Hyperspherical Approach to Quantal Three-body Theory
... (a) Full energy landscape for the three-body potentials at a = ∞ for our vλa model potential. (b) Effective diabatic potentials Wν relevant for Efimov physics for vλa with an increasingly large number of bound states (λ∗n is the value of λ that produces a = ∞ and n s-wave bound states). The Wν conve ...
... (a) Full energy landscape for the three-body potentials at a = ∞ for our vλa model potential. (b) Effective diabatic potentials Wν relevant for Efimov physics for vλa with an increasingly large number of bound states (λ∗n is the value of λ that produces a = ∞ and n s-wave bound states). The Wν conve ...
Algorithms for entanglement renormalization
... is particularly successful at describing ground states at quantum criticality1,5–11 or with topological order.12,13 From the computational viewpoint, the key property of the MERA is that it can be manipulated efficiently, due to the causal structure of the underlying quantum circuit.5 As a result, i ...
... is particularly successful at describing ground states at quantum criticality1,5–11 or with topological order.12,13 From the computational viewpoint, the key property of the MERA is that it can be manipulated efficiently, due to the causal structure of the underlying quantum circuit.5 As a result, i ...
Fluctuations in Ideal and Interacting Bose
... Prof. Herbert Walther is a quantum optics star of galactic magnitude! Experimental physicists admire his ability to conduct experiments previously considered impossible. Theoretical physicists eagerly look forward to the stunning results that come out of his laboratory. His discoveries have brought ...
... Prof. Herbert Walther is a quantum optics star of galactic magnitude! Experimental physicists admire his ability to conduct experiments previously considered impossible. Theoretical physicists eagerly look forward to the stunning results that come out of his laboratory. His discoveries have brought ...
Emergence of a classical world from within quantum theory
... by the opponents of this epistemic interpretation, it is difficult to reconcile this point of view with our common notion of “physical reality”, which exists independently of our monitoring, and can be discovered without disturbance. Indeed, if quantum theory is correct, it should apply to classical ...
... by the opponents of this epistemic interpretation, it is difficult to reconcile this point of view with our common notion of “physical reality”, which exists independently of our monitoring, and can be discovered without disturbance. Indeed, if quantum theory is correct, it should apply to classical ...
From Molecules to Cooper Pairs: Experiments in the BEC
... the distinct quantum statistical description of these two classes of matter becomes apparent when the gas is cooled to such low temperatures that the quantum mechanical wave packets of the particles begin to overlap. For bosons this marks the onset of BoseEinstein condensation (BEC). This phase tran ...
... the distinct quantum statistical description of these two classes of matter becomes apparent when the gas is cooled to such low temperatures that the quantum mechanical wave packets of the particles begin to overlap. For bosons this marks the onset of BoseEinstein condensation (BEC). This phase tran ...
quantum simulations on square and triangular hubbard models
... changing from electron-like to hole-like. The peak in the density of states also crosses the Fermi level at the Lifshitz transition line (chapter 4 and ref. [24]). We will show that the relation between the superconducting dome and the Lifshitz line is coupled to a subtle competition between the cha ...
... changing from electron-like to hole-like. The peak in the density of states also crosses the Fermi level at the Lifshitz transition line (chapter 4 and ref. [24]). We will show that the relation between the superconducting dome and the Lifshitz line is coupled to a subtle competition between the cha ...
Classical Mechanics: a Critical Introduction
... certain amount of material. It is difficult, or even impossible, to “cover” the standard topics in mechanics in one semester without passing too hastily over a number of fundamental concepts which form the basis for everything which follows. Perhaps the most common area of confusion has to do with t ...
... certain amount of material. It is difficult, or even impossible, to “cover” the standard topics in mechanics in one semester without passing too hastily over a number of fundamental concepts which form the basis for everything which follows. Perhaps the most common area of confusion has to do with t ...
Martinec-ContinuumMechanics.pdf
... ~ t) are called the relative motion functions. The subscripts t and The functions χ ~ t (~x, τ ) and χ ~ τ (ξ, τ at functions χ are used to recall which configuration is taken as reference. We assume that the functions ~γ0 , ~γt , χ ~, χ ~ t and χ ~ τ are single-valued and possess continuous partia ...
... ~ t) are called the relative motion functions. The subscripts t and The functions χ ~ t (~x, τ ) and χ ~ τ (ξ, τ at functions χ are used to recall which configuration is taken as reference. We assume that the functions ~γ0 , ~γt , χ ~, χ ~ t and χ ~ τ are single-valued and possess continuous partia ...
8.5 Collisions 8 Momentum
... External forces may have an effect after the collision: • Billiard balls encounter friction with the table and the air. • After a collision of two trucks, the combined wreck slides along the pavement and friction decreases its momentum. • Two space vehicles docking in orbit have the same net momentu ...
... External forces may have an effect after the collision: • Billiard balls encounter friction with the table and the air. • After a collision of two trucks, the combined wreck slides along the pavement and friction decreases its momentum. • Two space vehicles docking in orbit have the same net momentu ...
