β - Indico
... 5. Aharonov Y., Cohen E., Elitzur A.C. (2012), Coexistence of past and future measurements’ effects, predicted by the Two-State-Vector-Formalism and revealed by weak measurement. Submitted to Phys. Rev. A. http://arxiv.org/abs/1207.0667 . 6. Aharonov Y., Cohen E., Grossman D., Elitzur A.C. (2012), C ...
... 5. Aharonov Y., Cohen E., Elitzur A.C. (2012), Coexistence of past and future measurements’ effects, predicted by the Two-State-Vector-Formalism and revealed by weak measurement. Submitted to Phys. Rev. A. http://arxiv.org/abs/1207.0667 . 6. Aharonov Y., Cohen E., Grossman D., Elitzur A.C. (2012), C ...
Document
... Quantum Information – what for? • First, quantum computers can crack some of the strongest cryptographic systems (e.g. RSA) • Second, they might be useful for various other things as well (simulating quantum systems etc.) • Quantum cryptography provides new solutions to some cryptographic problems ...
... Quantum Information – what for? • First, quantum computers can crack some of the strongest cryptographic systems (e.g. RSA) • Second, they might be useful for various other things as well (simulating quantum systems etc.) • Quantum cryptography provides new solutions to some cryptographic problems ...
Quantum Chemistry and Spectroscopy (Chem 341)
... grade on the final exam. If something unusual happens that causes you to miss a second exam, we will work something out on a case-by-case basis depending upon the situation. Problem sets: There will be 4 graded problem sets, which, together, comprise a significant portion (one fourth) your course gr ...
... grade on the final exam. If something unusual happens that causes you to miss a second exam, we will work something out on a case-by-case basis depending upon the situation. Problem sets: There will be 4 graded problem sets, which, together, comprise a significant portion (one fourth) your course gr ...
Quantum computing with nanoscale infrastructure
... do with something called ‘entanglement’, simply meaning that entangled states of the qubit register cannot be written as a product, like e.g. |0010110101>, similar to a single classical configuration. The quantum register (See Figure 1, overleaf) allows configuration mixing leading to non-classical ...
... do with something called ‘entanglement’, simply meaning that entangled states of the qubit register cannot be written as a product, like e.g. |0010110101>, similar to a single classical configuration. The quantum register (See Figure 1, overleaf) allows configuration mixing leading to non-classical ...
Quantum dynamics with ~10 6 - Weizmann Institute of Science
... Asher Peres (1984): distance between same state evolved by close Hamiltonians grows faster for (underlying) classical chaotic dynamics ??? H H n exp i 2 exp i 1 n ...
... Asher Peres (1984): distance between same state evolved by close Hamiltonians grows faster for (underlying) classical chaotic dynamics ??? H H n exp i 2 exp i 1 n ...
The Theory of Everything
... explain the behavior of the protectorates we have mentioned as it evolved historically. In solid-state physics, the experimental tools available were mainly long-wavelength, so that one needed to exploit the atomic perfection of crystal lattices to infer the rules. Imperfection is always present, bu ...
... explain the behavior of the protectorates we have mentioned as it evolved historically. In solid-state physics, the experimental tools available were mainly long-wavelength, so that one needed to exploit the atomic perfection of crystal lattices to infer the rules. Imperfection is always present, bu ...
Nextnano_NEGF - Walter Schottky Institut
... Determination of wave functions and bound states OUTPUT ...
... Determination of wave functions and bound states OUTPUT ...
... Several years ago, we pointed out that another consequence of the analogy with the artificial atom is that we may observe physics connected with the Kondo problem in quantum dots. The Kondo problem usually refers to the coupling of the electron spins localized on an impurity atom to the spin of the ...
First lecture, 7.10.03
... 1. Prepare a state |i> (by measuring a particle to be in that state; see 4) 2. Let Schrödinger do his magic: |i> |f>=U(t) |i>, deterministically 3. Upon a measurement, |f> some result |n> , randomly 4. Forget |i>, and return to step 2, starting with |n> as new state. ...
... 1. Prepare a state |i> (by measuring a particle to be in that state; see 4) 2. Let Schrödinger do his magic: |i> |f>=U(t) |i>, deterministically 3. Upon a measurement, |f> some result |n> , randomly 4. Forget |i>, and return to step 2, starting with |n> as new state. ...
pure
... Note: in fact, the SEB doesn’t appear like this. It is more distorted. Actually it is proved the SEB is determined by four points [Hayashi et. al ‘04]. ...
... Note: in fact, the SEB doesn’t appear like this. It is more distorted. Actually it is proved the SEB is determined by four points [Hayashi et. al ‘04]. ...