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... The force between the electric field of the gold atom of charge Z2 and the incoming alpha particle of charge Z1 = 4 is found by ...
... The force between the electric field of the gold atom of charge Z2 and the incoming alpha particle of charge Z1 = 4 is found by ...
Read Notes #1
... The force between the electric field of the gold atom of charge Z2 and the incoming alpha particle of charge Z1 = 4 is found by ...
... The force between the electric field of the gold atom of charge Z2 and the incoming alpha particle of charge Z1 = 4 is found by ...
XXth century_physics (1)
... nucleus is equal to the atomic number and not to half the atomic weight seems to me very promising. This idea has already been used by Bohr in his theory of the constitution of atoms. The strongest and most convincing evidence in support of this hypothesis will be found in a paper by Moseley in Phil ...
... nucleus is equal to the atomic number and not to half the atomic weight seems to me very promising. This idea has already been used by Bohr in his theory of the constitution of atoms. The strongest and most convincing evidence in support of this hypothesis will be found in a paper by Moseley in Phil ...
what is time in some modern physics theories: interpretation problems
... Iamblichus’s ideas) [Proclus 2011] has developed kind of time and eternity dialectics. Time for him is duration, fluidity, continuity. Time is (again in Plato`s spirit) a motile image of eternity and eternity is a fixed image of time. Time is associated with motion and for its flow something to forc ...
... Iamblichus’s ideas) [Proclus 2011] has developed kind of time and eternity dialectics. Time for him is duration, fluidity, continuity. Time is (again in Plato`s spirit) a motile image of eternity and eternity is a fixed image of time. Time is associated with motion and for its flow something to forc ...
$doc.title
... There are as many states as there are possible n,m combinations (N.B. n & m are positive) Two distinct wave functions are DEGENERATE if they have the same energy. e.g. the states 1,3 and 3,1 are degenerate if a = b If a/b is irrational there are no degeneracies ...
... There are as many states as there are possible n,m combinations (N.B. n & m are positive) Two distinct wave functions are DEGENERATE if they have the same energy. e.g. the states 1,3 and 3,1 are degenerate if a = b If a/b is irrational there are no degeneracies ...
Wave function collapse
... a subset of observables can be fixed at any given moment. A maximally determined state obtains by fixing a maximal set of simultaneously measurable (“compatible”) observables, e.g. the position components. But there will be other observables, here the momenta, which do not posses definite values in ...
... a subset of observables can be fixed at any given moment. A maximally determined state obtains by fixing a maximal set of simultaneously measurable (“compatible”) observables, e.g. the position components. But there will be other observables, here the momenta, which do not posses definite values in ...
Renormalization
In quantum field theory, the statistical mechanics of fields, and the theory of self-similar geometric structures, renormalization is any of a collection of techniques used to treat infinities arising in calculated quantities.Renormalization specifies relationships between parameters in the theory when the parameters describing large distance scales differ from the parameters describing small distances. Physically, the pileup of contributions from an infinity of scales involved in a problem may then result in infinities. When describing space and time as a continuum, certain statistical and quantum mechanical constructions are ill defined. To define them, this continuum limit, the removal of the ""construction scaffolding"" of lattices at various scales, has to be taken carefully, as detailed below.Renormalization was first developed in quantum electrodynamics (QED) to make sense of infinite integrals in perturbation theory. Initially viewed as a suspect provisional procedure even by some of its originators, renormalization eventually was embraced as an important and self-consistent actual mechanism of scale physics in several fields of physics and mathematics. Today, the point of view has shifted: on the basis of the breakthrough renormalization group insights of Kenneth Wilson, the focus is on variation of physical quantities across contiguous scales, while distant scales are related to each other through ""effective"" descriptions. All scales are linked in a broadly systematic way, and the actual physics pertinent to each is extracted with the suitable specific computational techniques appropriate for each.