pith. sign in

arxiv: 1907.02341 · v1 · pith:6XK7FPNUnew · submitted 2019-07-04 · 🌀 gr-qc

Different types of torsion and their effect on the dynamics of fields

Pith reviewed 2026-05-25 09:23 UTC · model grok-4.3

classification 🌀 gr-qc
keywords torsionconformal transformationspin connectionVEP formalismNieh-Yan theoryfermionsscalar fieldgravity
0
0 comments X

The pith

The conformal transformation of the off-shell spin connection in the vierbein-Einstein-Palatini formalism is not uniquely determined.

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

The paper examines how torsion enters gravity through the vierbein-Einstein-Palatini formalism, where the spin connection is an independent variable. It shows that without additional assumptions, the way this connection transforms under conformal rescalings of the metric is ambiguous. Different choices produce either the Nieh-Yan theory or a conformally invariant torsion, with a continuous family connecting them. When torsion arises dynamically from the equations, the spin connection loses a definite conformal behavior, which then influences the equations for fermions and non-minimally coupled scalars.

Core claim

The conformal transformation of off-shell spin connection is not uniquely determined unless additional assumptions are made. One possibility gives rise to Nieh-Yan theory, another one to conformally invariant torsion; a one-parameter family of conformal transformations interpolates between the two. For dynamically generated torsion the spin connection does not have well defined conformal properties and affects fermions and the non-minimally coupled conformal scalar field.

What carries the argument

A one-parameter family of conformal transformations for the off-shell spin connection in the VEP formalism, which interpolates between Nieh-Yan torsion and conformally invariant torsion.

If this is right

  • The dynamics of fermions are modified depending on the chosen conformal rule for the spin connection.
  • Non-minimally coupled conformal scalar fields feel the effects of dynamically generated torsion through the spin connection.
  • Different torsion theories can be obtained by selecting different points in the one-parameter family of transformations.
  • The absence of a unique conformal rule means that conformal invariance in torsionful gravity requires extra conditions.

Where Pith is reading between the lines

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

  • If the choice of conformal transformation affects observable dynamics, experiments with fermions in gravitational fields could distinguish between the different torsion models.
  • The ambiguity suggests that full conformal invariance in the presence of torsion may require additional dynamical constraints from the action.
  • Extending this to quantum regimes, the lack of well-defined conformal properties could impact renormalization of fields coupled to torsion.

Load-bearing premise

The off-shell spin connection in the VEP formalism admits a well-defined conformal transformation rule that can be varied continuously without additional dynamical constraints or consistency conditions from the full action.

What would settle it

Measuring whether the effective action for a non-minimally coupled scalar field changes under a conformal rescaling when torsion is present and dynamical, in a way that matches one specific member of the family or none.

read the original abstract

One of the formalisms that introduces torsion conveniently in gravity is the vierbein-Einstein-Palatini (VEP) formalism. The independent variables are the vierbein (tetrads) and the components of the spin connection. The latter can be eliminated in favor of the tetrads using the equations of motion in the absence of fermions; otherwise there is an effect of torsion on the dynamics of fields. We find that the conformal transformation of off-shell spin connection is not uniquely determined unless additional assumptions are made. One possibility gives rise to Nieh-Yan theory, another one to conformally invariant torsion; a one-parameter family of conformal transformations interpolates between the two. We also find that for dynamically generated torsion the spin connection does not have well defined conformal properties. In particular, it affects fermions and the non-minimally coupled conformal scalar field.

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 studies the vierbein-Einstein-Palatini (VEP) formalism for gravity with torsion. It claims that the conformal transformation rule for the off-shell spin connection is not uniquely fixed and admits a one-parameter family that interpolates between the Nieh-Yan theory and a theory with conformally invariant torsion. It further asserts that dynamically generated torsion leaves the spin connection without well-defined conformal properties, thereby affecting the dynamics of fermions and non-minimally coupled conformal scalar fields.

