
Theory for an order-driven disruption of the liquid state in water
... ground state to be in by lowering its energy of interaction with the applied field. The grand potential per site of the liquid phase should be given by ᐉ = −q⑀ / 2 − , while for the aligned phase a = −log关1 + e+␥兴. Setting these two quantities equal gives the critical field at which the first-or ...
... ground state to be in by lowering its energy of interaction with the applied field. The grand potential per site of the liquid phase should be given by ᐉ = −q⑀ / 2 − , while for the aligned phase a = −log关1 + e+␥兴. Setting these two quantities equal gives the critical field at which the first-or ...
Pseudoholomorphic Curves and Mirror Symmetry
... geometry of the other (the name “mirror symmetry” comes from a graphical realization of the relation between Hodge numbers of the mirror manifolds). These ideas first arose from considerations in string theory, where it is shown that mirror manifolds give rise to the same physical theory when used a ...
... geometry of the other (the name “mirror symmetry” comes from a graphical realization of the relation between Hodge numbers of the mirror manifolds). These ideas first arose from considerations in string theory, where it is shown that mirror manifolds give rise to the same physical theory when used a ...
Applications of Clifford Algebras in Physics
... plane of rotation and whose magnitude gives half the angle of rotation. By using the rotor R = exp (Θ) instead of a product of three rotations about specified angles, one can avoid degeneracies in the Euler-angle decomposition. The simple rotor expression allows smooth rotations in a single plane an ...
... plane of rotation and whose magnitude gives half the angle of rotation. By using the rotor R = exp (Θ) instead of a product of three rotations about specified angles, one can avoid degeneracies in the Euler-angle decomposition. The simple rotor expression allows smooth rotations in a single plane an ...
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... usual interpretive axioms of quantum mechanics come into play only when the system interacts with something else, is ‘observed’. For the universe there is nothing else, and quantum mechanics in its traditional form has simply nothing else to say. It gives no way of, indeed no meaning of, picking out ...
... usual interpretive axioms of quantum mechanics come into play only when the system interacts with something else, is ‘observed’. For the universe there is nothing else, and quantum mechanics in its traditional form has simply nothing else to say. It gives no way of, indeed no meaning of, picking out ...
Document #05
... to deal with a wide range of electronic, electrical, and electro-magnetic devices. To fully understand how these devices work, their strengths and limitations, we require a basic and fundamental understanding of the physical laws of the universe that govern the interactions in electricity and magnet ...
... to deal with a wide range of electronic, electrical, and electro-magnetic devices. To fully understand how these devices work, their strengths and limitations, we require a basic and fundamental understanding of the physical laws of the universe that govern the interactions in electricity and magnet ...
Algebra/Geometry Institute Summer 2006
... Step 2 Align one side of the equilateral triangle with one side of the equilateral triangle on the second sheet. Trace the triangle so that the two copies of the triangle are now on one of the patty papers. Step 3 Continue tracing the triangles in this manner filing the paper with tessellations of e ...
... Step 2 Align one side of the equilateral triangle with one side of the equilateral triangle on the second sheet. Trace the triangle so that the two copies of the triangle are now on one of the patty papers. Step 3 Continue tracing the triangles in this manner filing the paper with tessellations of e ...