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Quantum Mechanics (this is a sophomore/junior
Quantum Mechanics (this is a sophomore/junior

... unknown to students, so they should be able to derive it themselves, with a little help from me. This is why it is possible to use a mixed lecture-discussion format here. My approach is to present students with experimental findings and then to ask them to try and explain the experiments. Discoveri ...
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... no quantum numbers other than energy, and so the only quantum number that can separate two electrons is the spin. One electron can have spin up and the other spin down. So we can have at most two electrons. In the other shells we can have more electrons because the state has other quantum numbers su ...
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PPT - LSU Physics & Astronomy

... loss in order to maximize the extraction of the available phase information in an interferometer. Our approach optimizes over the entire available input Hilbert space with no constraints, other than fixed total initial photon number. ...
In the early 1930s, the relativistic electron
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... Note how Table 6.1 is set up. For n=1, the only allowed possibilities are ℓ=mℓ=0. For this case, Beiser lists the three solutions R, , and . For n=2, ℓ can be either 0 or 1. If ℓ=0 then mℓ=0. If ℓ=1 then mℓ=0 and mℓ=1 are allowed. The solutions for mℓ=1 are the same. Beiser tabulates the three ...
Discussion Class 7
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... Discussion Class 7 19 October 2007 1. The induced dipole moment of a neutral atom is approximately proportional to the external electric field: p = αE The constant of proportionality α is called atomic polarizability. Now consider a hydrogen atom in its ground state. The electron cloud has a charge ...
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Variation of the Gravitational Constant and its Consequences

... experience.1 It is reasonable to extrapolate and suggest that in the limit of zero time, gravity could have been infinitely strong or at least extremely large.2 Enough to say that at some early moment after t = 0 it would surely have been as strong as the electromagnetic field we know today. This le ...
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... mechanical. Note that if factors of ~ and c are made explicit in Eqn. (3), our dimensional analysis is consistent with that microscopic calculation. As seen from Eqn. (4), the BICEP result suggests a scale of inflation of Einflation ≈ 2 × 1016 GeV. Remarkably, that same scale appears in quite a diff ...
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QUANTUM TUNNELING AND SPIN by Robert J

... The SG experiment demonstrates that the act of measuring something can affect its state. If the second SG experiment had not been done, the third SG experiment would have found only a single beam of particles. The act of measuring the spins of those particles in an orthogonal direction affected the ...
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... then deflecting them with a magnetic field. (a) Velocity selector: When a charged particle travels through crossed E and B fields (both of which fill the region below), the trajectory will be undeflected (continuing in a straight line) only if the velocity has a certain relationship to E and B. This ...
The qubits and the equations of physics
The qubits and the equations of physics

... Information Theory where the spin is the fundamental qubit and the massive particle is its carrier whose dynamical evolution is enslaved by the spin dynamics. Both degrees of freedom use the same clock (a ...
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Gedanken and real experiments in modern physics - IPN-Kiel

... angle the measurements exhibits some non-trivial correlations. The existence of such correlation worried Einstein, it seemed to him that information about the outcome of Alice’s measurement must be somehow transferred to Bob’s particle, otherwise he could not explain the correlations. These argument ...
Common notions from hep-th
Common notions from hep-th

... ĝab again describes some simply geometry. The transformation then involves mapping a given state of the CFT in one geometry to a new state in a new geometry. The utility of this approach will be that we may have a better understanding into the physics of the second state but by applying the inverse ...
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Document

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History of quantum field theory

In particle physics, the history of quantum field theory starts with its creation by Paul Dirac, when he attempted to quantize the electromagnetic field in the late 1920s. Major advances in the theory were made in the 1950s, and led to the introduction of quantum electrodynamics (QED). QED was so successful and ""natural"" that efforts were made to use the same basic concepts for the other forces of nature. These efforts were successful in the application of gauge theory to the strong nuclear force and weak nuclear force, producing the modern standard model of particle physics. Efforts to describe gravity using the same techniques have, to date, failed. The study of quantum field theory is alive and flourishing, as are applications of this method to many physical problems. It remains one of the most vital areas of theoretical physics today, providing a common language to many branches of physics.
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