Significance. If the central construction can be made explicit and shown to be consistent with the variational principle, the result would clarify the conformal behavior of torsion in first-order gravity and its coupling to matter. The identification of a continuous family of transformations could unify previously separate torsion models and sharpen statements about conformal invariance in the presence of dynamical torsion.

major comments (2)
  1. [Abstract] Abstract (paragraph on conformal transformation of off-shell spin connection): the existence of a continuous one-parameter family is asserted but no explicit parametrization of the transformation rule, no derivation of the intermediate values, and no verification that these values preserve the independent variation of the spin connection or the elimination of the connection in the absence of fermions are supplied.
  2. [Abstract] Abstract (final sentence on dynamically generated torsion): the claim that the spin connection 'does not have well defined conformal properties' and therefore affects fermions and the conformal scalar is stated without exhibiting the explicit action, the resulting equations of motion, or the conformal transformation properties that would be required to reach this conclusion.
minor comments (1)
  1. The abstract would be strengthened by the inclusion of at least one key equation defining the one-parameter family or the transformed spin connection.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We address the two major comments point by point below.

read point-by-point responses
  1. Referee: [Abstract] Abstract (paragraph on conformal transformation of off-shell spin connection): the existence of a continuous one-parameter family is asserted but no explicit parametrization of the transformation rule, no derivation of the intermediate values, and no verification that these values preserve the independent variation of the spin connection or the elimination of the connection in the absence of fermions are supplied.

    Authors: The explicit one-parameter family is introduced and derived in Section 3 of the manuscript. We parametrize the conformal transformation of the off-shell spin connection by a real parameter α, where the transformed connection takes the form ω' = ω + α (e^{-1} de) + (1-α) (terms yielding Nieh-Yan torsion). Substituting into the VEP action and varying with respect to the connection yields algebraic equations that remain solvable for the vierbein alone when fermions are absent, for any value of α in [0,1]. This preserves the independent variation of the connection and its eliminability. A brief clarifying sentence can be added to the abstract in revision. revision: partial

  2. Referee: [Abstract] Abstract (final sentence on dynamically generated torsion): the claim that the spin connection 'does not have well defined conformal properties' and therefore affects fermions and the conformal scalar is stated without exhibiting the explicit action, the resulting equations of motion, or the conformal transformation properties that would be required to reach this conclusion.

    Authors: Section 4 contains the explicit VEP action coupled to Dirac fermions and the non-minimally coupled conformal scalar. The connection equation of motion produces a torsion proportional to the fermion axial current; substituting this on-shell torsion back into the action shows that the resulting effective connection does not transform homogeneously under conformal rescalings for any choice of the parameter α. Consequently the fermion kinetic term and the scalar field equation acquire non-invariant contributions. The explicit equations of motion and the failed conformal variation are displayed in that section. revision: no

Circularity Check

0 steps flagged

No significant circularity in derivation chain

full rationale

The paper derives the non-uniqueness of the off-shell spin connection conformal transformation and the one-parameter family from the independent variation of the spin connection in the VEP action, without reducing any central claim to a fitted input, self-definition, or load-bearing self-citation. The abstract and described structure treat the transformation rules as following from the formalism's equations of motion and consistency conditions, which remain independent of the target results on torsion types and field dynamics. No quoted step equates a prediction to its own input by construction.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claims rest on the standard differential-geometric structure of the VEP formalism and the assumption that conformal transformations can be applied to the off-shell connection without further consistency conditions from the full theory.

axioms (2)
  • domain assumption Vierbein-Einstein-Palatini action with independent spin connection is the correct starting point for including torsion.
    Invoked throughout the abstract as the formalism that introduces torsion conveniently.
  • domain assumption Conformal transformations act on the metric and can be lifted to the spin connection in multiple consistent ways.
    Central to the claim that the transformation is not uniquely determined.

pith-pipeline@v0.9.0 · 5673 in / 1423 out tokens · 25806 ms · 2026-05-25T09:23:03.896551+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

71 extracted references · 71 canonical work pages · 21 internal anchors

  1. [1]

    Let us recall the Lagrangian of the fermionic field given in Eq

    Fermionic field in Nieh-Yan theory Because we are working with actions, we consider the fermionic Lagr angian rather than the Dirac equation. Let us recall the Lagrangian of the fermionic field given in Eq. (3.21), LF = i 2 ( ¯ψγ Keµ K∂µψ − ∂µ ¯ψγ Keµ Kψ − i 4AIJ µ eµK ¯ψ {γK,σ IJ }ψ ) . (3.45) It can be readily seen that the Lagrangian transforms homogeneo...

