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The Postulates of Quantum Mechanics Postulate 1 Postulate 2 H
The Postulates of Quantum Mechanics Postulate 1 Postulate 2 H

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... Putting it all together  Take the Hadamard code C  Reduce its degree as a bi-partite graph: C  C’.  Apply the hypergraph-product to C’: derive a quantum CSS code from a classical code.  Argue: the local constraints of the code are an NLTS local Hamiltonian. ...
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... the principal quantum number (n). B. the angular momentum quantum number (l). C. the magnetic quantum number (ml). D. the spin quantum number (ms). E. none of these choices is correct 21. Atomic orbitals developed using quantum mechanics A. describe regions of space in which one is most likely to fi ...
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... inward. These pinching forces are balanced by non-magnetic pressure gradient forces (for example, elastic forces for a solid metal, or compressed-gas pressures for a plasma). Find an expression for the pressure, p = p(r), inside the conductor for the uniform current distribution of part b), and sket ...
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... immense pressures at the depth of Saturn’s core. 4. Implausible. Any large impactor approaching Saturn would be broken up by tidal forces. 5. Implausible. Saturn’s high rotation would prevent an impactor from reaching its core. ...
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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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