 
									
								
									The metron model - Max-Planck
									
... eigenvalue equation (9) yields trapped-mode solutions which approach zero for r → ∞ and have vanishing derivative at r = 0. The corresponding equations for the wave-guide (n = 0) and forced waves (n = 2) are characterized by zero-eigenvalue operators (en = 0) and non-zero source functions qn that de ...
                        	... eigenvalue equation (9) yields trapped-mode solutions which approach zero for r → ∞ and have vanishing derivative at r = 0. The corresponding equations for the wave-guide (n = 0) and forced waves (n = 2) are characterized by zero-eigenvalue operators (en = 0) and non-zero source functions qn that de ...
									CDMTCS Research Report Series
									
... pected from any “hypercomputation” beyond universal computability as defined by Turing. It should be always kept in mind that all our sense perceptions are derived from elementary discrete events, such as clicks in photon or particle detectors, even if they appear to be analog: the apparently smoot ...
                        	... pected from any “hypercomputation” beyond universal computability as defined by Turing. It should be always kept in mind that all our sense perceptions are derived from elementary discrete events, such as clicks in photon or particle detectors, even if they appear to be analog: the apparently smoot ...
									Quantum Computers - Computing Sciences
									
... Just like in the two slit experiment, where measuring the photons collapsed the probabilities, measuring a quantum bit collapses the bit into only one value. Which value is measured is random. So measuring our quantum bit that contains the values 0 and 1 will result in the bit taking on the value of ...
                        	... Just like in the two slit experiment, where measuring the photons collapsed the probabilities, measuring a quantum bit collapses the bit into only one value. Which value is measured is random. So measuring our quantum bit that contains the values 0 and 1 will result in the bit taking on the value of ...
									- Philsci
									
... phenomena it is about. Following the available literature, we will refer to such explanations as structural explanations. In order to illustrate our main claim, we will present two case studies, involving two of the most typical and puzzling quantum phenomena, namely Heisenberg’s Uncertainty Relatio ...
                        	... phenomena it is about. Following the available literature, we will refer to such explanations as structural explanations. In order to illustrate our main claim, we will present two case studies, involving two of the most typical and puzzling quantum phenomena, namely Heisenberg’s Uncertainty Relatio ...
									OPTICS14399
									
... Since the early days of quantum mechanics, it has been known that certain quantum states have a mysterious non-local behavior [1]. The phenomenon responsible for these non-local correlations among the subsystems of a composite quantum system is called entanglement [2]. Quantum entanglement, having n ...
                        	... Since the early days of quantum mechanics, it has been known that certain quantum states have a mysterious non-local behavior [1]. The phenomenon responsible for these non-local correlations among the subsystems of a composite quantum system is called entanglement [2]. Quantum entanglement, having n ...
									Quantum Phase Transitions
									
... h⇒| σ̂jz |⇒i = 0. Further, perturbation theory in 1/g shows that these features of the ground state are preserved for a finite range of large g values (indeed, for all g > gc ). One can visualize this ground state as one in which strong quantum fluctuations have destroyed the ferromagnetism, with th ...
                        	... h⇒| σ̂jz |⇒i = 0. Further, perturbation theory in 1/g shows that these features of the ground state are preserved for a finite range of large g values (indeed, for all g > gc ). One can visualize this ground state as one in which strong quantum fluctuations have destroyed the ferromagnetism, with th ...
									Lecture 12: Holevo`s theorem and Nayak`s bound
									
... We will first discuss some of the concepts that Holevo’s theorem concerns, and then state and prove the theorem itself. Although the theorem is difficult to prove from first principles, it turns out that there is a very simple proof that makes use of the strong subadditivity of the von Neumann entro ...
                        	... We will first discuss some of the concepts that Holevo’s theorem concerns, and then state and prove the theorem itself. Although the theorem is difficult to prove from first principles, it turns out that there is a very simple proof that makes use of the strong subadditivity of the von Neumann entro ...
									PPT - Fernando Brandao
									
... Gives first polynomial-time quantum algorithm for preparing Gibbs states of commuting models at high temperature. Caveat: At high temperature cluster expansion works well for computing local expectation values. (Open: How the two threshold T’s compare?) Q advantage: we get the full Gibbs state (e.g. ...
                        	... Gives first polynomial-time quantum algorithm for preparing Gibbs states of commuting models at high temperature. Caveat: At high temperature cluster expansion works well for computing local expectation values. (Open: How the two threshold T’s compare?) Q advantage: we get the full Gibbs state (e.g. ...
									Time evolution - MIT OpenCourseWare
									
