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Theoretical Chemistry
Theoretical Chemistry

Basic physics of high harmonic generation (HHG)
Basic physics of high harmonic generation (HHG)

... constraints for parametric process) ...
Conservation Laws I - Department of Physics, HKU
Conservation Laws I - Department of Physics, HKU

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... Rydberg blockade interaction will prevent double excitations within a blockade radius. However, the question arises whether the thermal motion of atoms does not destroy the desired emission pattern. To solve that problem we have studied a correspondence between temperature of an atomic cloud and ave ...
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... nonmetals atoms are sharing unequally. The reason that they are sharing electrons unequally is that the two atoms have different electronegativities. -A covalent bond is a bond between two nonmetals. If those two nonmetals are the same element as in the case of HOFBrINCl’s then its a nonpolar covale ...
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... where mo is the body’s “rest mass,” i.e., the body’s mass when it is at rest, and c ≈ 3 × 108 m/s is the speed of light. Amazingly, Einstein’s correction to the laws of motion was produced theoretically before being discovered experimentally, which is uncommon in physics. This may be explained by th ...
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... For nmax D 100, the internal energy grows rapidly with the temperature, reaching an asymptotic value equal to the ionization potential, while for nmax D 10 the growth is much slower, and up to T D 50;000 K the asymptotic value of 1;282 kJ/mole has not been reached yet. The upper limit of the interna ...
Time propagation of extreme two-electron wavefunctions F Robicheaux
Time propagation of extreme two-electron wavefunctions F Robicheaux

... It is a truism that all numerical methods have limitations so that, actually, it is not difficult to find situations where the methods above will not converge with current resources or would be so difficult to converge that it is not worth the effort. For example, Pisharody and Jones [5] describe an ...
Final Review Answers
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Physics 452 - BYU Physics and Astronomy
Physics 452 - BYU Physics and Astronomy

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ATS MOLS - School of Chemistry

Mixed quantum and classical processes in strong fields
Mixed quantum and classical processes in strong fields

... will depend on the approximation scheme adopted to calculate the fully interacting wave function. In contrast, a classical rescattering event has a direct physical meaning. An electron ionized by the oscillatory field will initially move away from the remnant ion. When the field reverses direction, ...
unit-3-atoms-and-nuclear - Waukee Community School District Blogs
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... b. The daughter nuclide thus has a new atomic number because the number of protons increases by 1; mass stays the same c. New atomic number = new element symbol ...
Grade 10 NSC Chemistry Curriculum
Grade 10 NSC Chemistry Curriculum

Landau Levels
Landau Levels

... These eigenfunctions form Landau levels. First examine the lowest Landau level wavefunctions (n = 0 according to this scheme). y00 has some zero-point kinetic energy (the spread of the Gaussian); y01 represents a cyclotron orbit that closes on itself after one cycle; y02 represents a cyclotron orbit ...
Quantum Mechanics of the Solar System - Latin
Quantum Mechanics of the Solar System - Latin

Time-Gated Photoionization Spectroscopy Demonstrated for Cesium Rydberg Wave Packets
Time-Gated Photoionization Spectroscopy Demonstrated for Cesium Rydberg Wave Packets

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Bohr model



In atomic physics, the Rutherford–Bohr model or Bohr model, introduced by Niels Bohr in 1913, depicts the atom as a small, positively charged nucleus surrounded by electrons that travel in circular orbits around the nucleus—similar in structure to the solar system, but with attraction provided by electrostatic forces rather than gravity. After the cubic model (1902), the plum-pudding model (1904), the Saturnian model (1904), and the Rutherford model (1911) came the Rutherford–Bohr model or just Bohr model for short (1913). The improvement to the Rutherford model is mostly a quantum physical interpretation of it. The Bohr model has been superseded, but the quantum theory remains sound.The model's key success lay in explaining the Rydberg formula for the spectral emission lines of atomic hydrogen. While the Rydberg formula had been known experimentally, it did not gain a theoretical underpinning until the Bohr model was introduced. Not only did the Bohr model explain the reason for the structure of the Rydberg formula, it also provided a justification for its empirical results in terms of fundamental physical constants.The Bohr model is a relatively primitive model of the hydrogen atom, compared to the valence shell atom. As a theory, it can be derived as a first-order approximation of the hydrogen atom using the broader and much more accurate quantum mechanics and thus may be considered to be an obsolete scientific theory. However, because of its simplicity, and its correct results for selected systems (see below for application), the Bohr model is still commonly taught to introduce students to quantum mechanics or energy level diagrams before moving on to the more accurate, but more complex, valence shell atom. A related model was originally proposed by Arthur Erich Haas in 1910, but was rejected. The quantum theory of the period between Planck's discovery of the quantum (1900) and the advent of a full-blown quantum mechanics (1925) is often referred to as the old quantum theory.
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