The Grr − Gtt is finite if the A(r) = 0. One of the possible choices is A(r) = Z = const. Is interesting hereby, what if X = ρ/2, then p(r) = 0 for any r and ρ(r) = 2 N/3. The metric outside the ball of star r > R is of Schwarzschild with mass M found from the condition what the metric functions are continues at the surface r = S of the star: Z = 1 − 4π ρS 2 = 1 − 2M/S > 0. II. THE ENERGY-MOMENTUM TENSOR OF THE HIGGS FIELD The Lagrangian of scalar field of the complex mass is found in Wikipedia 2016 (“Higgs boson”): L(φ, φ,ν ), see [3]. Of course, we have also the Lagrangian of Dark Matter or Dark Energy: f (t, x, y, z). The solution of L = f for φ can be easily found numerically, because it has only quadratic non-linearity. III. UPRISING OF THE SAINTS Uprising of the saints: are professors more “fat” than independent researches? Hello, we are small fishes only in our imagination
of them. The result is a concise material, covering the generalities of Boolean functions and their properties relevant in cryptography. 3 2. Boolean functions and their representations In the following chapters the vector space of all binary vectors of length n will be denoted as 𝔽𝑛2 . For two vectors 𝑎 = (𝑎1 , … , 𝑎 𝑛 ) and 𝑏 = (𝑏1 , … , 𝑏𝑛 ) in 𝔽𝑛2 we define the scalar product < 𝑎, 𝑏 > = 𝑎 1 𝑏1 ⊕ …⊕ 𝑎 𝑛 𝑏𝑛 , where all the operations are over a finite field with two elements 𝔽2 . The logical negation (or complement) of a Boolean function 𝑓 is 𝑓 = 𝑓 ⊕ 1 . Definition 2.1. A Boolean function 𝑓 of 𝑛 variables is a map from 𝔽𝑛2 to 𝔽2 . 𝐹𝑛 will be used to mark the set of all Boolean functions of 𝑛 variables. The value vector of a Boolean function is very important term when describing the function
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