Resumen Se presenta nuestra contribución por hacer de la dualidad onda- Partícula un fenómeno intuitivo a través de un análisis histórico que muestra los . PRINCIPALES CARACTERISTICAS DE DUALIDAD ONDA PARTICULA También llamada onda from ECBTI _1 at National Open and Distance. Oeuvre de Vanesa Muñoz, ” Dualidad Onda Partícula II”.

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An interaction as in a Feynman diagram is accepted as a calculationally convenient approximation where the outgoing legs are known to be simplifications of the propagation and the internal lines are for some order in an expansion of the field interaction.

However, in Albert Einstein took Planck’s black body model to produce his solution to another outstanding problem of the day: Parallel arguments apply to pure wave states. The field permits solutions that follow the wave equation, which are referred to as the wave functions.

But the wave onra of their motion become more difficult to observe as their wavelengths become shorter A dramatic series of experiments emphasizing ondx action of gravity in relation to wave—particle duality was conducted in the s using the neutron interferometer. Alternative views are also presented here. Furthermore, classical electrodynamics was not the only classical theory rendered incomplete. Thus, the he established the validity of Einstein’s photoelectric equation instead of disproving it.

Lettere al Nuovo Cimento. The resulting Huygens—Fresnel principle was extremely successful at reproducing light’s behavior and was subsequently supported by Thomas Young ‘s discovery of interference by dialidad double-slit experiment. The pilot wave theory was initially rejected because it generated non-local effects when applied to systems involving more than one particle.


Turning the reasoning around, ordinary quantum mechanics can be deduced as a specialized consequence of quantum field theory.

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We are faced with a new kind of difficulty. Although the use of the wave-particle duality has worked well in physics, the meaning or interpretation has not been satisfactorily resolved; see Interpretations of quantum mechanics.

Following the development of quantum field theory the ambiguity disappeared. This double nature of radiation and of material corpuscles Since the demonstrations of wave-like properties in photons and electronssimilar experiments have been conducted with neutrons and protons.

Only photons of a high enough frequency above a certain threshold value could knock an electron free.

De Broglie’s formula was confirmed three years later for electrons which differ from photons in having a rest mass with the observation of electron diffraction in two independent experiments.

For particles with mass this equation has solutions that follow the form of the wave equation.

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If one now shines a very intense beam of low-frequency light upon the same metal, a whole slew of electrons are ejected; however they possess the same low energy, there are merely more of them. Up quark antiquark Down quark antiquark Charm quark antiquark Strange quark partciula Top quark antiquark Bottom quark antiquark.

For this reason, in Arthur Eddington [54] coined the name ” wavicle ” to describe the objects although it is not regularly used today. Superpartners Gauginos Gluino Gravitino Photino. The best illustration of the pilot-wave model was given by Couder’s “walking droplets” experiments, [20] demonstrating the pilot-wave behaviour in a macroscopic mechanical analog.


It expresses the inability of the classical concepts “particle” or “wave” to fully describe the behavior of quantum-scale objects. Mathematics and Foundations, 3 4also arXiv: Low-frequency light only ejects low-energy electrons because each electron is excited by the absorption of a single photon. Particle impacts make visible the interference pattern of waves. Just as it is nonsensical to discuss the precise location of a wave on a string, particles do not have perfectly precise positions; likewise, just as it is nonsensical to discuss the wavelength of a “pulse” wave traveling down a string, particles do not have perfectly precise momenta which corresponds to the inverse of wavelength.

Mead has cut the Gordian knot of quantum complementarity. Photon Gluon W and Z bosons. According to the classical theory of light and matter, the strength or amplitude of a light wave was in proportion to its brightness: However the value of Planck’s constant determined from his experiments came out to be very close to the original value. Einstein’s “light quanta” would not be called photons untilbut even in they represented the quintessential example of wave-particle duality.

This became known as the black body problem.

The deflection of the trajectory of each diffracted photon was explained as ona to quantized momentum transfer from the spatially regular structure of the diffracting crystal.

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