A Numerical Approach to Virasoro Blocks and the Information
... We will observe in section 4 that the exact and semiclassical correlators behave very similarly at these points, though they seem to differ markedly both very near (within √1 ) and beyond the first forbidden singularity. The results can be seen in figure 15. As c previously discussed [7], we expect ...
... We will observe in section 4 that the exact and semiclassical correlators behave very similarly at these points, though they seem to differ markedly both very near (within √1 ) and beyond the first forbidden singularity. The results can be seen in figure 15. As c previously discussed [7], we expect ...
Quantum Orders and Symmetric Spin Liquids
... in the sense that a quantum Hall liquid cannot be compressed. Thus a quantum Hall liquid has a fixed and welldefined density. When we measure the electron density in terms of filling factor ν, we found that all discovered quantum Hall states have such densities that the filling factors are exactly g ...
... in the sense that a quantum Hall liquid cannot be compressed. Thus a quantum Hall liquid has a fixed and welldefined density. When we measure the electron density in terms of filling factor ν, we found that all discovered quantum Hall states have such densities that the filling factors are exactly g ...
Macroscopic Local Realism: How Do We Define It and Is It
... position) on the particle at B. Now the ``locality'' assumption tells us that the measurement at B could not have disturbed the system at A. Hence, EPR reason, because one can predict precisely the result of the measurement of position of particle A without disturbing the system, ``realism'' implies ...
... position) on the particle at B. Now the ``locality'' assumption tells us that the measurement at B could not have disturbed the system at A. Hence, EPR reason, because one can predict precisely the result of the measurement of position of particle A without disturbing the system, ``realism'' implies ...
Approaches to Quantum Gravity
... clearly come from looking at how similar difficulties had been solved in another. It is even possible that, in order to achieve our common goal, formulate a complete theory of Quantum Gravity and unravel the fundamental nature of space and time, we will have to regard (at least some of) these approa ...
... clearly come from looking at how similar difficulties had been solved in another. It is even possible that, in order to achieve our common goal, formulate a complete theory of Quantum Gravity and unravel the fundamental nature of space and time, we will have to regard (at least some of) these approa ...
Ground-state energy and excitation spectrum of the Lieb
... g1D is an effective one-dimensional coupling constant which can be deduced from experimental parameters [42, 43] and δ is the Dirac function. We assume g1D > 0, corresponding to repulsive interactions. In second-quantized form, the Hamiltonian reads [2] ...
... g1D is an effective one-dimensional coupling constant which can be deduced from experimental parameters [42, 43] and δ is the Dirac function. We assume g1D > 0, corresponding to repulsive interactions. In second-quantized form, the Hamiltonian reads [2] ...
Two-gluon rapidity correlations of strong colour
... density when two trigger gluon are collimation [31–33], the initial state quantum mechanical effects, and/or the fluctuations of a colour flux tube in the longitudinal space [5]? In order to see why ridge-like correlation in initial state, we focus our calculations on the gluon level alone and use o ...
... density when two trigger gluon are collimation [31–33], the initial state quantum mechanical effects, and/or the fluctuations of a colour flux tube in the longitudinal space [5]? In order to see why ridge-like correlation in initial state, we focus our calculations on the gluon level alone and use o ...
MOMENTUM
... Q9.3. Reason: When the question talks about forces, times, and momenta, we immediately think of the impulsemomentum theorem, which tells us that to change the momentum of an object we must exert a net external force on it G G over a time interval: Favg Δt = Δp. Because equal forces are exerted over ...
... Q9.3. Reason: When the question talks about forces, times, and momenta, we immediately think of the impulsemomentum theorem, which tells us that to change the momentum of an object we must exert a net external force on it G G over a time interval: Favg Δt = Δp. Because equal forces are exerted over ...
String Theory. Volume 1, Introduction to the Bosonic String
... Standard Model, and to collect general results on the physics of fourdimensional string theories as derived from world-sheet and spacetime symmetries. New developments have led to a third goal, which is to introduce the recent discoveries concerning string duality, M-theory, D-branes, and black hole ...
... Standard Model, and to collect general results on the physics of fourdimensional string theories as derived from world-sheet and spacetime symmetries. New developments have led to a third goal, which is to introduce the recent discoveries concerning string duality, M-theory, D-branes, and black hole ...
Reconstruction on Wigner Functions on Different
... reconstructed. To accomplish this task we utilize the concept of observation levels [22] (see also [23]) where each observation level is specified by a set of linearly independent operators G & (&=1, 2, ..., n) for which expectation values G & are given (measured). With the help of the Jaynes princ ...
... reconstructed. To accomplish this task we utilize the concept of observation levels [22] (see also [23]) where each observation level is specified by a set of linearly independent operators G & (&=1, 2, ..., n) for which expectation values G & are given (measured). With the help of the Jaynes princ ...
lecture 3
... Running of quark mass entails that calculations at even modest Q2 require a Poincaré-covariant approach. Covariance + M(p2) require existence of quark orbital angular momentum in hadron's rest-frame wave function. Confinement is expressed through a violent change of the propagators for coloured ...
... Running of quark mass entails that calculations at even modest Q2 require a Poincaré-covariant approach. Covariance + M(p2) require existence of quark orbital angular momentum in hadron's rest-frame wave function. Confinement is expressed through a violent change of the propagators for coloured ...