... We consider the semi-classical problem of a spin-1/2 particle in a classical magnetic field. To each spin with spin angular momentum J is associated a magnetic moment µ = γS where γ is called the gyromagnetic ratio, a property of each spin-carrying particle (nucleus, electron, etc.). The energy of th ...
                        	... We consider the semi-classical problem of a spin-1/2 particle in a classical magnetic field. To each spin with spin angular momentum J is associated a magnetic moment µ = γS where γ is called the gyromagnetic ratio, a property of each spin-carrying particle (nucleus, electron, etc.). The energy of th ...
									The Universal Uncertainty Principle v1
									
... no need to introduce any additional physical concepts or postulates. In a second paper entitled “The Size of Fundamental Particles”, I applied the same principle again to calculate the diameter of the electron. As a result the size of the electron turned out to be smaller than 10.166 times the Planc ...
                        	... no need to introduce any additional physical concepts or postulates. In a second paper entitled “The Size of Fundamental Particles”, I applied the same principle again to calculate the diameter of the electron. As a result the size of the electron turned out to be smaller than 10.166 times the Planc ...
									in PPT
									
... Sinf(ρ) = -0.71 log2 .71 – 0.29 log2 .29 = 0.868 bits The eigenvalues of ρ are 0.242 and 0.758 and, therefore, the von Neumann entropy is: ...
                        	... Sinf(ρ) = -0.71 log2 .71 – 0.29 log2 .29 = 0.868 bits The eigenvalues of ρ are 0.242 and 0.758 and, therefore, the von Neumann entropy is: ...
									Peter Heuer - Quantum Cryptography Using Single and Entangled
									
... refraction of diamond. When illuminated, color centers fluoresce much like a quantum dot. Unlike quantum dots, color centers do not bleach or blink, making them more much more stable. However, since color centers are natural rather than manufactured, it is harder to create uniform single emitters th ...
                        	... refraction of diamond. When illuminated, color centers fluoresce much like a quantum dot. Unlike quantum dots, color centers do not bleach or blink, making them more much more stable. However, since color centers are natural rather than manufactured, it is harder to create uniform single emitters th ...
									1 The Postulates of Quantum Mechanics
									
... The time evolution of the state of a quantum system is described by |ψ(t)i = Û(t, t0 )|ψ(t0 )i, for some unitary operator Û. Comments • We have not got to this subject yet. I include it for completeness. • Under time evolution, a state |ψi moves through the space of states on a trajectory we can d ...
                        	... The time evolution of the state of a quantum system is described by |ψ(t)i = Û(t, t0 )|ψ(t0 )i, for some unitary operator Û. Comments • We have not got to this subject yet. I include it for completeness. • Under time evolution, a state |ψi moves through the space of states on a trajectory we can d ...
									Chemistry 4.2 notes - Bryant School District
									
... Atomic Orbitals and Quantum Numbers • Quantum numbers specify the properties of atomic orbitals and the properties of electrons in orbitals. • The principal quantum number, symbolized by n, indicates the main energy level occupied by the electron. 1, 2, 3, etc. as n increases the electron’s energy l ...
                        	... Atomic Orbitals and Quantum Numbers • Quantum numbers specify the properties of atomic orbitals and the properties of electrons in orbitals. • The principal quantum number, symbolized by n, indicates the main energy level occupied by the electron. 1, 2, 3, etc. as n increases the electron’s energy l ...
									3 Nov 08 - Seattle Central College
									
... “A scientific truth does not triumph by convincing its opponents and making them see the light, but rather because its opponents eventually die and a new generation grows up that is familiar with it.” (Max Planck, 1920) “All these fifty years of conscious brooding have brought me no nearer to the an ...
                        	... “A scientific truth does not triumph by convincing its opponents and making them see the light, but rather because its opponents eventually die and a new generation grows up that is familiar with it.” (Max Planck, 1920) “All these fifty years of conscious brooding have brought me no nearer to the an ...
									Annual Report 2003-2004 The Institute for Quantum Engineering, Science, and Technology
									
... Using SF6, we expect to reach Rayleigh numbers up to 2 x 1013 for σ = 0.8. Much of this parameter range is as yet unexplored by previous experiments. Some of it will overlap with results from experiments using cryogenic helium and thus will help to elucidate interesting questions provoked by that wo ...
                        	... Using SF6, we expect to reach Rayleigh numbers up to 2 x 1013 for σ = 0.8. Much of this parameter range is as yet unexplored by previous experiments. Some of it will overlap with results from experiments using cryogenic helium and thus will help to elucidate interesting questions provoked by that wo ...
 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									