisiting stability in new general relativity,” Phys. Rev. D 111(2025) no. 6, 064080,arXiv:2404.02972 [gr-qc]
-
[34]
Lorentz gauge-invariant variables in torsion-based theories of gravity,
D. Blixt, R. Ferraro, A. Golovnev, and M.-J. Guzm´ an, “Lorentz gauge-invariant variables in torsion-based theories of gravity,” Phys. Rev. D105(2022) no. 8, 084029,arXiv:2201.11102 [gr-qc]
-
[35]
The covariant formulation of f(T) gravity
M. Krˇ sˇ s´ ak and E. N. Saridakis, “The covariant formulation of f(T) gravity,”Class. Quant. Grav.33(2016) no. 11, 115009,arXiv:1510.08432 [gr-qc]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[36]
Global and local stability for ghosts coupled to positive energy degrees of freedom,
C. Deffayet, A. Held, S. Mukohyama, and A. Vikman, “Global and local stability for ghosts coupled to positive energy degrees of freedom,” JCAP11(2023) 031,arXiv:2305.09631 [gr-qc]
-
[37]
Jim´ enez Cano,Metric-affine Gauge theories of gravity
A. Jim´ enez Cano,Metric-affine Gauge theories of gravity. Foundations and new insights. PhD thesis, Granada U., Theor. Phys. Astrophys., 2021.arXiv:2201.12847 [gr-qc]
-
[38]
Introducing Cadabra: a symbolic computer algebra system for field theory problems
K. Peeters, “Introducing Cadabra: A Symbolic computer algebra system for field theory problems,” arXiv:hep-th/0701238
work page internal anchor Pith review Pith/arXiv arXiv
-
[39]
F. W. Hehl, J. D. McCrea, E. W. Mielke, and Y. Ne’eman, “Metric affine gauge theory of gravity: Field equations, Noether identities, world spinors, and breaking of dilation invariance,” Phys. Rept.258(1995) 1–171, arXiv:gr-qc/9402012
work page internal anchor Pith review Pith/arXiv arXiv 1995
-
[40]
Teleparallel gravity: from theory to cosmology,
S. Bahamonde, K. F. Dialektopoulos, C. Escamilla-Rivera, G. Farrugia, V. Gakis, M. Hendry, M. Hohmann, J. Levi Said, J. Mifsud, and E. Di Valentino, “Teleparallel gravity: from theory to cosmology,” Rept. Prog. Phys.86(2023) no. 2, 026901,arXiv:2106.13793 [gr-qc]
-
[41]
Static spherically symmetric solutions in new general relativity,
A. Golovnev, A. N. Semenova, and V. P. Vandeev, “Static spherically symmetric solutions in new general relativity,” Class. Quant. Grav.41(2024) no. 5, 055009,arXiv:2305.03420 [gr-qc]
-
[42]
Hamiltonian structure of the teleparallel formulation of GR
M. Blagojevic and I. A. Nikolic, “Hamiltonian structure of the teleparallel formulation of GR,” Phys. Rev. D62(2000) 024021,arXiv:hep-th/0002022
work page internal anchor Pith review Pith/arXiv arXiv 2000
-
[43]
Dynamical structure and definition of energy in general relativity,
S. Deser, “Dynamical structure and definition of energy in general relativity,” Colloq. Int. CNRS91(1962) 395–407
work page 1962
-
[44]
Canonical variables for general relativity,
R. L. Arnowitt, S. Deser, and C. W. Misner, “Canonical variables for general relativity,” Phys. Rev.117(1960) 1595–1602
work page 1960
-
[45]
The Dynamics of General Relativity
R. L. Arnowitt, S. Deser, and C. W. Misner, “The Dynamics of general relativity,” Gen. Rel. Grav.40(2008) 1997–2027, arXiv:gr-qc/0405109
work page internal anchor Pith review Pith/arXiv arXiv 2008
-
[46]
POISSON BRACKETS OF THE CONSTRAINTS IN THE HAMILTONIAN FORMULATION OF TETRAD GRAVITY,
M. Henneaux, “POISSON BRACKETS OF THE CONSTRAINTS IN THE HAMILTONIAN FORMULATION OF TETRAD GRAVITY,” Phys. Rev. D27(1983) 986–989
work page 1983
-
[47]
Canonical Vielbeins for General Relativity: D + 1 Decomposition and Constraint Analysis,
J. Flinckman and D. Blixt, “Canonical Vielbeins for General Relativity: D + 1 Decomposition and Constraint Analysis,” arXiv:2602.18491 [gr-qc]
