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+1/2
+1/2

... Chromodynamics :- theory of the strong interaction, colour plays the same role as charge in electrodynamics. Need three colours, but hadrons have to be colourless Use red, green and blue (parallel to TV and photo and print) Anti-colours = white – colour ; cyan, magenta and yellow ...
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Elementary Linear Algebra
Elementary Linear Algebra

... sum A+B is the matrix obtained by adding the entries of B to the corresponding entries of A. Vice versa, the difference A-B is the matrix obtained by subtracting the entries of B from the corresponding entries of A. Note: Matrices of different sizes cannot be added or ...
Chern-Simons theory and Weyl quantization
Chern-Simons theory and Weyl quantization

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Chapter 7 The Collapse of the Wave Function
Chapter 7 The Collapse of the Wave Function

... We have also said that x spin and z spin can’t be known at the same time, so if you’ve measured x spin, the particle can’t have a definite value of z spin. And, we saw previously that evidently an SGx machine makes this measurement of x spin, because you can figure out the x spin of the electron by ...
new TPC (NTPC)
new TPC (NTPC)

Exact Solutions for Non-Hermitian Dirac
Exact Solutions for Non-Hermitian Dirac

... Here we are producing our investigation of non-Hermitian systems with γ5 -mass term extension taking into account the external magnetic field. We also are studying the spectral and polarization properties of such systems and with this aim we start to consider solutions of the modified Dirac equation ...
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Anderson transition ???????? Critical Statistics
Anderson transition ???????? Critical Statistics

... are universally described by random matrix theory. With the help of the one parameter scaling theory we propose an alternative characterization of this universality class. It is also identified the universality class associated to the metal-insulator transition. In low dimensions it is characterized ...
Conservation Laws
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Relaxation dynamics of a quantum Brownian particle in an ideal gas
Relaxation dynamics of a quantum Brownian particle in an ideal gas

... state. The gas particles then do not interact with each other, but they influence the Brownian particle via two-body forces, which should be taken sufficiently short-ranged to permit a scattering theory description of the interaction processes. The corresponding effective equation of motion for the quan ...
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... function at any time t and position x. Once we have the wave function, our problem is “solved.” In this chapter we will solve Schrödinger's equation for some simple potentials. Let’s get to work… ...
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First Principle Calculations of Positron

... Positron state in a CdSe Qdot • The state of the positron can be explained in terms of the positron Affinity (calculated by DFT GGA) between the Qdot and the matrix. • Potential well is about 2 eV therefore positrons are trapped in the CdSe Qdots. • Using an LMTO basis set we find that almost 80% o ...
Testing the Symmetrization Postulate of Quantum Mechanics and
Testing the Symmetrization Postulate of Quantum Mechanics and

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An Introduction to Elementary Particle Phenomenology

View Commentary  - Journal Club for Condensed Matter Physics
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Fermion Doubling in Loop Quantum Gravity - UWSpace
Fermion Doubling in Loop Quantum Gravity - UWSpace

... 2.2. NIELSEN-NINOMIYA NO-GO THEOREM lattices with a compact (closed and bounded) momentum space. This is the key feature we will look at in our proof. Helicity is not a meaningful observable if a particle is massive. This can be summarized quite simply, a massive particle does not travel at the spe ...
Quantum Hall effect in three-dimensional layered systems Yigal Meir
Quantum Hall effect in three-dimensional layered systems Yigal Meir

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L z

... The vector model This is a useful semi-classical model of the quantum results. Imagine L precesses around the z-axis. Hence the magnitude of L and the z-component Lz are constant while the x and y components can take a range of values and average to zero, just like the quantum eigenfunctions. A giv ...
L. Snobl: Representations of Lie algebras, Casimir operators and
L. Snobl: Representations of Lie algebras, Casimir operators and

The integer quantum Hall effect II
The integer quantum Hall effect II

Chapter 12
Chapter 12

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Symmetry in quantum mechanics

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