structure and thermodynamics of lanthanide
... sphere20. This model of solvent separated ion pairing was supported by studies of the spectra of Nd(iii) which showed• no change up to concentrations of 5M chloride ion2 1 A spectral change was observed at higher concentrations which may be related to a change in coordination number from nine to eig ...
... sphere20. This model of solvent separated ion pairing was supported by studies of the spectra of Nd(iii) which showed• no change up to concentrations of 5M chloride ion2 1 A spectral change was observed at higher concentrations which may be related to a change in coordination number from nine to eig ...
An Atomic Source of Quantum Light - Institute for Quantum Science
... (a) Theoretically predicted relative intensity squeezing in the presence of loss. In the presence of loss the amount of squeezing obtained is not monotonically decreasing with increasing gain. (b) Loss in the signal (idler) channel is modelled as a beam splitter of transmissivity ηs(i) and a vacuum ...
... (a) Theoretically predicted relative intensity squeezing in the presence of loss. In the presence of loss the amount of squeezing obtained is not monotonically decreasing with increasing gain. (b) Loss in the signal (idler) channel is modelled as a beam splitter of transmissivity ηs(i) and a vacuum ...
Quantum Fingerprints that Keep Secrets
... string x of length n, we want to efficiently produce its “partial description” by d bits, typically with d ≪ n, such that given only the description of x and any y ∈ {0, 1}n one can test, with high accuracy, whether x = y. This can be achieved classically, for example by using a randomized mapping x ...
... string x of length n, we want to efficiently produce its “partial description” by d bits, typically with d ≪ n, such that given only the description of x and any y ∈ {0, 1}n one can test, with high accuracy, whether x = y. This can be achieved classically, for example by using a randomized mapping x ...
Discrete Abelian Gauge Symmetries
... theorem. In contrast, the group action of discrete symmetries cannot be described by continuous transformations. While for a global symmetry the transformation law is the same everywhere in spacetime, a local symmetry allows the transformation law to vary smoothly for different points of the spaceti ...
... theorem. In contrast, the group action of discrete symmetries cannot be described by continuous transformations. While for a global symmetry the transformation law is the same everywhere in spacetime, a local symmetry allows the transformation law to vary smoothly for different points of the spaceti ...
THE RENORMALIZATION GROUP AND CRITICAL PHENOMENA
... exp(-H/kT) over all configurations of the magnetic moments, where k is Boltzmann’s constant. The free energy F is proportional to the negative logarithm of Z. The Boltzmann factor exp(-H/kT) is an analytic function of T near Tc, in fact for all T except T = 0. A sum of analytic functions is also ana ...
... exp(-H/kT) over all configurations of the magnetic moments, where k is Boltzmann’s constant. The free energy F is proportional to the negative logarithm of Z. The Boltzmann factor exp(-H/kT) is an analytic function of T near Tc, in fact for all T except T = 0. A sum of analytic functions is also ana ...
Experimental test of Heisenberg`s measurement uncertainty relation
... Ref. [39]). If the angle between the vectors a − c and b − d is an acute or obtuse angle, the Bloch vector of |ψi should be collinear with a + b − c − d or a − b − c + d, respectively. If the angle is a right angle, the Bloch vector should be collinear with either. For the measurement, different sch ...
... Ref. [39]). If the angle between the vectors a − c and b − d is an acute or obtuse angle, the Bloch vector of |ψi should be collinear with a + b − c − d or a − b − c + d, respectively. If the angle is a right angle, the Bloch vector should be collinear with either. For the measurement, different sch ...
