Starting from the classical Newton's second law which, according to our\nassumption, is valid in any instantaneous inertial rest frame of body that\nmoves in Minkowskian space-time we get the relativistic equat
motivating the pursuit of an axiomatic description of entanglement akin to the laws of thermodynamics. A long-standing open problem has been to establish a true second law of entanglement, and in particular a unique function that governs all transformations between entangled systems, mirroring...
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In this paper we will establish a second law beyond the linearized approximation for a large class of theories. Our approach will be to treat these theories as EFTs, ordering terms in the equations of motion according to how many derivatives they contain. The lowest order terms are the 2-...
[2,3,4,5,6,7]. This result can be regarded as a derivation of the second law of thermodynamics from statistical mechanics. It is natural to ask whether the second law conversely characterizes the Gibbs distribution or not. This question has been traditionally studied in terms of passivity [...
Derivation of the Boussinesq-type approximation In short we state all the steps, though they overlap with [8] (and [10], [11]) to some extent. This is convenient for the reader since we give clear guidance and correct some misprints in [8]. Moreover, we think that this provides a be...
Sound sources in the world are experienced as stable even when intermittently obscured, implying perceptual completion mechanisms that “fill in” missing sensory information. We demonstrate a filling-in phenomenon in which the brain extrapolates the sta
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9Altmetric Abstract The self coupling[Math Processing Error]λof the Higgs boson in the Standard Model may show critical behavior, i.e. the Higgs potential may have a point at an energy scale[Math Processing Error]∼1017−18GeV where both the first and second derivatives (almost) vanish....
(10) In order to see that δpen is indeed very small during SR, consider the equation of motion for δφ [80,86]: δφ¨ + 3H δφ˙ − ∇2δφ a2 + V δφ = 0. In momentum space this becomes (11) δφ¨k + 3H δφ˙k + k2 a2 δφk + V δφk = 0. (12)...