Production Mechanism of Quark Gluon Plasma in Heavy Ion
... color strings are formed between them. These strings merge to form ‘color rope’ (i.e. CEF is formed). Consequently the production process reduces to the instability of the QCD vacuum in the presence of a classical CEF which is in general space-time dependent. We study both the 2 g and q q production ...
... color strings are formed between them. These strings merge to form ‘color rope’ (i.e. CEF is formed). Consequently the production process reduces to the instability of the QCD vacuum in the presence of a classical CEF which is in general space-time dependent. We study both the 2 g and q q production ...
Phenomenological study of scalar and pseudo
... Discovery of the Higgs boson at the LHC in 2012 However the SM ignore many physical observed phenomena The gravitational interaction Matter-antimatter asymmetry No dark matter Neutrinos mass And suffer from theoretical problem in the Higgs sector Introduce an ad hoc potential in the theory The fine- ...
... Discovery of the Higgs boson at the LHC in 2012 However the SM ignore many physical observed phenomena The gravitational interaction Matter-antimatter asymmetry No dark matter Neutrinos mass And suffer from theoretical problem in the Higgs sector Introduce an ad hoc potential in the theory The fine- ...
Some Basic Aspects of Fractional Quantum Numbers
... This field theory description does not yet quite correspond to the picture of polyacetylene sketched in the previous section, because the breaking of translational symmetry (from x → x + a to x → x + 2a) has not appeared. We need not change the equations, however, we need only draw out their implica ...
... This field theory description does not yet quite correspond to the picture of polyacetylene sketched in the previous section, because the breaking of translational symmetry (from x → x + a to x → x + 2a) has not appeared. We need not change the equations, however, we need only draw out their implica ...
Solution to Exercise 2.1-2: Density of States for Lower Dimensions
... Solution to Exercise 2.1-2: Density of States for Lower Dimensions Calculate the density of states for a one-dimensional semiconductor ("quantum wire") and for the two-dimensional case. Draw some conclusions from the results. The number of states Z(k) up to a wave vector k is generally given by Volu ...
... Solution to Exercise 2.1-2: Density of States for Lower Dimensions Calculate the density of states for a one-dimensional semiconductor ("quantum wire") and for the two-dimensional case. Draw some conclusions from the results. The number of states Z(k) up to a wave vector k is generally given by Volu ...
1 Heisenberg Uncertainty Principle
... electron with an uncertainty δx, by having the electron interact with X-ray light. For an X-ray of wavelength λ, the best that can be done is δx ∼ λ. But if an X-ray photon scatters from an electron, it will disturb the electron’s momentum by an amount δp. We expect δp to be of order the X-ray photo ...
... electron with an uncertainty δx, by having the electron interact with X-ray light. For an X-ray of wavelength λ, the best that can be done is δx ∼ λ. But if an X-ray photon scatters from an electron, it will disturb the electron’s momentum by an amount δp. We expect δp to be of order the X-ray photo ...
Simulation programs for teaching quantum mechanics
... width. In a hands-on session the students are asked to quantify this behaviour, which leads to a first glimpse at the Heisenberg uncertainty relation. The uncertainty relation for a free particle After the notions of position and momentum uncertainty have been introduced, the next program displays t ...
... width. In a hands-on session the students are asked to quantify this behaviour, which leads to a first glimpse at the Heisenberg uncertainty relation. The uncertainty relation for a free particle After the notions of position and momentum uncertainty have been introduced, the next program displays t ...
quarks
... 1926 Schroedinger develops wave mechanics, which describes the behavior of quantum systems for bosons. Born gives a probability interpretation of quantum mechanics.G.N. Lewis proposes the name "photon" for a light quantum. 1927 Certain materials had been observed to emit electrons (beta decay). Sinc ...
... 1926 Schroedinger develops wave mechanics, which describes the behavior of quantum systems for bosons. Born gives a probability interpretation of quantum mechanics.G.N. Lewis proposes the name "photon" for a light quantum. 1927 Certain materials had been observed to emit electrons (beta decay). Sinc ...
Lecture 2: Dirac Notation and Two-State Systems
... bra, can be represented by a row matrix with complex-conjugated numbers. An operator can be expanded in terms of |ei ihej |. The coefficient of the expansion is hei |O|ej i and can be arranged in the form of a square matrix. All expressions in terms of bras, kets, and operators can be converted into ...
... bra, can be represented by a row matrix with complex-conjugated numbers. An operator can be expanded in terms of |ei ihej |. The coefficient of the expansion is hei |O|ej i and can be arranged in the form of a square matrix. All expressions in terms of bras, kets, and operators can be converted into ...