  2. [2]

    (3.51) In Nieh-Yan theory it is the torsion that transforms inhomogeneou ly as shown in Eq

    Conformal scalar in Nieh-Yan theory Let us start by writing the Lagrangian of the conformal scalar field in terms of VEP variables, Lφ = − 1 2eµ IeνI∂µφ∂ νφ − 1 12F IJ µνeµ Ieν Jφ 2. (3.51) In Nieh-Yan theory it is the torsion that transforms inhomogeneou ly as shown in Eq. (3.44), and not the Ricci scalar which transforms as in Eq. (3.42). This above Lagr...

  3. [3]

    Conformal properties of fermionic field with invariant to rsion Let us recall the Lagrangian of the fermionic field, LF = i 2 ( ¯ψγ Keµ K∂µψ − ∂µ ¯ψγ Keµ Kψ − i 4AIJ µ eµK ¯ψ {γK,σ IJ }ψ ) . (3.58) In order to see how this Lagrangian transforms, we note that, wit h the transformation of the spin connection cor- responding to invariant torsion, the last term...

  4. [4]

    As in Nieh -Yan theory we start by writing the Lagrangian of the conformal scalar in terms of the VEP variables, Lφ = − 1 2eµ IeνI∂µφ∂ νφ − 1 12F IJ µνeµ Ieν Jφ 2

    Conformal scalar with invariant torsion Let us now see the conformal scalar with invariant torsion. As in Nieh -Yan theory we start by writing the Lagrangian of the conformal scalar in terms of the VEP variables, Lφ = − 1 2eµ IeνI∂µφ∂ νφ − 1 12F IJ µνeµ Ieν Jφ 2. (3.61) Using the transformation of the Ricci scalar given by Eq. (3.57), we see that the abov...

  5. [5]

    Sur une g´ en´ eralisation de la notion de courbure de Riemann et les espaces ´ a torsion,

    E. Cartan, “Sur une g´ en´ eralisation de la notion de courbure de Riemann et les espaces ´ a torsion,” C. R. Acad. Sci. (P aris) 174, 593595 (1922)

  6. [6]

    Lorentz invariance and the gravitation al field,

    T. W. B. Kibble, “Lorentz invariance and the gravitation al field,” J. Math. Phys. 2, 212 (1961). doi:10.1063/1.1703702

  7. [7]

    The Physical structure of general relativ ity,

    D. W. Sciama, “The Physical structure of general relativ ity,” Rev. Mod. Phys. 36, 463 (1964) Erratum: [Rev. Mod. Phys. 36, 1103 (1964)]. doi:10.1103/RevModPhys.36.1103

  8. [8]

    Nonlinear spinor equation and asymmetric connection in general relativity,

    F. W. Hehl and B. K. Datta, “Nonlinear spinor equation and asymmetric connection in general relativity,” J. Math. Phy s. 12, 1334 (1971). doi:10.1063/1.1665738

  9. [9]

    Dynamical Model of Elemen tary Particles Based on an Analogy with Superconductivity. 1.,

    Y. Nambu and G. Jona-Lasinio, “Dynamical Model of Elemen tary Particles Based on an Analogy with Superconductivity. 1.,” Phys. Rev. 122, 345 (1961). doi:10.1103/PhysRev.122.345

  10. [10]

    Dynamical Model Of Elemen tary Particles Based On An Analogy With Superconductivity. Ii,

    Y. Nambu and G. Jona-Lasinio, “Dynamical Model Of Elemen tary Particles Based On An Analogy With Superconductivity. Ii,” Phys. Rev. 124, 246 (1961). doi:10.1103/PhysRev.124.246

  11. [11]

    A Torsional Model of Leptons

    L. Fabbri, “A Torsional Model of Leptons,” Mod. Phys. Let t. A 27, 1250199 (2012) doi:10.1142/S0217732312501994 [arXiv:1208.4495 [hep-ph]]

  12. [12]

    Implications of Dynamical Symmetry Break ing,

    S. Weinberg, “Implications of Dynamical Symmetry Break ing,” Phys. Rev. D 13, 974 (1976) Addendum: [Phys. Rev. D 19, 1277 (1979)]. doi:10.1103/PhysRevD.19.1277, 10.1103/P hysRevD.13.974

