Transport properties of quantum-classical systems
... can be evaluated in the quantum-classical limit. For the present, however, it is convenient to first take a Wigner transform 关22兴 over all degrees of freedom, subsystem plus bath, and later single out the subsystem and bath degrees of freedom for different treatments. Introducing a coordinate repres ...
... can be evaluated in the quantum-classical limit. For the present, however, it is convenient to first take a Wigner transform 关22兴 over all degrees of freedom, subsystem plus bath, and later single out the subsystem and bath degrees of freedom for different treatments. Introducing a coordinate repres ...
Bormio2016_talk_JFSS
... Bohr & Mottelson Vol II “A vibrational mode of excitation is characterized by the property that it can be repeated a large number of times. The nth excited state of a specified mode can thus be viewed as consisting of n individual quanta. The quanta obey Bose statistics…” Page 330 “… but it might be ...
... Bohr & Mottelson Vol II “A vibrational mode of excitation is characterized by the property that it can be repeated a large number of times. The nth excited state of a specified mode can thus be viewed as consisting of n individual quanta. The quanta obey Bose statistics…” Page 330 “… but it might be ...
5 Quantum Theory of Radiation
... The interaction Ĥ2 couples to the intrinsic magnetic moment of the particles only. The intrinsic magnetic moment is the moment associated with spin angular momentum. Hence, the matrix element you calculated in (a) does not involve the total magnetic moment of the particles. The orbital component ha ...
... The interaction Ĥ2 couples to the intrinsic magnetic moment of the particles only. The intrinsic magnetic moment is the moment associated with spin angular momentum. Hence, the matrix element you calculated in (a) does not involve the total magnetic moment of the particles. The orbital component ha ...
INTRODUCTION TO WAVE PACKETS
... In linear approximation the wave packet is undistorted and undergoes a uniform translation ...
... In linear approximation the wave packet is undistorted and undergoes a uniform translation ...
Introduction to Single Molecular Magnet
... Yet, there is another kind of paramagnetic behavior exhibited by some metals which arises on the application of magnetic field that can be realized in a free electron gas mode. The density of states of free electron gas in absence of external magnetic field has equal number of up spins and down spins ...
... Yet, there is another kind of paramagnetic behavior exhibited by some metals which arises on the application of magnetic field that can be realized in a free electron gas mode. The density of states of free electron gas in absence of external magnetic field has equal number of up spins and down spins ...
Observable Measure of Quantum Coherence in Finite
... efficient route to measure the amount of quantum coherence carried by the state of a system in dimension d > 2. It is customary to employ quantifiers tailored to the scenario of interest, i.e., of not general employability, expressed in terms of ad hoc entropic functions, correlators, or functions o ...
... efficient route to measure the amount of quantum coherence carried by the state of a system in dimension d > 2. It is customary to employ quantifiers tailored to the scenario of interest, i.e., of not general employability, expressed in terms of ad hoc entropic functions, correlators, or functions o ...
Momentum - HRSBSTAFF Home Page
... A baseball of mass 0.145kg is pitched toward a batter with an initial velocity of 35m/s. If the batter hits the ball in the opposite direction at 45m/s, determine the force that is applied by the bat on the ball if the contact time was 0.013s. ...
... A baseball of mass 0.145kg is pitched toward a batter with an initial velocity of 35m/s. If the batter hits the ball in the opposite direction at 45m/s, determine the force that is applied by the bat on the ball if the contact time was 0.013s. ...
Whittaker Functions and Quantum Groups
... ) be the states of the top and bottom rows. The partition function then is a row transfer matrix ΘS (δ, ε). The partition function with several rows is the product of the row transfer matrices. Theorem 4. (Baxter) If ∆S = ∆T then ΘS and ΘT commute. Though we will not explain this point, the commuta ...
... ) be the states of the top and bottom rows. The partition function then is a row transfer matrix ΘS (δ, ε). The partition function with several rows is the product of the row transfer matrices. Theorem 4. (Baxter) If ∆S = ∆T then ΘS and ΘT commute. Though we will not explain this point, the commuta ...
Nanostructured Carbon Allotropes as Weyl
... to explore many-body interactions which cannot be easily obtained from experiment via serendipity. → Theory is and will lead the way. Compared to traditional particle physics, condensed matter is a much richer field and experimental test should be easier. → An emerging battlefield of particle physic ...
... to explore many-body interactions which cannot be easily obtained from experiment via serendipity. → Theory is and will lead the way. Compared to traditional particle physics, condensed matter is a much richer field and experimental test should be easier. → An emerging battlefield of particle physic ...
Part II
... Topological states with non-abelian anyons are rare, and hard to control. But, recently, similar anyons (Majorana bound states) might have been observed in one-dimensional nano-wires. This could give better control on the system. The anyons of the Moore-Read state are not universal, the phase gate c ...
... Topological states with non-abelian anyons are rare, and hard to control. But, recently, similar anyons (Majorana bound states) might have been observed in one-dimensional nano-wires. This could give better control on the system. The anyons of the Moore-Read state are not universal, the phase gate c ...
Why Quarks are Different from Leptons –
... gλi1 Bi2 i3 i4 vαh1 α2 δA1 A2 δΛ1 Λ2 (v h C)α3 α4 δA3 A4 δΛ3 1 δΛ4 2 δ(r1 − r2 )δ(r1 − r3 )δ(r1 − r4 ), ...
... gλi1 Bi2 i3 i4 vαh1 α2 δA1 A2 δΛ1 Λ2 (v h C)α3 α4 δA3 A4 δΛ3 1 δΛ4 2 δ(r1 − r2 )δ(r1 − r3 )δ(r1 − r4 ), ...
Coherent-state analysis of the quantum bouncing ball
... Gaussian-Klauder coherent states are applied to the bound “quantum bouncer,” a gravitating particle above an infinite potential boundary. These Gaussian-Klauder states, originally created for Rydberg atoms, provide an overcomplete set of wave functions that mimic classical trajectories for extended ...
... Gaussian-Klauder coherent states are applied to the bound “quantum bouncer,” a gravitating particle above an infinite potential boundary. These Gaussian-Klauder states, originally created for Rydberg atoms, provide an overcomplete set of wave functions that mimic classical trajectories for extended ...
Rank-one and Quantum XOR games
... games. The simplest such games, XOR games [CHTW04], correspond to the simplest and most widely studied class of Bell inequalities, the so-called correlation inequalities. In an XOR game, two players have a one-round interaction with a referee. The referee asks each player a question, to which they h ...
... games. The simplest such games, XOR games [CHTW04], correspond to the simplest and most widely studied class of Bell inequalities, the so-called correlation inequalities. In an XOR game, two players have a one-round interaction with a referee. The referee asks each player a question, to which they h ...