-
[48]
Canonical formalism for degenerate Lagrangians,
S. Shanmugadhasan, “Canonical formalism for degenerate Lagrangians,” Journal of Mathematical Physics14(1973) no. 6, 677–687,https://pubs.aip.org/aip/jmp/article-pdf/14/6/677/8146586/677 1 online.pdf
work page 1973
-
[49]
T. Maskawa and H. Nakajima, “Singular Lagrangian and the Dirac-Faddeev Method: Existence Theorem of Constraints in ’Standard Form’,” Progress of Theoretical Physics56(1976) no. 4, 1295–1309, https://academic.oup.com/ptp/article-pdf/56/4/1295/5360551/56-4-1295.pdf
work page 1976
-
[50]
Poincare-cartan Integral Invariant and Canonical Transformations for Singular Lagrangians,
D. Dominici and J. Gomis, “Poincare-cartan Integral Invariant and Canonical Transformations for Singular Lagrangians,” J. Math. Phys.21(1980) 2124–2130. [Addendum: J.Math.Phys. 23, 256 (1982)]
work page 1980
-
[51]
K. Tomonari, “On the well-posed variational principle in degenerate point particle systems using embeddings of the symplectic manifold,” PTEP2023(2023) no. 6, 063A05,arXiv:2304.00877 [math-ph]
-
[52]
On the Relation of First Class Constraints to Gauge Degrees of Freedom,
R. Sugano and T. Kimura, “On the Relation of First Class Constraints to Gauge Degrees of Freedom,” Prog. Theor. Phys.69(1983) 252
work page 1983
-
[53]
Generator of Gauge Transformation in Phase Space and Velocity Phase Space,
R. Sugano, Y. Saito, and T. Kimura, “Generator of Gauge Transformation in Phase Space and Velocity Phase Space,” 23 Prog. Theor. Phys.76(1986) 283
work page 1986
-
[54]
Gauge Transformations for Dynamical Systems With First and Second Class Constraints,
R. Sugano and T. Kimura, “Gauge Transformations for Dynamical Systems With First and Second Class Constraints,” Phys. Rev. D41(1990) 1247
work page 1990
-
[55]
Extension to velocity dependent gauge transformations. 1: General form of the generator,
R. Sugano and Y. Kagraoka, “Extension to velocity dependent gauge transformations. 1: General form of the generator,” Z. Phys. C52(1991) 437–442
work page 1991
-
[56]
R. Sugano and Y. Kagraoka, “Extension to velocity dependent gauge transformations. 2. Properties of velocity dependent gauge transformations,” Z. Phys. C52(1991) 443–448
work page 1991
-
[57]
Hamiltonian formulation of teleparallel gravity
R. Ferraro and M. J. Guzm´ an, “Hamiltonian formulation of teleparallel gravity,” Phys. Rev. D94(2016) no. 10, 104045, arXiv:1609.06766 [gr-qc]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[58]
Hamiltonian formalism for f(T) gravity
R. Ferraro and M. J. Guzm´ an, “Hamiltonian formalism for f(T) gravity,” Phys. Rev. D97(2018) no. 10, 104028, arXiv:1802.02130 [gr-qc]
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[59]
f(T) gravity mimicking dynamical dark energy. Background and perturbation analysis
J. B. Dent, S. Dutta, and E. N. Saridakis, “f(T) gravity mimicking dynamical dark energy. Background and perturbation analysis,” JCAP01(2011) 009,arXiv:1010.2215 [astro-ph.CO]
work page internal anchor Pith review Pith/arXiv arXiv 2011
-
[60]
Cosmological perturbations in f(T) gravity
S.-H. Chen, J. B. Dent, S. Dutta, and E. N. Saridakis, “Cosmological perturbations in f(T) gravity,” Phys. Rev. D83 (2011) 023508,arXiv:1008.1250 [astro-ph.CO]
work page internal anchor Pith review Pith/arXiv arXiv 2011
-
[61]
Matter Density Perturbations in Modified Teleparallel Theories
Y.-P. Wu and C.-Q. Geng, “Matter Density Perturbations in Modified Teleparallel Theories,” JHEP11(2012) 142, arXiv:1211.1778 [gr-qc]
work page internal anchor Pith review Pith/arXiv arXiv 2012
-
[62]
