
Full-text PDF - American Mathematical Society
... of such eigenfunctions. More generally, when we refer to arithmetic QUE we are assuming that our states are always Hecke eigenstates. This is the means by which we circumvent the issue of the unlikely, but potentially possible, high multiplicities m(λ). It is known that the multiplicities of the spa ...
... of such eigenfunctions. More generally, when we refer to arithmetic QUE we are assuming that our states are always Hecke eigenstates. This is the means by which we circumvent the issue of the unlikely, but potentially possible, high multiplicities m(λ). It is known that the multiplicities of the spa ...
www.osa-opn.org 36 | OPN Optics & Photonics News Illustration by Phil Saunders/ spacechannel.org
... specific case of orbital angular momentum), the participating modes for the SPDC, SFWM and TOSPand in frequency/time, as well as sources of hyper-entangled DC processes. photon pairs with simultaneous entanglement in more than one degree of freedom. Alternate processes for generating non-classical l ...
... specific case of orbital angular momentum), the participating modes for the SPDC, SFWM and TOSPand in frequency/time, as well as sources of hyper-entangled DC processes. photon pairs with simultaneous entanglement in more than one degree of freedom. Alternate processes for generating non-classical l ...
Universal computation by multi-particle quantum walk
... • Establishes the computational power of interacting many-body systems such as the BoseHubbard model, fermions with nearest neighbour interactions, and more. Our method for performing universal computation exploits the connection between quantum walk and a discrete version of scattering theory [Farh ...
... • Establishes the computational power of interacting many-body systems such as the BoseHubbard model, fermions with nearest neighbour interactions, and more. Our method for performing universal computation exploits the connection between quantum walk and a discrete version of scattering theory [Farh ...
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... 3. The rQHW (rQGA) solution • The analysis provided in the critique section suggests the cure: rQHW • The rQHW concept was already addressed ...
... 3. The rQHW (rQGA) solution • The analysis provided in the critique section suggests the cure: rQHW • The rQHW concept was already addressed ...
The quantum phases of matter - Subir Sachdev
... and Kivelson9 described RVB physics in terms of the ‘quantum dimer’ model, and discovered a remarkable solvable point at which the simplest RVB state, the equal superposition of all nearest-neighbor singlet pairings, was the exact ground state. Fradkin and Kivelson10 showed that the quantum dimer mo ...
... and Kivelson9 described RVB physics in terms of the ‘quantum dimer’ model, and discovered a remarkable solvable point at which the simplest RVB state, the equal superposition of all nearest-neighbor singlet pairings, was the exact ground state. Fradkin and Kivelson10 showed that the quantum dimer mo ...
Lecture 7
... Problem 2 : Given x0,...,xN-1 with a guarantee that there is exactly one xi=1, find i Problem 3: Given x0,...,xN-1, compute OR(x0,...,xN-1) Problem 4: Given x0,...,xN-1 with guarantee that either exactly one xi=1 or no xi=1, decide which 2),3) are easier than 1), and 4) is easier than 2),3) ...
... Problem 2 : Given x0,...,xN-1 with a guarantee that there is exactly one xi=1, find i Problem 3: Given x0,...,xN-1, compute OR(x0,...,xN-1) Problem 4: Given x0,...,xN-1 with guarantee that either exactly one xi=1 or no xi=1, decide which 2),3) are easier than 1), and 4) is easier than 2),3) ...