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Responder a RE: Prueba de foros.
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Anónimo, modificado hace 7 meses.
RE: Prueba de foros.
https://failfake.com/pl/31-t-shirt-z-nadrukiem-meski
koszulki męskie
Strictly speaking, the phase in Weyl's theory is not the same as the (universal) phase in quantum formalism; they differ by a factor resulting from the electric charge of a given particle. The principal property on which Weyl's theory is based is the presence of a so-called continuous symmetry group (see §A.7, last paragraph) for each P event in space-time. In Weyl's original theory, the symmetry group consisted of all positive real numbers, which allowed scaling of the gauge. These potential numerical factors are simply positive real numbers, marked by mathematicians by the symbol ℝ +, hence the associated symmetry group is sometimes referred to as the multiplicative ℝ + group. In the later version of Weyl's theory, which has a more direct physical meaning, the elements of the group are rotations on the complex plane (without reflections) - such a group is referred to as SO (2) or U (1), and its elements are complex numbers eiθ with a unit module, representing different angles of rotation of the unit circle on the Wessel complex plane, where I simply designate this circle with the unit radius as S1. It may be noted (regarding this entry, see also the last paragraph of §A.7, which also mentions the concept of the group), that the letter 'O' in 'SO (2)' comes from the word 'orthogonal', which means in practice that we are dealing with a group of rotations (i.e. transformations maintaining orthogonality, i.e. the property of right angles, which in the case of rotations in 2 dimensions is written as "SO (2)"). The letter 'S' comes from the word 'special', which means that reflections are excluded. The letter "U" in the notation "U (1)" comes from the word "unitary" - that is: maintaining unit norms
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[quote=Anónimo][url=https://failfake.com/pl/31-t-shirt-z-nadrukiem-meski]https://failfake.com/pl/31-t-shirt-z-nadrukiem-meski[/url] koszulki męskie [code]Strictly speaking, the phase in Weyl's theory is not the same as the (universal) phase in quantum formalism; they differ by a factor resulting from the electric charge of a given particle. The principal property on which Weyl's theory is based is the presence of a so-called continuous symmetry group (see §A.7, last paragraph) for each P event in space-time. In Weyl's original theory, the symmetry group consisted of all positive real numbers, which allowed scaling of the gauge. These potential numerical factors are simply positive real numbers, marked by mathematicians by the symbol ℝ +, hence the associated symmetry group is sometimes referred to as the multiplicative ℝ + group. In the later version of Weyl's theory, which has a more direct physical meaning, the elements of the group are rotations on the complex plane (without reflections) - such a group is referred to as SO (2) or U (1), and its elements are complex numbers eiθ with a unit module, representing different angles of rotation of the unit circle on the Wessel complex plane, where I simply designate this circle with the unit radius as S1. It may be noted (regarding this entry, see also the last paragraph of §A.7, which also mentions the concept of the group), that the letter 'O' in 'SO (2)' comes from the word 'orthogonal', which means in practice that we are dealing with a group of rotations (i.e. transformations maintaining orthogonality, i.e. the property of right angles, which in the case of rotations in 2 dimensions is written as "SO (2)"). The letter 'S' comes from the word 'special', which means that reflections are excluded. The letter "U" in the notation "U (1)" comes from the word "unitary" - that is: maintaining unit norms[/code] [url=https://failfake.com/pl/31-t-shirt-z-nadrukiem-meski]koszulki męskie[/url][/quote]
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