The Newtonian limit of fourth and higher order gravity ∗
Ines Qu, Hans‐Jürgen Schmidt
Abstract
Ines Qu, Hans‐Jürgen Schmidt
Abstract
We consider the Newtonian limit of the theory based on the Lagrangian ( p∑ L = R + k=0 ak R ✷ k R √−g The gravitational potential of a point mass turns out to be a combination of Newtonian and Yukawa terms. For sixth-order gravity (p = 1) the coefficients are calculated explicitly. For general p one gets ( p∑ Φ = m/r 1 + ci exp(−r/li) i=0 with ∑ p i=0 ci = 1/3. Therefore, the potential is always unbounded near the origin. Wir betrachten den Newtonschen Grenzwert der durch den Lagrangian
OpenAlex reports 40 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
We consider the Newtonian limit of the theory based on the Lagrangian ( p∑ L = R + k=0 ak R ✷ k R √−g The gravitational potential of a point mass turns out to be a combination of Newtonian and Yukawa terms. For sixth-order gravity (p = 1) the coefficients are calculated explicitly. For general p one gets ( p∑ Φ = m/r 1 + ci exp(−r/li) i=0 with ∑ p i=0 ci = 1/3. Therefore, the potential is always unbounded near the origin. Wir betrachten den Newtonschen Grenzwert der durch den Lagrangian
Key concepts: Physics, Newtonian potential, Yukawa potential, Newtonian fluid, Limit (mathematics), Newtonian limit, Gravitational potential, Gravitation