scholarly journals Conformal dynamical equivalence and applications

2011 ◽  
Vol 283 ◽  
pp. 012035 ◽  
Author(s):  
N K Spyrou
2008 ◽  
Vol 59 (2) ◽  
pp. 417-427 ◽  
Author(s):  
Thilo Gross ◽  
Ulrike Feudel

2012 ◽  
Vol 14 (10) ◽  
pp. 105014 ◽  
Author(s):  
Helge Aufderheide ◽  
Lars Rudolf ◽  
Thilo Gross

2012 ◽  
Vol 21 (04) ◽  
pp. 1250034 ◽  
Author(s):  
YI ZHANG ◽  
YUNGUI GONG ◽  
ZONG-HONG ZHU

Because of the dynamical equivalence between the f(R) gravity and the Brans-Dicke theory, the dynamical equation in the f(R) gravity is suggested to be derived from a view point of thermodynamics here. By a conformal transformation, the Brans–Dicke theory in the Jordan frame could be expressed as a minimal coupling scalar field theory in Einstein frame. Using the entropy-area relation [Formula: see text], the correct Friedmann equations could be gotten in both frames. Furthermore, we also discuss the corresponding generalized Misner–Sharp energies for theoretical consistence.


2017 ◽  
Vol 474 (3) ◽  
pp. 3740-3745 ◽  
Author(s):  
Diogo Belloni ◽  
Pavel Kroupa ◽  
Helio J Rocha-Pinto ◽  
Mirek Giersz

Abstract In order to allow a better understanding of the origin of Galactic field populations, dynamical equivalence of stellar-dynamical systems has been postulated by Kroupa and Belloni et al. to allow mapping of solutions of the initial conditions of embedded clusters such that they yield, after a period of dynamical processing, the Galactic field population. Dynamically equivalent systems are defined to initially and finally have the same distribution functions of periods, mass ratios and eccentricities of binary stars. Here, we search for dynamically equivalent clusters using the mocca code. The simulations confirm that dynamically equivalent solutions indeed exist. The result is that the solution space is next to identical to the radius–mass relation of Marks & Kroupa, $\left( r_{\rm h}/{\rm pc} \right)= 0.1^{+0.07}_{-0.04}{\, } \left( M_{\rm ecl}/{\rm M}_{\odot } \right)^{0.13\pm 0.04}$. This relation is in good agreement with the observed density of molecular cloud clumps. According to the solutions, the time-scale to reach dynamical equivalence is about 0.5 Myr which is, interestingly, consistent with the lifetime of ultra-compact H ii regions and the time-scale needed for gas expulsion to be active in observed very young clusters as based on their dynamical modelling.


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