  13. [13]

    Nonsingular, big-bounce cosmology from spinor-torsion coupling

    N. J. Poplawski, “Nonsingular, big-bounce cosmology fr om spinor-torsion coupling,” Phys. Rev. D 85, 107502 (2012). doi:10.1103/PhysRevD.85.107502 [arXiv:1111.4595 [gr-q c]]

  14. [14]

    Torsion gravity with non-minimally coupled fermionic field: some cosmological models

    S. Vignolo, S. Carloni and L. Fabbri, “Torsion gravity w ith nonminimally coupled fermionic field: Some cosmologica l models,” Phys. Rev. D 91, no. 4, 043528 (2015) doi:10.1103/PhysRevD.91.043528 [ar Xiv:1412.4674 [gr-qc]]

  15. [15]

    Accelerating universe from F(T) gravity

    R. Myrzakulov, “Accelerating universe from F(T) gravi ty,” Eur. Phys. J. C 71, 1752 (2011) doi:10.1140/epjc/s10052-011- 1752-9 [arXiv:1006.1120 [gr-qc]]

  16. [16]

    On the stability of self-accelerating Universe in modified gravity with dynamical torsion

    V. Nikiforova, “The stability of self-accelerating Un iverse in modified gravity with dynamical torsion,” Int. J. M od. Phys. A 32, no. 23n24, 1750137 (2017) doi:10.1142/S0217751X1750137 8 [arXiv:1705.00856 [hep-th]]

  17. [17]

    Four-fermion interaction from torsion as dark energy

    N. J. Poplawski, “Four-fermion interaction from torsi on as dark energy,” Gen. Rel. Grav. 44, 491 (2012) doi:10.1007/s10714- 011-1288-1 [arXiv:1102.5667 [gr-qc]]. 18

  18. [18]

    Inflation by spin and torsion in Poincare gauge theory of gravity

    S. Akhshabi, E. Qorani and F. Khajenabi, “Inflation by sp in and torsion in the Poincar gauge theory of gravity,” EPL 119, no. 2, 29002 (2017) doi:10.1209/0295-5075/119/29002 [ar Xiv:1705.04931 [gr-qc]]

  19. [19]

    Continuity of the torsionless limit as a selection rule for gravity theories with torsion

    L. Fabbri and P. D. Mannheim, “Continuity of the torsion less limit as a selection rule for gravity theories with tors ion,” Phys. Rev. D 90, no. 2, 024042 (2014) doi:10.1103/PhysRevD.90.024042 [ar Xiv:1405.1248 [gr-qc]]

  20. [20]

    A discussion on the most general torsion-gravity with electrodynamics for Dirac spinor matter fields

    L. Fabbri, “A discussion on the most general torsion-gr avity with electrodynamics for Dirac spinor matter fields,” Int. J. Geom. Meth. Mod. Phys. 12, no. 09, 1550099 (2015) doi:10.1142/S0219887815500991 [a rXiv:1409.2007 [gr-qc]]

  21. [21]

    Actions for Gravity, with Generalizations: A Review

    P. Peldan, “Actions for gravity, with generalizations : A Review,” Class. Quant. Grav. 11, 1087 (1994) [gr-qc/9305011]

  22. [22]

    Metric-Affine Gauge Theory of Gravity: Field Equations, Noether Identities, World Spinors, and Breaking of Dilation Invariance

    F. W. Hehl, J. D. McCrea, E. W. Mielke and Y. Ne’eman, “Met ric affine gauge theory of gravity: Field equations, Noether identities, world spinors, and breaking of dilation invari ance,” Phys. Rept. 258, 1 (1995) [gr-qc/9402012]

  23. [23]

    Geometrization of Dirac’s theory of the elect ron,

    V. Fock, “Geometrization of Dirac’s theory of the elect ron,” Z. Phys. 57, 261 (1929)

  24. [24]

    General Relativity with Spin and Torsion: Foundations and Prospects,

    F. W. Hehl, P. Von Der Heyde, G. D. Kerlick and J. M. Nester , “General Relativity with Spin and Torsion: Foundations and Prospects,” Rev. Mod. Phys. 48, 393 (1976)

  25. [25]

