
The initialization and manipulation of quantum information
... increase towards the limiting value of 2T1 . The very long spin coherence times we measure show that Si:Bi is well suited for storing quantum information. We have flipped the electron spin in a time of 13 ns, and find T2 = 2 ms: over 105 times longer. We conclude that quantum information processing ...
... increase towards the limiting value of 2T1 . The very long spin coherence times we measure show that Si:Bi is well suited for storing quantum information. We have flipped the electron spin in a time of 13 ns, and find T2 = 2 ms: over 105 times longer. We conclude that quantum information processing ...
Entropy and Entanglement of Moving Two Atoms in a Squeezed
... squeezed states, even and odd coherent states and so on, don’t have minimum-uncertainty and they are nonclassical states, and have more applications for quantum communications and weak signal detection [8]. Quantum and classical correlations are at the heart of quantum information theory. It is seen ...
... squeezed states, even and odd coherent states and so on, don’t have minimum-uncertainty and they are nonclassical states, and have more applications for quantum communications and weak signal detection [8]. Quantum and classical correlations are at the heart of quantum information theory. It is seen ...
Perfect state transfer over distance
... The transfer of a quantum state from one part of a physical unit, e.g., a qubit, to another part is a crucial ingredient for many quantum information processing protocols [6]. Currently, there are several ways of moving data around in a quantum computer. While some methods transfer quantum states by ...
... The transfer of a quantum state from one part of a physical unit, e.g., a qubit, to another part is a crucial ingredient for many quantum information processing protocols [6]. Currently, there are several ways of moving data around in a quantum computer. While some methods transfer quantum states by ...
Nature template - PC Word 97
... An atom in the momentum state |-kL> can be reflected to the state |+kL> by a standing wave laser pulse. This is a process called Bragg diffration. After a time T0 = 2 ħk/mg≈1.2 ms for 87Rb, the state |+kL> evolves back into the state |-kL> because of the downwards acceleration of gravity g. Repeatin ...
... An atom in the momentum state |-kL> can be reflected to the state |+kL> by a standing wave laser pulse. This is a process called Bragg diffration. After a time T0 = 2 ħk/mg≈1.2 ms for 87Rb, the state |+kL> evolves back into the state |-kL> because of the downwards acceleration of gravity g. Repeatin ...
A quantum probability perspective on the nature of psychological uncertainty
... quantum probability (QP) theory (note that in this work by QP theory we simply mean the rules for how to assign probabilities to events from quantum theory; for more specific proposals see Aerts, 2009, or Atmanspacher, Romer & Wallach, 2006). We can acquire some preliminary intuition from models for ...
... quantum probability (QP) theory (note that in this work by QP theory we simply mean the rules for how to assign probabilities to events from quantum theory; for more specific proposals see Aerts, 2009, or Atmanspacher, Romer & Wallach, 2006). We can acquire some preliminary intuition from models for ...
Guidance Applied to Quantum Operations in Josephson
... where ac is the acceleration required or ‘commanded’, N’ is a constant known as the navigation constant and typically chosen between 4 and 8. ZEM is the Zero Effort Miss. The controls are moderated by 1/tgo2 where tgo is the time to go until the end of the operation. Classically proportional navigat ...
... where ac is the acceleration required or ‘commanded’, N’ is a constant known as the navigation constant and typically chosen between 4 and 8. ZEM is the Zero Effort Miss. The controls are moderated by 1/tgo2 where tgo is the time to go until the end of the operation. Classically proportional navigat ...