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2003
DOI: 10.1088/0305-4470/36/18/315
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Harmonic potential as an effective limit of a discrete classical interaction

Abstract: Motivated by improving the understanding of the quantum-to-classical transition we use a simple model of classical discrete interactions for studying the discrete-to-continuous transition in the classical harmonic oscilator. A parallel is traced with gravity for stressing the relevance of such discrete interaction models. Fundamental interactions, according to quantum field theory, are realized through the exchange of interaction quanta-packets of matter-energy with defined quantum numbers, viz. momentum-energ… Show more

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Cited by 4 publications
(3 citation statements)
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“…Let us consider that the field-generating particle (gravitational or electric) is at the origin of the considered coordinate system and that the test particle is in the position r 0 with momentum p 0 and that r 0 < 1 with δr j << 1, this ensures that the two particles are very close to each other (such as inside a nucleus). We will also consider δt j << 1, this ensures that the iterative process approaches the continuous fields picture as expected, it is important to note that there are analytic approaches in which the fields are considered as discrete, [17][18][19] is not the case in question. Defining the time increment as being constant, i.e., δt j ≡ ω > 0, equations ( 11) and ( 10) then become…”
Section: Obtaining the Yukawa Potentialmentioning
confidence: 99%
“…Let us consider that the field-generating particle (gravitational or electric) is at the origin of the considered coordinate system and that the test particle is in the position r 0 with momentum p 0 and that r 0 < 1 with δr j << 1, this ensures that the two particles are very close to each other (such as inside a nucleus). We will also consider δt j << 1, this ensures that the iterative process approaches the continuous fields picture as expected, it is important to note that there are analytic approaches in which the fields are considered as discrete, [17][18][19] is not the case in question. Defining the time increment as being constant, i.e., δt j ≡ ω > 0, equations ( 11) and ( 10) then become…”
Section: Obtaining the Yukawa Potentialmentioning
confidence: 99%
“…O vetor posição x n = x nî , muda continuamente, descrevendo uma trajetória poligonal. Nesta abordagem a velocidade (momento linear se quisermos dar um tratamento semi-clássico [24]) muda discretamente. As variáveis contínuas tempo e posição entram na descrição do movimento como se fossem parâmetros discretos somente porque esses eventos de iteração são nossos pontos de referência para a contagem do tempo.…”
Section: Abordagem Iterativa Para O Oscilador Harmônico Simplesunclassified
“…At low values of n, this is sensible -we expect that the increased oscillations as we climb the eigenfunction ladder do indeed correspond to greater quantumness. However, this does not hold at high values of n. The correspondence principle dictates that the limit as n → ∞ of the harmonic oscillator [5] should yield a transition from quantum to classical behavior. As such, a monotonic increase in quantumness with n is not correct.…”
Section: Introductionmentioning
confidence: 99%