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Stationary states and time
Stationary states and time

... despite the decay, the WF does not reach zero at points corresponding to large displacements from the centre. As shown in the diagram, the WFs become small, but remain finite. This is because in the ‘particle in a box’ system the potential energy ...
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... The Bethe-Bloch equation describes the mean energy loss When a charged particle passes the layer of material with thickness x , the energy distribution of the δ-electrons and the fluctuations of their number (nδ) cause fluctuations of the energy losses ΔE The energy loss ΔE in a layer of material is ...
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Noncommutative space-time and Dirac constraints - Indico

... As the dispersion relations used by these models are quadratic in while the spatial momentum scale as z the models are in principle renormalizable by power counting arguments at least for z  3 . ...
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... Finally, on a cautionary note, while the phenomenon of quantum mechanical tunneling is well-established, it is difficult to access in a convincing experimental manner. Although a classical particle with energy E < V0 is unable to penetrate the barrier region, in a physical setting, one is usually co ...
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Aalborg Universitet Quantum Gravity Chromo Dynamics (QGCD) Javadi, Hossein; Forouzbakhsh, Farshid
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Terahertz Spectroscopy of CdSe Quantum Dots
Terahertz Spectroscopy of CdSe Quantum Dots

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The unbreakable code: Is this the lock?
The unbreakable code: Is this the lock?

... scheme is far more general and much more powerful than I originally anticipated; it works even with devices of dubious provenance. This means that you and your friend may purchase cryptographic equipment from any company, even from your competitors or enemies, and still be able to establish a secret ...
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... and minima are calculated according to Kirchhoff’s diffraction formula and compared with the measured values. 2. To calculate the uncertainty of momentum from the diffraction patterns of single slits of differing widths and to confirm Heisenberg’s uncertainty principle. Set-up and procedure Differen ...
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... ‘ruler’ model  Order along the ruler models event order: ‘before’ and ‘after’  But no notion of change - a non-process model  In physics the distance along the ruler is represented by the symbol ‘t’. ...
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Atomic Structure, angular momentum, electron orbitals

... hydrogen atom state with l = 2. For a given value of Lz, A. the angular momentum vector can point in any direction tangent to the cone for that value of Lz. B. the electron orbits along the corresponding red circle, so the orbit may or may not have the nucleus at its ...
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... SMALLER THAN 25 LARGER THAN 25 10) A source moves toward and observer and the observer moves away from the source at the same speed. Compared to the source frequency, the observed frequency is SMALLER EQUAL GREATER 11) Two loud speakers are working in phase, producing waves with a wavelength of 1.44 ...
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information, physics, quantum: the search for links

... Fourth and last no: No space, no time. Heaven did not hand down the word "time". Man invented it, perhaps positing hopefully as he did that "Time is Nature's way to keep everything from happening all at once" [79]. If there are problems with the concept of time, they are of our own creation! As Leib ...
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Bohr–Einstein debates



The Bohr–Einstein debates were a series of public disputes about quantum mechanics between Albert Einstein and Niels Bohr. Their debates are remembered because of their importance to the philosophy of science. An account of the debates was written by Bohr in an article titled ""Discussions with Einsteinon Epistemological Problems in Atomic Physics"". Despite their differences of opinion regarding quantum mechanics, Bohr and Einstein had a mutual admiration that was to last the rest of their lives.The debates represent one of the highest points of scientific research in the first half of the twentieth century because it called attention to an element of quantum theory, quantum non-locality, which is absolutely central to our modern understanding of the physical world. The consensus view of professional physicists has been that Bohr proved victorious, and definitively established the fundamental probabilistic character of quantum measurement.
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