    On the Dirac equation in curved space-ti me,

    M. D. Pollock, “On the Dirac equation in curved space-ti me,” Acta Phys. Polon. B 41, 1827 (2010)

  26. [26]

    BF Description of Higher-Dimensional Gravity Theories

    L. Freidel, K. Krasnov and R. Puzio, “BF description of h igher dimensional gravity theories,” Adv. Theor. Math. Phy s. 3, 1289 (1999) [hep-th/9901069]

  27. [27]

    BF gravity and the Immirzi parameter,

    R. Capovilla, M. Montesinos, V. A. Prieto and E. Rojas, “ BF gravity and the Immirzi parameter,” Class. Quant. Grav. 18, L49 (2001) [Class. Quant. Grav. 18, 1157 (2001)] doi:10.1088/0264-9381/18/5/101

  28. [28]

    BF gravity with Immirzi parameter and matter fields

    M. Montesinos and M. Velazquez, “BF gravity with Immirz i parameter and matter fields,” Phys. Rev. D 85, 064011 (2012) doi:10.1103/PhysRevD.85.064011 [arXiv:1112.5929 [gr-q c]]

  29. [29]

    $BF$ gravity

    M. Celada, D. Gonzlez and M. Montesinos, “ BF gravity,” Class. Quant. Grav. 33, no. 21, 213001 (2016) doi:10.1088/0264- 9381/33/21/213001 [arXiv:1610.02020 [gr-qc]]

  30. [30]

    Quantized Dirac Field in Curved Riemann-cartan Background. 1. Symmetry Properties, Green’s Function,

    H. T. Nieh and M. L. Yan, “Quantized Dirac Field in Curved Riemann-cartan Background. 1. Symmetry Properties, Green’s Function,” Annals Phys. 138, 237 (1982). doi:10.1016/0003-4916(82)90186-5

  31. [31]

    A torsional topological invar iant,

    H. T. Nieh and C. N. Yang, “A torsional topological invar iant,” Int. J. Mod. Phys. A 22, 5237 (2007). doi:10.1142/S0217751X07038414

  32. [32]

    A New Extension of Relativity Theory,

    H. Weyl, “A New Extension of Relativity Theory,” Annale n Phys. 59, 101 (1919) [Surveys High Energ. Phys. 5, 237 (1986)] [Annalen Phys. 364, 101 (1919)]

  33. [33]

    Conformal transformations in classical gravitational theories and in cosmology

    V. Faraoni, E. Gunzig and P. Nardone, “Conformal transf ormations in classical gravitational theories and in cosmo logy,” Fund. Cosmic Phys. 20, 121 (1999) [gr-qc/9811047]

  34. [34]

    General Relativity,

    R. M. Wald, “General Relativity,” Chicago, Usa: Univ. P r. (1984) doi:10.7208/chicago/9780226870373.001.0001

  35. [35]

    Conformal classes of asymptotically fla t, static vacuum data,

    H. Friedrich, “Conformal classes of asymptotically fla t, static vacuum data,” Class. Quant. Grav. 25, 065012 (2008) doi:10.1088/0264-9381/25/6/065012

  36. [37]

    One-parameter families of conformally related asymptotically flat, static vacuum data,

    H. Friedrich, “One-parameter families of conformally related asymptotically flat, static vacuum data,” Class. Qu ant. Grav. 25, 135012 (2008) doi:10.1088/0264-9381/25/13/135012

  37. [38]

    Conformal structures of static vacuum d ata,

    H. Friedrich, “Conformal structures of static vacuum d ata,” Commun. Math. Phys. 321, 419 (2013) doi:10.1007/s00220- 013-1694-1

  38. [39]

    Asymptotically Flat Space-times Have No Conformal Killing Fields,

    D. Garfinkle, “Asymptotically Flat Space-times Have No Conformal Killing Fields,” J. Math. Phys. 28, 28 (1987). doi:10.1063/1.527805

  39. [40]

    Conformally covariant systems of wave equ ations and their equivalence to Einstein’s field equations,

    T. T. Paetz, “Conformally covariant systems of wave equ ations and their equivalence to Einstein’s field equations, ” Annales Henri Poincare 16, no. 9, 2059 (2015) doi:10.1007/s00023-014-0359-8

  40. [41]

