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Two-dimensional momentum imaging of Rydberg states using half-cycle pulse ionization
Two-dimensional momentum imaging of Rydberg states using half-cycle pulse ionization

... tron in the x,y directions far away from the core, where the Coulomb field is negligible, represents the velocity map. The quantum mechanical calculations reproduce the momentum distribution of the excited Rydberg state by adding the momentum distributions of all 34 hydrogenic k states for n ⫽34 as ...
Angular momentum operator
Angular momentum operator

... each other. Following our previous discussion on compatible observables, this means that the components are not compatible observables. We cannot measure, for instance, Lx and Ly simultaneously, and we do not have a basis of common eigenfunctions of the two operators. Physically, this also implies t ...
10/29/2007 Julia Velkovska PHY 340a
10/29/2007 Julia Velkovska PHY 340a

... • Baryons – QQQ (p, n, L, D) ...
Feynman-Kac formula for L´evy processes and semiclassical (Euclidean) momentum representation
Feynman-Kac formula for L´evy processes and semiclassical (Euclidean) momentum representation

... In addition we also study the limiting behaviors of the solutions given by FeynmanKac type formulas in terms of large deviations. In particular we show in detail that these limiting behaviors have exactly the same patterns as the semiclassical limits of (Euclidean) quantum mechanics in several speci ...
QCD: (the origin of mass of the visible universe)
QCD: (the origin of mass of the visible universe)

... The vast majority of the mass of ordinary matter ultimate (Higgs or alternative) mechanism: responsible for the mass of the leptons and for the mass of the quarks interestingly enough: just a tiny fraction of the visible mass (such as stars, the earth, the audience, atoms) electron: almost massless, ...
8 Selectivity of the O e
8 Selectivity of the O e

... Equation ~7! contains three main ingredients: the final-state wave function c f , the nuclear current J m , and the twonucleon overlap integral c i . The derivation of Eq. ~7! involves bound and scattering states c i and c f which are consistently derived from an energy-dependent non-Hermitian Feshb ...
Atom-atom interactions in ultracold gases - cours en ligne CEL
Atom-atom interactions in ultracold gases - cours en ligne CEL

... accumulated a phase shift with respect to the V=0 case. The superposition of the 2 waves is thus a shifted sinusoid. ...
Parameterization and orbital angular momentum of anisotropic
Parameterization and orbital angular momentum of anisotropic

... a specific line in the sx, yd plane, as if the phase map were stretched along this line (assumed, for simplicity, to go through the origin). Thus the two most important characteristics of the anisotropic dislocation are the amount of stretching and its direction. The other two characteristics are th ...
Hadronization of Quark Theories
Hadronization of Quark Theories

... Here the sign factor ǫH (q) controls the norm of the mesonic state a+ H |0i ≡ |Hi. In general there will be many states with unphysical norms since the bare mesons are produced by ladder diagrams only and may not be directly related to physical particles. This situation presents no fundamental diffi ...
"Pentaquarks: Theory & Experiment"(ppt 1.59M)
"Pentaquarks: Theory & Experiment"(ppt 1.59M)

... with spin ½ and negative (–) parity, in PDG This may suggest a negative parity for antidecuplet members in the chiral soliton model: parity in chiral solition has two parts: quantized part with positive parity and classical part with unknown parity; the collective coordinate quantization can not ine ...
pptx - Curtis A. Meyer
pptx - Curtis A. Meyer

... Partial Wave Analysis For a three-body reaction from a ``known’’ initial state, one can do a Dalitz analysis. Only two variables are needed to describe the full kinematics. hp0p Intermediate resonances include the a2(1320)->hp and the r(770)->pp and a possible 1-+ wave p1->hp Hybrid Mesons ...
Chapter 11 : Matter Notes
Chapter 11 : Matter Notes

... Chapter 11 : Matter Notes ...
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... phenomenological parameters, which were introduced at a time of limited computational resources in order to assist with the theoretical estimation of essentially nonperturbative stronginteraction matrix elements.  A universality of these condensates was assumed, namely, that the properties of all h ...
Efficient generation of a maximally entangled state by
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... In fact, various interesting and peculiar phenomena are predicted on the basis of highly nonclassical states, and entanglement plays a key role in quantum information protocols [1]. They all rely on the generation of nontrivial states and are not realized without establishing strategies for the prep ...
Interference-effects in the laser
Interference-effects in the laser

... of the system Hamiltonian. This time evolution can be calculated by quantum mechanical standard methods w17x. In this paper, the consequences of such a diabatic treatment of the DIET process are investigated with respect to the resulting velocity distributions, which are an observable measured for d ...
Düren (ppt 10,1MB)
Düren (ppt 10,1MB)

...  When integrated over x, one gets the momentum density.  When integrated over p, one gets the probability density. ...
talk_pacific - University of Kentucky
talk_pacific - University of Kentucky

... For a QM particle the configuration/path is one possible history for the dynamical variable involved (its coordinate) For quantum field it is the same: the history of field values in 3-d space ...
Strong coupling QCD
Strong coupling QCD

... Δλ=0,1, depending on whether helicity is conserved or flipped … prediction of 1/k2 vector-boson exchange logarithm = distinctive feature & concrete prediction of QCD  Initially imagined that Λ = 1GeV!  So, JLab was initially built to reach 4GeV. Craig Roberts: Strong-coupling QCD and the ins and o ...
Through scattering theory with gun and camera: Coping with conventions
Through scattering theory with gun and camera: Coping with conventions

... of undergraduate and introductory graduate quantum courses. It is necessary to choose a zero of energy, and it is possible to multiply the wave function by an overall global phase factor, and that’s about it. Continuum-state quantum mechanics, by contrast, presents four options—all of which, as we s ...
Jian_Zhou
Jian_Zhou

... An explicit NLO cross section calculation shows that both the large logarithm appear. 2013, Mueller, Xiao, Yuan ...
ppt - EPFL
ppt - EPFL

... Branching ratio and helicity amplitudes for Lb  L(pK) g decays (L spin = 3/2) Combined work of: Gudrun Hiller (Dortmund UNI), the Bearer of the Light Thomas Schietinger (PSI), the Scholar Mathias Knecht and Federica Legger (EPFL), the water Carriers ...
Topic 6: Momentum and Collisions
Topic 6: Momentum and Collisions

... Momentum is important in mechanics. A few examples include car collisions, billiards, rockets or any matter that is moving. Momentum plays a role in radiation as in X-ray photons penetrating a piece of metal or a human, UV photons passing through a cloud, or light photons passing through glass. On t ...
a 1 - SMU Physics
a 1 - SMU Physics

...  Hadron spectrum, and elastic and transition form factors provide unique information about long-range interaction between lightquarks and distribution of hadron's characterising properties amongst its QCD constituents.  Dynamical Chiral Symmetry Breaking (DCSB) is most important mass generating me ...
Relativistic nucleus-nucleus collisions, Transverse mass, Effective
Relativistic nucleus-nucleus collisions, Transverse mass, Effective

... Theoretical analysis of these data is still in progress. RHIC continues to study the detailed properties of the strongly interacting matter using p+p, d+Au and Au+Au systems at various colliding energies from 7.7 GeV up to 200 GeV. Measurements of transverse momentum spectra for particles emerging f ...
Elementary Particle Physics
Elementary Particle Physics

... L12  angular momentum of 1 and 2 in "subsystem" L3  angular momentum of 3 about c.m of 1 and 2 in the overall c.m. frame: Ltot  L12  L3 We only consider ground state baryons: angular momentum comes only from spin: L12  L3  0 ...
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Light-front quantization applications

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