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Heisenberg’s uncertainty

Ip = hG/c y is the Planck length. Since c6t < 6x, A and B are outside of each other s light cone and local field theory assures us that these two experiments can be performed completely independently of one another. Heisenberg s uncertainty principle, however, asserts that these two measurements will also yield an energy fluctuation on the order of AE > Ip. We know that the gravitational... [Pg.655]

Notice that in this example, the speed of the packet is inversely proportional to the packet s spatial size. While there is certainly nothing unique about this particular representation, it is interesting to speculate, along with Minsky, whether it may be true that, just as the simultaneous information about position and momentum is fundamentally constrained by Heisenberg s uncertainty relation in the physical universe, so too, in a discrete CA universe, there might be a fundamental constraint between the volume of a given packet and the amount of information that can be encoded within it. [Pg.663]

Heisenberg s uncertainty principle forced a change in thinking about how to describe the universe, hi a universe subject to uncertainty, many things cannot be measured exactly, and it is never possible to predict with certainty exactly what will occur next. This uncertainty has become accepted as a fundamental feature of the universe at the scale of electrons, protons, and neutrons. [Pg.468]

A survey spectrum covers a wide range of values of Eh, typically from OeV to 1000 eV or higher. The measured signals in Ekin would be converted to values of binding energy, and an ideal survey spectrum would appear as in Figure 2.4. Here it is assumed that the experiment is conducted with T— 0 K with an ideal source and detector, and furthermore that Heisenberg s uncertainty principle does not operate, the electrons have no spin and that all the electrons created leave the sample with no losses. [Pg.27]

According to Galilei, the observation of natural phenomena using suitable measuring instruments provides certain numerical values which must be related to one another the solution of the equations derived from the numbers allows us to forecast future developments. This led to the misunderstanding that knowledge could only be obtained in such a manner. The result was deterministic belief, which was disproved for microscopic objects by Heisenberg s uncertainty principle. On the macroscopic scale, however, it appeared that the deterministic approach was still valid. Determinism was only finally buried when deterministic chaos was discovered. [Pg.243]

The natural line width is determined by Heisenberg s uncertainty relation... [Pg.64]

Thnnelling has sometimes been regarded as a mysterious phenomenon by chemists. It is worth stressing, therefore, that tunnelling has the same firm foundation in quantum mechanics as zero-point energy, which is the most important component of a KIE both these phenomena are a consequence of Heisenberg s uncertainty principle. [Pg.212]

The ultimate (minimum) linewidth of an optical band is due to the natural or lifetime broadening. This broadening arises from the Heisenberg s uncertainty principle, AvAt < U2jt, Av being the full frequency width at half maximum of the transition and the time available to measure the frequency of the transition (basically, the life-... [Pg.10]

To explain this behaviour, physicists appeal to the very foundations of quantum theory. Because of their much reduced freedom to move in space, the particles can be considered to be more and more localised. Then, by Heisenberg s uncertainty principle, the spread in their velocities has to grow. In other words, some particles may have much higher velocities than those allowed by the temperature. A quantum pressure arises at high densities, when the mean distance between electrons becomes comparable with their associated wavelength... [Pg.130]

The rest of the atom is sparsely populated but also vibrant and dynamic. The ghostly electrons are arranged in vague clouds and have no clearly defined position. Heisenberg s Uncertainty Principle (1927) tells us that we can t pin-point their positions. Instead, we have to talk in terms of the probability of there being electrons of a certain energy in certain positions (or orbits) around the nucleus at certain times. [Pg.82]

Due to Heisenberg s uncertainty and Pauli s exclusion principles, the properties of a multifermionic system correspond to fermions being grouped into shells and subshells. The shell structure of the one-particle energy spectrum generates so-called shell effects, at different hierarchical levels (nuclei, atoms, molecules, condensed matter) [1-3]. [Pg.53]

Natural broadening occurs because of the finite lifetime (x) of the atom in the excited state. Heisenberg s uncertainty principle states that if we know the state of the atom, we must have uncertainty in the energy level. We assume that x for the ground state is infinity and therefore for a resonance line the natural width Av = IAtxx. [Pg.75]

Heisenberg s uncertainty principle and the necessity for quantum mechanics in the study of atomic structure... [Pg.1]

Let us now consider the increase in the spot size due to the effect of Heisenberg s uncertainty. When a particle is confined to pass through a small space of width Ay, at the tip, the uncertainty in the tangential component of the momentum of the particle is of the order of hi2 Ay, and the corresponding velocity component is h/2M Ayt. Thus the spread of the spot size at the screen by this uncertainty alone is... [Pg.95]

This is a statement of Heisenberg s uncertainty principle, namely... [Pg.27]

Describe how the photoelectric effect and electron diffraction demonstrate the particle-like character of radiation and the wave-like character of particles respectively. Show how Heisenberg s uncertainty principle embraces the concept of wave particle duality. [Pg.242]

Estimate the ground state energy using Heisenberg s uncertainty principle and compare with the exact result. [Pg.243]

While for some purposes it may be necessary to have accurate frequency definition, for others good time discrimination is useful. These are opposite requirements. Because of the Fourier relationship between frequency and time, the more precisely the time of a signal is known, the greater bandwidth of frequencies is necessary (there is a close analogy here with Heisenberg s uncertainty principle). Approximately, the time resolution t is the reciprocal of the bandwidth Bw, so that their product Bwr 1. [Pg.70]

F. A Measurement Process that Goes beyond Heisenberg s Uncertainty Relations... [Pg.501]

If we want to show that there are physical concrete situations not described by Heisenberg s uncertainty relations, it is necessary to predict the uncertainties, for the two conjugate noncommutative observables, for example, position, Ax, and the uncertainty in momentum, p, for the microparticle M, after the interaction with the photon, and then make their product and see whether they are contained in Heisenberg uncertainty measurement space. [Pg.550]


See other pages where Heisenberg’s uncertainty is mentioned: [Pg.2310]    [Pg.2894]    [Pg.389]    [Pg.1035]    [Pg.611]    [Pg.209]    [Pg.486]    [Pg.467]    [Pg.29]    [Pg.40]    [Pg.254]    [Pg.132]    [Pg.16]    [Pg.250]    [Pg.261]    [Pg.93]    [Pg.20]    [Pg.26]    [Pg.27]    [Pg.28]    [Pg.170]    [Pg.501]    [Pg.540]    [Pg.547]   


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