pptx - University of Washington
... UFG is stable and superfluid at zero temperature Full thermodynamic properties are known from ab initio calculations and many of them were confirmed by experiment The quasiparticle spectrum was determined in ab initio calculations at zero and finite temperatures UFG has the highest (relative ...
... UFG is stable and superfluid at zero temperature Full thermodynamic properties are known from ab initio calculations and many of them were confirmed by experiment The quasiparticle spectrum was determined in ab initio calculations at zero and finite temperatures UFG has the highest (relative ...
Significant-Loophole-Free Test of Bells Theorem with Entangled Photons
... open if the setting choice or the measurement result of one side could be communicated to the other side in time to influence the measurement result there. Spacelike separation of each local measurement from both the distant setting choice and the distant measurement closes the locality loophole. In ...
... open if the setting choice or the measurement result of one side could be communicated to the other side in time to influence the measurement result there. Spacelike separation of each local measurement from both the distant setting choice and the distant measurement closes the locality loophole. In ...
Fibonacci Quanta - University of Illinois at Chicago
... ratio, φ = (1 + _5)/2. On the other hand, the quadratic equation may have imaginary roots. (This happens when a 2 + 4b is less than zero.) Under these circumstances, the formal solution does not represent a real number. For example, if i denotes the square root of minus one, then we could write ...
... ratio, φ = (1 + _5)/2. On the other hand, the quadratic equation may have imaginary roots. (This happens when a 2 + 4b is less than zero.) Under these circumstances, the formal solution does not represent a real number. For example, if i denotes the square root of minus one, then we could write ...
Probability in the Many-Worlds Interpretation of Quantum Mechanics
... a completely symmetrical situation there cannot be different names. So, the symmetry is not complete. We only assume that all relevant aspects of the three stations are completely identical, but we accept a possibility, and in fact a necessity, that there are other properties of the stations, like p ...
... a completely symmetrical situation there cannot be different names. So, the symmetry is not complete. We only assume that all relevant aspects of the three stations are completely identical, but we accept a possibility, and in fact a necessity, that there are other properties of the stations, like p ...
Energy loss by a fast charged particle moving parallel to a surface
... electrons which move only in the vacuum and which do not bulk states. This appears in particular in the existence of penetrate inside the medium at all. As far as we know this coupling between the cross sections for excitation of bulk phenomenon in the theory has not been discussed up to this and su ...
... electrons which move only in the vacuum and which do not bulk states. This appears in particular in the existence of penetrate inside the medium at all. As far as we know this coupling between the cross sections for excitation of bulk phenomenon in the theory has not been discussed up to this and su ...
Lecture Notes in Statistical Mechanics and Mesoscopics Doron Cohen
... ====== [2.10] Two quantum particles in a box with interaction The calculation of the partition function Z2 for two identical quantum particle in a box, is both interesting and later on useful for the purpose of calculating the second virial coefficient of an N particle gas. The Hamiltonian is: H= ...
... ====== [2.10] Two quantum particles in a box with interaction The calculation of the partition function Z2 for two identical quantum particle in a box, is both interesting and later on useful for the purpose of calculating the second virial coefficient of an N particle gas. The Hamiltonian is: H= ...
Chapter 7 Spin and Spin–Addition
... All particles leaving the Stern-Gerlach apparatus are then in an eigenstate of the Sz operator, i.e., their spin is either ”up” or ”down” with respect to the z-direction. Let’s now concentrate on the ”spin up” particles (in z-direction), that means we block up the ”spin down” in some way, and perfor ...
... All particles leaving the Stern-Gerlach apparatus are then in an eigenstate of the Sz operator, i.e., their spin is either ”up” or ”down” with respect to the z-direction. Let’s now concentrate on the ”spin up” particles (in z-direction), that means we block up the ”spin down” in some way, and perfor ...
