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Lecture #3
Lecture #3

Holography, de Sitter space and SUSY breaking
Holography, de Sitter space and SUSY breaking

... Holographic cosmology implies future of normal region is dS with c.c. determined by number of quantum states in initial defect (TB, Fischler) Will outline (incomplete) quantum theory of eternal dS space, which describes asymptotic state of our universe (cf. Poincare invariant string theory of partic ...
Abstracts of the talks
Abstracts of the talks

... Given a surface S with a collection of special points on the boundary modulo isotopy, and a split reductive group G, we define a moduli space M (G, S) of G-local systems on S with some special data at the special points. We introduce a function W on M (G, S), the potential. It determines a set of W ...
Elements of a Physics Case for HE LHC
Elements of a Physics Case for HE LHC

... Tevatron 95% exclusion 160 GeV < mh < 170 GeV Experiment Summary: 115 GeV < mh < 160 GeV or 170 GeV < mh < 180 GeV In other words, Higgs boson (or equivalent dynamics) is likely to be LIGHT and PERTURBATIVE electroweak interactions are expected. ...
Link between the hierarchy of fractional quantum Hall states and
Link between the hierarchy of fractional quantum Hall states and

... Link between the hierarchy of fractional quantum Hall states and Haldane’s conjecture for quantum spin chains Masaaki Nakamura Department of Physics, Tokyo Institute of Technology, Tokyo 152-8551, Japan ...
Particle physics, from Rutherford to the LHC
Particle physics, from Rutherford to the LHC

HWU4-21 QUESTION: The principal quantum number, n, describes
HWU4-21 QUESTION: The principal quantum number, n, describes

... The principal quantum number, n, describes the energy level of a particular orbital as a function of the distance from the center of the nucleus. Additional quantum numbers exist to quantify the other characteristics of the electron. The angular momentum quantum number (ℓ), the magnetic quantum numb ...
Page 16(1)
Page 16(1)

New Frontiers in Particle Physics.
New Frontiers in Particle Physics.

... The Higgs Boson That’s almost the whole story…. But the gauge symmetries of the Standard Model do not permit particles to carry mass! Q. How is mass generated? A. By the non-trivial action of the vacuum! It grabs hold of things! ...
A Weak Gravity Conjecture for Scalar Field Theories
A Weak Gravity Conjecture for Scalar Field Theories

PHYS6510/4510 Quantum Mechanics I Fall 2012 HW #5
PHYS6510/4510 Quantum Mechanics I Fall 2012 HW #5

... c. Calculate ∆S/h̄ for a particle which moves 1 mm in 1 ms for two cases. The particle is a nanoparticle made up of 100 carbon atoms in one case. The other case is an electron. For which of these would you consider the motion “quantum mechanical” and why? (2) Modern Quantum Mechanics, Problem 2.28. ...
CHAPTER 2. LAGRANGIAN QUANTUM FIELD THEORY §2.1
CHAPTER 2. LAGRANGIAN QUANTUM FIELD THEORY §2.1

... Note that the discretized version of the QFT yields the mechanical interpretation of QFT as an infinite collection of quantum mechanical generalized coordinates. Before proceeding further let’s consider an example with which we are already familiar, the noninteracting, Hermitian, scalar (spin zero) ...
Many Worlds Theory/ `Relative State` formation of Quantum Mechanics
Many Worlds Theory/ `Relative State` formation of Quantum Mechanics

LOYOLA COLLEGE (AUTONOMOUS), CHENNAI
LOYOLA COLLEGE (AUTONOMOUS), CHENNAI

... Prove that the square of the angular momentum commutes with its components. What is meant by degeneracy of an energy level? What is an orthonormal basis? With an example explain simultaneous eigenfunctions. If A and B are two operators, then show that [A-1[A,B]] = 2B. ...
Why there is Something rather than Nothing (from
Why there is Something rather than Nothing (from

... boson could serve as the inflaton for a scenario with ns» 0.93 and T/S» 0.0004 The mechanism is very different from F.Bezrukov and M.Shaposhnikov, Phys.Lett. 659B (2008) 703 because it is dominated by the quantum effects: CMB data probe quantum anomalous scaling induced by all heavy massive particle ...
Rabi oscillations
Rabi oscillations

Isospin effect in asymmetric nuclear matter
Isospin effect in asymmetric nuclear matter

Quantum Mechanics and Applications
Quantum Mechanics and Applications

General Relativity as an Effective Field Theory
General Relativity as an Effective Field Theory

PDF
PDF

5.0. Wave Mechanics
5.0. Wave Mechanics

A Fundamental Particle of Relativistic Mass
A Fundamental Particle of Relativistic Mass

Hydrogen Atom in Spherical Coordinates (III) Eigenenergies of one
Hydrogen Atom in Spherical Coordinates (III) Eigenenergies of one

... [principal] energy [azimuthal] angular momentum: s, p, d, f, .. [magnetic] orientation in space (note: one more quantum number to come … Spin !) ...
Chern-Simons theory and the fractional quantum Hall effect
Chern-Simons theory and the fractional quantum Hall effect

... above formula corresponds to integer numbers. Surprisingly in 1983, Tsui and collaborators[2] observed the so called fractional quantum Hall effect (FQHE), for which ν = pq , p, q integers. In these notes we discuss how one can use the ChernSimons gauge theory to understand or to deal with the FQHE. ...
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Scalar field theory

In theoretical physics, scalar field theory can refer to a classical or quantum theory of scalar fields. A scalar field is invariant under any Lorentz transformation.The only fundamental scalar quantum field that has been observed in nature is the Higgs field. However, scalar quantum fields feature in the effective field theory descriptions of many physical phenomena. An example is the pion, which is actually a pseudoscalar.Since they do not involve polarization complications, scalar fields are often the easiest to appreciate second quantization through. For this reason, scalar field theories are often used for purposes of introduction of novel concepts and techniques.The signature of the metric employed below is (+, −, −, −).
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