Disorder-induced order with ultra-cold atoms
... already led to seminal breakthroughs like the creation of a Bose-Einstein Condensate [Anderson et al., 1995, Davis et al., 1995], the transition between Mott Insulator and Superfluid [Greiner et al., 2002], as well as the above-mentioned creation of Anderson Localization in matter waves. Due to the ...
... already led to seminal breakthroughs like the creation of a Bose-Einstein Condensate [Anderson et al., 1995, Davis et al., 1995], the transition between Mott Insulator and Superfluid [Greiner et al., 2002], as well as the above-mentioned creation of Anderson Localization in matter waves. Due to the ...
Entanglement Entropy
... ψ = aχ+ + bχ− (where a and b are fixed complex numbers satisfying |a|2 +|b|2 = 1), describe1 an electron spin oriented in a particular direction n = n (θ, ϕ) with θ = 2 arccos |a|, ϕ = arg b − arg a. This means that ψ can represent an electron beam polarized along n while it cannot represent an unpo ...
... ψ = aχ+ + bχ− (where a and b are fixed complex numbers satisfying |a|2 +|b|2 = 1), describe1 an electron spin oriented in a particular direction n = n (θ, ϕ) with θ = 2 arccos |a|, ϕ = arg b − arg a. This means that ψ can represent an electron beam polarized along n while it cannot represent an unpo ...
A Critique of Pure String Theory: Heterodox Opinions of Diverse
... like the (2, 0) theory in six dimensions, which have not yet been realized as infrared limits of Gaussian models (this is impossible) or discretized statistical sums (this is possible but unknown at the moment) that we have been forced to face the truly radical departure from Lagrangian dynamics th ...
... like the (2, 0) theory in six dimensions, which have not yet been realized as infrared limits of Gaussian models (this is impossible) or discretized statistical sums (this is possible but unknown at the moment) that we have been forced to face the truly radical departure from Lagrangian dynamics th ...
Lectures on Arithmetic Noncommutative Geometry Matilde Marcolli
... references to the relevant literature, where complete proofs are provided (in particular [32], [44], [38], and [83]). More explicitly, the text is organized as follows: • We start by recalling a few preliminary notions of noncommutative geometry (following [21]). • The second chapter describes how v ...
... references to the relevant literature, where complete proofs are provided (in particular [32], [44], [38], and [83]). More explicitly, the text is organized as follows: • We start by recalling a few preliminary notions of noncommutative geometry (following [21]). • The second chapter describes how v ...
Superconducting Qubit Storage and Entanglement with Nanomechanical Resonators A. N. Cleland
... vibrational mode. Upon cooling to 20 mK, the 1.8 GHz dilatational mode will be in the quantum regime, with a probability of thermally occupying the first excited (one phonon) state of about 102 . Using dilatational-phonon creation and annihilation operators, the resonator 0 ay a. Hamiltonian is H ...
... vibrational mode. Upon cooling to 20 mK, the 1.8 GHz dilatational mode will be in the quantum regime, with a probability of thermally occupying the first excited (one phonon) state of about 102 . Using dilatational-phonon creation and annihilation operators, the resonator 0 ay a. Hamiltonian is H ...
