1922
DOI: 10.1002/hlca.19220050415
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Über den 2,3,2′,3′‐Naphthindigo

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Cited by 32 publications
(48 citation statements)
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“…A long-standing question concerning 'massive gravity' is whether the so-called van-Dam-Veltman-Zakharov discontinuity [22] can be avoided. The 'discontinuity' is the fact that a massive graviton, as defined by the only ghost-free quadratic action, the Pauli-Fierz action [23], leads to physical predictions, such as light bending, which are significantly different from those of linearized general relativity, however small the graviton mass may be. A way to recover GR, proposed by Vainshtein [24], is to properly take into account nonlinearities of the theory.…”
Section: Massive Gravity and The Vainshtein Mechanismmentioning
confidence: 99%
“…A long-standing question concerning 'massive gravity' is whether the so-called van-Dam-Veltman-Zakharov discontinuity [22] can be avoided. The 'discontinuity' is the fact that a massive graviton, as defined by the only ghost-free quadratic action, the Pauli-Fierz action [23], leads to physical predictions, such as light bending, which are significantly different from those of linearized general relativity, however small the graviton mass may be. A way to recover GR, proposed by Vainshtein [24], is to properly take into account nonlinearities of the theory.…”
Section: Massive Gravity and The Vainshtein Mechanismmentioning
confidence: 99%
“…In this paper we do not pursue the interesting possibilities for lagrangian field theories on our hyperspaces M, nor do we attempt to describe higher-spin dynamics using the algebras A. There are many such exciting possibilities for future work, extending, for instance, the early considerations of Fierz [5] on higher-spin dynamics, or the more recent investigations of Fradkin and Vasiliev [4,6] on the realisation of higher-spin superalgebras A on interacting fields including gravity. We restrict ourselves here to one simple field-theoretical application: We consider gauge fields on the hyperspaces M. Since the vector fields X act as superderivations on functions of Y , they can be gauge covariantised by adding a gauge potential A transforming according to the same representation of the Lorentz group as X. Commutators of gauge-covariantised vector fields, i.e.…”
Section: 3mentioning
confidence: 99%
“…In 1961, Robert H. Dicke and Carl H. Brans proposed a scalartensor theory, known as Brans-Dicke (BD) theory, [1] to describe gravitation by incorporating Mach's principle. The foundation of this theory was built on the previous work of Pascual Jordan [2] as well as Markus Fierz, [3] and sometimes it is also referred to as Jordan-Fierz-Brans Dicke theory. In Einstein's general relativity (GR), the coupling constant between matter and spacetime is given by G (the Newtonian constant of gravitation).…”
Section: Introductionmentioning
confidence: 99%