Life in the Higgs condensate, where electrons have mass
... Texas A&M University, Department of Physics and Astronomy, College Station, USA The particle recently discovered by the CMS and ATLAS collaborations at CERN is almost certainly a Higgs boson, fulfilling a quest that can be traced back to three seminal high-energy papers of 1964, but which is intimat ...
... Texas A&M University, Department of Physics and Astronomy, College Station, USA The particle recently discovered by the CMS and ATLAS collaborations at CERN is almost certainly a Higgs boson, fulfilling a quest that can be traced back to three seminal high-energy papers of 1964, but which is intimat ...
Cornell University – Toby Berger
... classical and quantum information theoretical techniques to find an expression for the optimal tradeoff curve attainable by the above method. In addition [5] contains new upper bounds on the high-entanglement region, improving on those of Bennett et al. 4. THE UNION OF PHYSICS AND INFORMATION [4]. C ...
... classical and quantum information theoretical techniques to find an expression for the optimal tradeoff curve attainable by the above method. In addition [5] contains new upper bounds on the high-entanglement region, improving on those of Bennett et al. 4. THE UNION OF PHYSICS AND INFORMATION [4]. C ...
Jort Bergfeld : Completeness for a quantum hybrid logic.
... Abstract: In this presentation I will introduce a quantum hybrid logic (QHL) on finite dimensional quantum Kripke frames. This quantum hybrid logic has, besides the classical connectives, an operator expressing non-orthogonality, @_i operators to express truth at a fixed state i and a "down arrow" t ...
... Abstract: In this presentation I will introduce a quantum hybrid logic (QHL) on finite dimensional quantum Kripke frames. This quantum hybrid logic has, besides the classical connectives, an operator expressing non-orthogonality, @_i operators to express truth at a fixed state i and a "down arrow" t ...
Why I Still Like String Theory
... as another idea that may be more interesting. Really though I dont see these as alternatives. The “alternatives theory view” is a social construct that came out of in-fighting between physicists. There is only one right theory of quantum gravity and if more than one idea seems to have good features ...
... as another idea that may be more interesting. Really though I dont see these as alternatives. The “alternatives theory view” is a social construct that came out of in-fighting between physicists. There is only one right theory of quantum gravity and if more than one idea seems to have good features ...
COMPLEXITY OF QUANTUM FIELD THEORIES 1. Introduction
... may only solve a very restricted class of theories exactly – such theories typically have infinitely many fields or reside in one spatial dimension[3]. Therefore, for computing quantities in realistic field theories we turn to numerical solutions. The algorithms developed for classical computers hav ...
... may only solve a very restricted class of theories exactly – such theories typically have infinitely many fields or reside in one spatial dimension[3]. Therefore, for computing quantities in realistic field theories we turn to numerical solutions. The algorithms developed for classical computers hav ...
Document
... Prove that, given a pair of normalized but not orthogonal functions ψ1 and ψ2, the function ψ3 = ψ2 – Sψ1 is orthogonal to ψ1 if S is the overlap integral of ψ1 and ψ2. Is ψ3 normalized? (Use the back of the page if necessary). ...
... Prove that, given a pair of normalized but not orthogonal functions ψ1 and ψ2, the function ψ3 = ψ2 – Sψ1 is orthogonal to ψ1 if S is the overlap integral of ψ1 and ψ2. Is ψ3 normalized? (Use the back of the page if necessary). ...
ПУБЛИКАЦИИ ЛАБОРАТОРИИ ФИЗИКИ ФУНДАМЕНТАЛЬНЫХ
... We construct interactions of nucleons N with higher-spin resonances R invariant under point and gauge transformations of the Rarita-Schwinger field. It is found for arbitrarily high spin of a resonance that the requirement of point- and gauge-invariance uniquely determines a Lagrangian of NR interac ...
... We construct interactions of nucleons N with higher-spin resonances R invariant under point and gauge transformations of the Rarita-Schwinger field. It is found for arbitrarily high spin of a resonance that the requirement of point- and gauge-invariance uniquely determines a Lagrangian of NR interac ...
Homework 4 plus notes out: 4-22 due: 4
... show that if the system is initially in the vacuum (for modes 1 and 2), then at finite times the expectations hn1 i = hn2 i are finite, but the variance in n1 − n2 vanishes. (This takes a bit of operator algebra. See me if you need help!) Thus, remarkably, one can have a noise-free quantity in some ...
... show that if the system is initially in the vacuum (for modes 1 and 2), then at finite times the expectations hn1 i = hn2 i are finite, but the variance in n1 − n2 vanishes. (This takes a bit of operator algebra. See me if you need help!) Thus, remarkably, one can have a noise-free quantity in some ...
Two Times - University of Southern California
... 2T-physics solves this (a property of 4+2 dims.) – no need for axion! •Why these degrees of freedom? And why in these patterns? •25 parameters : masses, couplings, mixings – is there a theory that determines them from first principles? Is Higgs the answer to the origin of mass ? LHC 2008 !! 2T-p ...
... 2T-physics solves this (a property of 4+2 dims.) – no need for axion! •Why these degrees of freedom? And why in these patterns? •25 parameters : masses, couplings, mixings – is there a theory that determines them from first principles? Is Higgs the answer to the origin of mass ? LHC 2008 !! 2T-p ...
Smolin - Bell paper - International Journal of Quantum Foundations
... temperature T → 0 in a way that keeps a fixed value for the diffusion constant νλ fixed. This regime is defined by holding fixed a dimensionless scaled temperature t= ...
... temperature T → 0 in a way that keeps a fixed value for the diffusion constant νλ fixed. This regime is defined by holding fixed a dimensionless scaled temperature t= ...
