Geometric Entropy of Self-Gravitating Systems
... thermodynamical potential and q is the electric charge, and the dots represent other terms that can of course appear depending on how liberal we decide to be in allowing other physical quantities, e.g. when more general gauge fields are present). Equation (2) is known as the first law of Black-Holes ...
... thermodynamical potential and q is the electric charge, and the dots represent other terms that can of course appear depending on how liberal we decide to be in allowing other physical quantities, e.g. when more general gauge fields are present). Equation (2) is known as the first law of Black-Holes ...
Longitudinal and Transverse Zeeman Ladders in the
... makes the longitudinal modes more massive (at higher energy) than their transverse counterpart, as we observe in BaCo2 V2 O8 . The ground state is then an admixture of Sz ¼ 0 two domain wall states added to the Néel state, producing a weakening of the ordered moment. In the ϵ ≪ 1 limit, the intensit ...
... makes the longitudinal modes more massive (at higher energy) than their transverse counterpart, as we observe in BaCo2 V2 O8 . The ground state is then an admixture of Sz ¼ 0 two domain wall states added to the Néel state, producing a weakening of the ordered moment. In the ϵ ≪ 1 limit, the intensit ...
topological invariants of knots and links
... by means of which it is possible, in many cases, to distinguish one type of knot from another. There exists one invariant, in particular, which is quite simple and effective. It takes the form of a polynomial A(x) with integer coefficients, where both the degree of the polynomial and the values of i ...
... by means of which it is possible, in many cases, to distinguish one type of knot from another. There exists one invariant, in particular, which is quite simple and effective. It takes the form of a polynomial A(x) with integer coefficients, where both the degree of the polynomial and the values of i ...
achieving 128-bit security against quantum attacks in openvpn
... c = 1/(1 − nk )1− n . This attack, however, only uses a ‘basic’ information-set decoding attack as described by McEliece [9] and originally introduced in 1962 by Prange [39]. A number of more advanced classical information-set decoding attacks exist and can be found in [21], [40], [41], [42], [43], ...
... c = 1/(1 − nk )1− n . This attack, however, only uses a ‘basic’ information-set decoding attack as described by McEliece [9] and originally introduced in 1962 by Prange [39]. A number of more advanced classical information-set decoding attacks exist and can be found in [21], [40], [41], [42], [43], ...
achieving 128-bit security against quantum attacks in openvpn
... c = 1/(1 − nk )1− n . This attack, however, only uses a ‘basic’ information-set decoding attack as described by McEliece [9] and originally introduced in 1962 by Prange [39]. A number of more advanced classical information-set decoding attacks exist and can be found in [21], [40], [41], [42], [43], ...
... c = 1/(1 − nk )1− n . This attack, however, only uses a ‘basic’ information-set decoding attack as described by McEliece [9] and originally introduced in 1962 by Prange [39]. A number of more advanced classical information-set decoding attacks exist and can be found in [21], [40], [41], [42], [43], ...
Twenty years of the Weyl anomaly
... an external gauge field [32] in addition to the gravitational field.) For n = 6, ga8(Tmo) would have to be cubic in curvature and so on. (At one-loop, and ignoring boundary terms, there is no anomaly for n odd). I showed these expressions to Steve Christensen, with whom I was sharing an office, and ...
... an external gauge field [32] in addition to the gravitational field.) For n = 6, ga8(Tmo) would have to be cubic in curvature and so on. (At one-loop, and ignoring boundary terms, there is no anomaly for n odd). I showed these expressions to Steve Christensen, with whom I was sharing an office, and ...
DIPLOMA THESIS Classical Chaos in Collective Nuclear Models
... Although nuclei are microscopic objects, it is reasonable to study dynamics also in the classical versions of nuclear models since they provide a helpful intuitive picture which is moreover closely related to quantal properties. Quite remarkably, it turns out that it is possible to find semiclassica ...
... Although nuclei are microscopic objects, it is reasonable to study dynamics also in the classical versions of nuclear models since they provide a helpful intuitive picture which is moreover closely related to quantal properties. Quite remarkably, it turns out that it is possible to find semiclassica ...
Hubbard model description of silicon spin qubits: charge stability
... generalization to the finite magnetic field situation49 is straightforward. III. ...
... generalization to the finite magnetic field situation49 is straightforward. III. ...
lectur~4-1 - Dr. Khairul Salleh Basaruddin
... force during its time interval of action. I acts in the same direction as F and has units of N·s or lb·s. The impulse may be determined by direct integration. Graphically, it can be represented by the area under the force versus time curve. If F is constant, then I = F (t2 – t1) . ENT 142 – ENGINEER ...
... force during its time interval of action. I acts in the same direction as F and has units of N·s or lb·s. The impulse may be determined by direct integration. Graphically, it can be represented by the area under the force versus time curve. If F is constant, then I = F (t2 – t1) . ENT 142 – ENGINEER ...
Chapters 1–5 Schedule of Crisis Centre
... • Elastic collision: the total kinetic energy after collision is equal ! to the total before collision. • Inelastic collision: the total kinetic energy is not conserved. If ! objects stick together after collision, the collision is “perfectly ! inelastic” – no bounce of one object from the other. Ex ...
... • Elastic collision: the total kinetic energy after collision is equal ! to the total before collision. • Inelastic collision: the total kinetic energy is not conserved. If ! objects stick together after collision, the collision is “perfectly ! inelastic” – no bounce of one object from the other. Ex ...
Dynamical Theories of Brownian Motion
... There was opposition on the part of some topologists to this process, due to the loss of generality and the impurity of methods. It seems to me that the theory of stochastic processes is in the doldrums today. It is in the doldrums for the same reason, and the remedy is the same. We need to introduc ...
... There was opposition on the part of some topologists to this process, due to the loss of generality and the impurity of methods. It seems to me that the theory of stochastic processes is in the doldrums today. It is in the doldrums for the same reason, and the remedy is the same. We need to introduc ...
Valley polarization assisted spin polarization in two dimensions
... In stark contrast to expectations from a non-interacting model, we show experimentally that less magnetic field can be required to fully spin polarize a valley-polarized system than a valley-degenerate one. Furthermore, we show that these observations are quantitatively described by parameter-free ab ...
... In stark contrast to expectations from a non-interacting model, we show experimentally that less magnetic field can be required to fully spin polarize a valley-polarized system than a valley-degenerate one. Furthermore, we show that these observations are quantitatively described by parameter-free ab ...
Cotunneling in the ν Robert Zielke, Bernd Braunecker,
... temperature T such that the perturbative result is accurate. Our calculations show that the different charge carriers can be clearly distinguished by standard transport measurements. Our approach is also applicable to a setup of two separate FQH samples with common Laughlin FQH edge states at fillin ...
... temperature T such that the perturbative result is accurate. Our calculations show that the different charge carriers can be clearly distinguished by standard transport measurements. Our approach is also applicable to a setup of two separate FQH samples with common Laughlin FQH edge states at fillin ...
Quantum liquid of repulsively bound pairs of particles in a lattice
... late and create a dimer at site j. Within the subspace of states in which all occupation numbers are even, these operators behave exactly as canonical creation and annihilation operators, possessing the standard bosonic commutation relations [cj , c†i ] = δji and [cj , ci ] = [c†j , c†i ] = 0. The d ...
... late and create a dimer at site j. Within the subspace of states in which all occupation numbers are even, these operators behave exactly as canonical creation and annihilation operators, possessing the standard bosonic commutation relations [cj , c†i ] = δji and [cj , ci ] = [c†j , c†i ] = 0. The d ...