Cosmological Perturbation in f(T) Gravity Revisited
K. Izumi and Y. C. Ong, “Cosmological Perturbation in f(T) Gravity Revisited,” JCAP06(2013) 029,arXiv:1212.5774 [gr-qc]
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[63]
Cosmological perturbations in modified teleparallel gravity models,
A. Golovnev and T. Koivisto, “Cosmological perturbations in modified teleparallel gravity models,” JCAP11(2018) 012, arXiv:1808.05565 [gr-qc]
-
[64]
M´ emoires sur les ´ equations diff´ erentielles, relatives au probl` eme des isop´ erim` etres,
M. Ostrogradsky, “M´ emoires sur les ´ equations diff´ erentielles, relatives au probl` eme des isop´ erim` etres,”Mem. Acad. St. Petersbourg6(1850) no. 4, 385–517
-
[65]
Ostrogradski Theorem for Higher Order Singular Lagrangians,
J. M. Pons, “Ostrogradski Theorem for Higher Order Singular Lagrangians,” Lett. Math. Phys.17(1989) 181
work page 1989
-
[66]
R. P. Woodard, “Ostrogradsky’s theorem on Hamiltonian instability,” Scholarpedia10(2015) no. 8, 32243, arXiv:1506.02210 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[67]
Healthy degenerate theories with higher derivatives
H. Motohashi, K. Noui, T. Suyama, M. Yamaguchi, and D. Langlois, “Healthy degenerate theories with higher derivatives,” JCAP07(2016) 033,arXiv:1603.09355 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[68]
The strong couplings of massive Yang-Mills theory,
A. Hell, “The strong couplings of massive Yang-Mills theory,” JHEP03(2022) 167,arXiv:2111.00017 [hep-th]
-
[69]
On the duality of massive Kalb-Ramond and Proca fields,
A. Hell, “On the duality of massive Kalb-Ramond and Proca fields,” JCAP01(2022) no. 01, 056,arXiv:2109.05030 [hep-th]
-
[70]
To the problem of nonvanishing gravitation mass,
A. I. Vainshtein, “To the problem of nonvanishing gravitation mass,” Phys. Lett. B39(1972) 393–394
work page 1972
-
[71]
C. G. Bohmer, R. J. Downes, and D. Vassiliev, “Rotational elasticity,” The Quarterly Journal of Mechanics and Applied Mathematics64(2011) no. 4, 415–439.http://dx.doi.org/10.1093/qjmam/hbr011
-
[72]
A gauge-theoretical approach to elasticity with microrotations,
C. G. B¨ ohmer and Y. N. Obukhov, “A gauge-theoretical approach to elasticity with microrotations,” Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences468(2012) no. 2141, 1391–1407. http://dx.doi.org/10.1098/rspa.2011.0718
-
[73]
Hamiltonian analysis in new general relativity,
D. Blixt, M. Hohmann, M. Krˇ sˇ s´ ak, and C. Pfeifer, “Hamiltonian analysis in new general relativity,” 5, 2019. arXiv:1905.11919v2 [gr-qc]
-
[74]
Constraints on bimetric gravity. Part II. Observational constraints,
M. H¨ og˚ as and E. M¨ ortsell, “Constraints on bimetric gravity. Part II. Observational constraints,”JCAP05(2021) 002, arXiv:2101.08795 [gr-qc]
-
[75]
On UV-completion of Palatini-Higgs inflation,
Y. Mikura and Y. Tada, “On UV-completion of Palatini-Higgs inflation,” JCAP05(2022) no. 05, 035, arXiv:2110.03925 [hep-ph]
-
[76]
Hybrid metric-Palatini Higgs inflation,
M. He, Y. Mikura, and Y. Tada, “Hybrid metric-Palatini Higgs inflation,” JCAP05(2023) 047,arXiv:2209.11051 [hep-th]
-
[77]
Towards a classification of UV completable Higgs inflation in metric-affine gravity,
Y. Mikura and Y. Tada, “Towards a classification of UV completable Higgs inflation in metric-affine gravity,” JCAP02 (2025) 044,arXiv:2410.11277 [hep-th]
-
[78]
Non-Linear Obstructions for Consistent New General Relativity,
J. Beltr´ an Jim´ enez and K. F. Dialektopoulos, “Non-Linear Obstructions for Consistent New General Relativity,”JCAP 01(2020) 018,arXiv:1907.10038 [gr-qc]
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.