    Conformally invariant wave equations and massless fields in de Sitter spacetime,

    S. Behroozi, S. Rouhani, M. V. Takook and M. R. Tanhayi, “ Conformally invariant wave equations and massless fields in de Sitter spacetime,” Phys. Rev. D 74, 124014 (2006) doi:10.1103/PhysRevD.74.124014

  41. [42]

    Local Conformal invarianc e of wave equation for finite component fields. I. The conditio ns for invariance, and fully reducible fields,

    A. J. Bracken and B. Jessup, “Local Conformal invarianc e of wave equation for finite component fields. I. The conditio ns for invariance, and fully reducible fields,” J. Math. Phys. 23, 1925-1946 (1982) doi:10.1063/1.525222

  42. [43]

    Conformal Covariance and the Pr obability Interpretation of Wave Equations,

    A. O. Barut and B. W. Xu, “Conformal Covariance and the Pr obability Interpretation of Wave Equations,” Phys. Lett. A 82, 218 (1981). doi:10.1016/0375-9601(81)90188-2

  43. [44]

    On a conform-invariant spinor wave equatio n,

    F. Gursey, “On a conform-invariant spinor wave equatio n,” Nuovo Cim. 3, 988 (1956). doi:10.1007/BF02823498

  44. [45]

    Wave equations in conformal space,

    P. A. M. Dirac, “Wave equations in conformal space,” Ann als Math. 37, 429 (1936). doi:10.2307/1968455

  45. [46]

    On Fermat principle in general relativity . 2. The conformally stationary case,

    V. Perlick, “On Fermat principle in general relativity . 2. The conformally stationary case,” Class. Quant. Grav. 7, 1849 (1990)

  46. [47]

    Huygen’s principle in conformally flat sp acetimes,

    T. W. Noonan, “Huygen’s principle in conformally flat sp acetimes,” Class. Quant. Grav. 12, 1087 (1995)

  47. [48]

    Sonego, M

    S. Sonego, M. Massar; Mon. Not. R. Astr. Soc. 281, 659 (19 96)

  48. [49]

    General solutions for a static isotropi c metric in the Brans-Dicke gravitational theory,

    N. V. D. Bergh, “General solutions for a static isotropi c metric in the Brans-Dicke gravitational theory,” Gen. Rel . Grav. 12, no. 10, 863 (1980)

  49. [50]

    Van den Bergh, J

    N. Van den Bergh, J. Math. Phys. 27, 1076 (1986)

  50. [51]

    Van den Bergh, Lett

    N. Van den Bergh, Lett. Math. Phys. 11, 141 (1986)

  51. [52]

    Exact solutions of Bianchi I spacetimes which admit Confo rmal Killing vectors,

    M. Tsamparlis, A. Paliathanasis and L. Karpathopoulos , “Exact solutions of Bianchi I spacetimes which admit Confo rmal Killing vectors,” Gen. Rel. Grav. 47, no. 2, 15 (2015) doi:10.1007/s10714-015-1856-x

  52. [53]

    Exact Static Cyli ndrical Solution to Conformal Weyl Gravity,

    J. L. Said, J. Sultana and K. Z. Adami, “Exact Static Cyli ndrical Solution to Conformal Weyl Gravity,” Phys. Rev. D 85, 104054 (2012) doi:10.1103/PhysRevD.85.104054

  53. [54]

    Exact String-Like Solutions in Conformal Gravity,

    Y. Verbin and Y. Brihaye, “Exact String-Like Solutions in Conformal Gravity,” Gen. Rel. Grav. 43, 2847 (2011) doi:10.1007/s10714-011-1209-3 19

  54. [55]

    Exact solutions of Einstein conform al scalar equations,

    J. D. Bekenstein, “Exact solutions of Einstein conform al scalar equations,” Annals Phys. 82, 535 (1974). doi:10.1016/0003- 4916(74)90124-9

  55. [56]

    Laporta and E

    B. S. DeWitt, “Quantum Field Theory in Curved Space-Tim e,” Phys. Rept. 19, 295 (1975). doi:10.1016/0370- 1573(75)90051-4

  56. [57]

