The quantum does not reduce to discrete bits
... As an example of a physicist who yearns for a hidden variable theory, Lee Smolin wrote recently, in response to an Edge.org question: I worry that we don't really understand quantum phenomena. … But there is another possibility: that quantum mechanics does not provide an explanation for what happens ...
... As an example of a physicist who yearns for a hidden variable theory, Lee Smolin wrote recently, in response to an Edge.org question: I worry that we don't really understand quantum phenomena. … But there is another possibility: that quantum mechanics does not provide an explanation for what happens ...
Transport Electron through a Quantum Wire by Side-Attached Asymmetric Quantum-Dot Chains
... Figure 3.a, N=3 and M=4 are set for first and second chains. It is clear that the sum of dots in two-chains (N+M) determines the number of anti-resonances in conductance spectrum and it is independent of the value of p. In other words, the number of mini gaps matches exactly the number of QDs chains ...
... Figure 3.a, N=3 and M=4 are set for first and second chains. It is clear that the sum of dots in two-chains (N+M) determines the number of anti-resonances in conductance spectrum and it is independent of the value of p. In other words, the number of mini gaps matches exactly the number of QDs chains ...
Chapter3
... Let (x*,u*,,μ,,) satisfy the necessary conditions in (3.11). If H(x,u,(t),t) is concave in (x,u) at each t[0,T], S in (3.2) is concave in x, g in (3.3) is quasiconcave in (x,u), a in (3.4) is quasiconcave in x, and b in (3.5) is linear in x, then (x*,u*) is optimal. The concavity of the Hamilto ...
... Let (x*,u*,,μ,,) satisfy the necessary conditions in (3.11). If H(x,u,(t),t) is concave in (x,u) at each t[0,T], S in (3.2) is concave in x, g in (3.3) is quasiconcave in (x,u), a in (3.4) is quasiconcave in x, and b in (3.5) is linear in x, then (x*,u*) is optimal. The concavity of the Hamilto ...
lowdin`s remarks on the aufbau principle and a philosopher`s view of
... tendency to exaggerate its success, especially on the part of some practicing quantum chemists and physicists. As a philosopher of chemistry I have the luxury of being able to examine the field as an outsider and of asking the kinds of questions which true practitioners might not even contemplate. T ...
... tendency to exaggerate its success, especially on the part of some practicing quantum chemists and physicists. As a philosopher of chemistry I have the luxury of being able to examine the field as an outsider and of asking the kinds of questions which true practitioners might not even contemplate. T ...
The potential quark model in theory of resonances
... • The complex energy is an appropriate tool in the studying of resonances. • A resonance is supposed to take place at E and to have “half–value breath” Г/2 [2]. • The imaginary part Г was associated with the inverse of the lifetime Г = 1/τ. • Such ‘decaying states’ were the first application of quant ...
... • The complex energy is an appropriate tool in the studying of resonances. • A resonance is supposed to take place at E and to have “half–value breath” Г/2 [2]. • The imaginary part Г was associated with the inverse of the lifetime Г = 1/τ. • Such ‘decaying states’ were the first application of quant ...
Document
... What is the nature of light? Although the velocity of light is large, it is not infinite. c = 300,000 km/sec or c = 186,000 miles/sec Ordinary matter cannot travel faster than the speed of light. ...
... What is the nature of light? Although the velocity of light is large, it is not infinite. c = 300,000 km/sec or c = 186,000 miles/sec Ordinary matter cannot travel faster than the speed of light. ...
Complete Analytical Solutions of the Mie
... eigenfunctions of H(q) respectively, then the HFT states that ∂En (q) ∂H(q) = hΨn (q)| |Ψn (q)i . ...
... eigenfunctions of H(q) respectively, then the HFT states that ∂En (q) ∂H(q) = hΨn (q)| |Ψn (q)i . ...
Lectures 10-11
... Thus, if we’re willing to accept more uncertainty about an electron’s momentum, we can have more certainty in knowing its position – and vice versa. This inverse relationship can be ...
... Thus, if we’re willing to accept more uncertainty about an electron’s momentum, we can have more certainty in knowing its position – and vice versa. This inverse relationship can be ...
Lectures 10-11
... Thus, if we’re willing to accept more uncertainty about an electron’s momentum, we can have more certainty in knowing its position – and vice versa. This inverse relationship can be ...
... Thus, if we’re willing to accept more uncertainty about an electron’s momentum, we can have more certainty in knowing its position – and vice versa. This inverse relationship can be ...
Lectures 6-7
... Thus, if we’re willing to accept more uncertainty about an electron’s momentum, we can have more certainty in knowing its position – and vice versa. This inverse relationship can be ...
... Thus, if we’re willing to accept more uncertainty about an electron’s momentum, we can have more certainty in knowing its position – and vice versa. This inverse relationship can be ...
a non-perturbative approach for quantum field theory
... Obtain the eigenvalues (electron mass) and eigenstates (electron wavefunctions) for ground state (physical electron) and several low-lying excited states (excited electrons) Evaluate other observables (anomalous magnetic moment, parton distribution function) from electron wavefunction (vector-matrix ...
... Obtain the eigenvalues (electron mass) and eigenstates (electron wavefunctions) for ground state (physical electron) and several low-lying excited states (excited electrons) Evaluate other observables (anomalous magnetic moment, parton distribution function) from electron wavefunction (vector-matrix ...
Momentum and Impulse
... Linear Momentum A new fundamental quantity, like force, energy The linear momentum p of an object of mass m moving with a velocity v is defined to be the product of the mass and velocity: ...
... Linear Momentum A new fundamental quantity, like force, energy The linear momentum p of an object of mass m moving with a velocity v is defined to be the product of the mass and velocity: ...
The importance of the Empty Set and
... but if one goes back in history one will find that the ancient Chinese may have been there first. Third one has to look at the work and philosophy of Henri Poincaré to deepen our understanding of the complete induction method. Fourth is to look at the science of converging and diverging series. Fift ...
... but if one goes back in history one will find that the ancient Chinese may have been there first. Third one has to look at the work and philosophy of Henri Poincaré to deepen our understanding of the complete induction method. Fourth is to look at the science of converging and diverging series. Fift ...
Quantum Theory of Radiation
... Dirac's theory of radiation is based on a very simple idea; instead of considering an atom and the radiation field with which it interacts as two distinct systems, he treats them as a single system whose energy is the sum of three terms: one representing the energy of the atom, a second representing ...
... Dirac's theory of radiation is based on a very simple idea; instead of considering an atom and the radiation field with which it interacts as two distinct systems, he treats them as a single system whose energy is the sum of three terms: one representing the energy of the atom, a second representing ...
Transport properties of quantum-classical systems
... In this article we construct general quantum-classical expressions for transport properties, starting from a full quantum treatment of the entire many-body system. The transport coefficient formulas again retain the full quantum equilibrium structure of the system and entail carrying out quantumclas ...
... In this article we construct general quantum-classical expressions for transport properties, starting from a full quantum treatment of the entire many-body system. The transport coefficient formulas again retain the full quantum equilibrium structure of the system and entail carrying out quantumclas ...
SECTION 6-3 Systems Involving Second
... case, we are only interested in real solutions. We start by solving the second equation for y in terms of x and substituting the result into the first equation. y x2 ...
... case, we are only interested in real solutions. We start by solving the second equation for y in terms of x and substituting the result into the first equation. y x2 ...