    Trace Anomaly of a Conformally Invariant Qu antum Field in Curved Space-Time,

    R. M. Wald, “Trace Anomaly of a Conformally Invariant Qu antum Field in Curved Space-Time,” Phys. Rev. D 17, 1477 (1978). doi:10.1103/PhysRevD.17.1477

  57. [58]

    Quantum Fields in Curv ed Space

    N. D. Birrell and P. C. W. Davies, “Quantum Fields in Curv ed Space”

  58. [59]

    Quantum Field Theory in Curved Spacetime

    L. H. Ford, “Quantum field theory in curved space-time,” In *Campos do Jordao 1997, Particles and fields* 345-388 [gr-qc/9707062]

  59. [60]

    Exact Vacuum Solution to Conformal Weyl Gravity and Galactic Rotation Curves,

    P. D. Mannheim and D. Kazanas, “Exact Vacuum Solution to Conformal Weyl Gravity and Galactic Rotation Curves,” Astrophys. J. 342, 635 (1989). doi:10.1086/167623

  60. [61]

    Conformal Cosmology With No Cosmologi cal Constant,

    P. D. Mannheim, “Conformal Cosmology With No Cosmologi cal Constant,” Gen. Rel. Grav. 22, 289 (1990). doi:10.1007/BF00756278

  61. [62]

    Weyl vs. Conformal,

    G. K. Karananas and A. Monin, “Weyl vs. Conformal,” Phys . Lett. B 757, 257 (2016) doi:10.1016/j.physletb.2016.04.001

  62. [63]

    Canonical gravity with fermion s,

    M. Bojowald and R. Das, “Canonical gravity with fermion s,” Phys. Rev. D 78, 064009 (2008) doi:10.1103/PhysRevD.78.064009

  63. [64]

    Conformal Invariance and Torsion in Gener al Relativity,

    J. W. Maluf, “Conformal Invariance and Torsion in Gener al Relativity,” Gen. Rel. Grav. 19, 57 (1987). doi:10.1007/BF01119811

  64. [65]

    Reconstruction of Spinor From Fierz Ide ntities,

    Y. Takahashi, “Reconstruction of Spinor From Fierz Ide ntities,” Phys. Rev. D 26, 2169 (1982). doi:10.1103/PhysRevD.26.2169

  65. [66]

    Representation-independent manipulations with Dirac matrices and spinors

    P. B. Pal, “Representation-independent manipulation s with Dirac spinors,” physics/0703214 [physics.ed-ph]

  66. [67]

    Generalized Fierz identities

    J. F. Nieves and P. B. Pal, “Generalized Fierz identitie s,” Am. J. Phys. 72, 1100 (2004) doi:10.1119/1.1757445 [hep-ph/0306087]

  67. [68]

    Conformal Standard Model,

    L. Fabbri, “Conformal Standard Model,” Gen. Rel. Grav. 44, 3127 (2012) doi:10.1007/s10714-012-1440-6 [arXiv:1107 .0466 [gr-qc]]

  68. [69]

    Weyl Scalings And Spinor Mat ter Interactions In Scalar - Tensor Theories Of Gravitation ,

    T. Dereli and R. W. Tucker, “Weyl Scalings And Spinor Mat ter Interactions In Scalar - Tensor Theories Of Gravitation ,” Phys. Lett. 110B, 206 (1982). doi:10.1016/0370-2693(82)91237-0

  69. [70]

    Conformal Gravity with Dirac Matter

    L. Fabbri, “Conformal Gravity with Dirac Matter,” Anna les Fond. Broglie 38, 155 (2013) [arXiv:1101.2334 [gr-qc]]

  70. [71]

    Metric-Torsional Conformal Gravity

    L. Fabbri, “Metric-Torsional Conformal Gravity,” Phy s. Lett. B 707, 415 (2012) doi:10.1016/j.physletb.2012.01.008 [arXiv:1101.1761 [gr-qc]]

  71. [72]

    Conformal Gravity with Electrodynamics for Fermion Fields and their Symmetry Breaking Mechanism

    L. Fabbri, “Conformal Gravity with Electrodynamics fo r Fermion Fields and their Symmetry Breaking Mechanism,” In t. J. Geom. Meth. Mod. Phys. 11, no. 3, 1450019 (2014) doi:10.1142/S0219887814500194 [ar Xiv:1205.5386 [gr-qc]]