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Charge conjugation

For the fields we have been considering the parity operator P has the following effect  [Pg.447]

It follows that is a vector, whereas 7 75 is a pseudo-vector, [Pg.447]

The charge conjugation operator C has the following effect CAfj, x,t)C = -Afj, x,t) for photons. [Pg.447]

Thus an n-photon state is an eigenstate of C with eigenvalue (—1) , known as the charge parity. [Pg.447]

It follows that the vector current built firom coloured quarks (Section 21.3) behaves under charge conjugation as follows  [Pg.448]

Graphite is an example of a zero-bandgap pol)mer whose behavior is metal-like. Most pol)mers behave more like semiconductors and require doping to achieve high conductivity (see Chapter 20 for more details). [Pg.351]

The Drude theory treats the electrons in a metal as a classical monatomic gas. This simple theory is able to explain many observed properties of metals such as why they are good [Pg.351]

To satisfy Ohm s law, this collision time must be independent of the field. If we assume that these collisions are between the electrons traveling over some mean free path A that is associated with the lattice, the average speed of the electrons would have to be much larger than the drift speed produced by the applied electric field. This would be the case if the electrons behaved as an ideal gas in thermal equilibrium with the lattice. [Pg.352]

The resistivity p = l/tr is found to have a linear relationship with temperature in the form p T) = po + aT (Matthiessen s rule), where po is due to collisions with structural and impurity imperfections and the temperature dependence comes about from collisions with the lattice ions whose cross sections increase linearly with temperature. Impurity atoms, such as foimd in solid solution alloys, produce a much larger increase in resistivity than structural defects such as dislocations and grain boundaries or condensed second phases because they are more widely dispersed. Also there is a departure from the linear temperature dependence of the resistivity at low temperatures because all of the phonon modes are active. Griineisen used the Debye theory to develop a universal relationship between reduced resistivity and reduced temperature that holds for all metals. [Pg.352]

The observed first power relation between resistivity and temperature implies that the collision velocity must not only be independent of the applied field and be much greater than the drift velocity but must also be independent of temperature, which rules out the thermal velocity as the motion responsible for the observed collision rate. With the discovery of quantum mechanics, the difficulties encountered by the classical electron gas model are resolved by having the electrons travel at the Fermi velocity. [Pg.352]


For a discussion of the transformation of the field operators under improper Lorentz transformations and discrete symmetry operations such as charge conjugation, see ... [Pg.547]

Invariance of Quantum Electrodynamics under Discrete Transformations.—In the present section we consider the invariance of quantum electrodynamics under discrete symmetry operations, such as space-inversion, time-inversion, and charge conjugation. [Pg.679]

The above transformation properties of the current operator make quantum electrodynamics invariant under the operation Ue, usually called charge conjugation, provided... [Pg.685]

The invariance of quantum electrodynamics under charge conjugation has several immediate consequences. [Pg.686]

A state of n incoming (outgoing) photons has the charge conjugation eigenvalue (— 1)". [Pg.686]

The invariance of the theory under charge conjugation implies that... [Pg.697]

Charge conjugate operator, 545 Charge-current density renormalized, 597... [Pg.771]

All solutions of this Hamiltonian are thereby electronic, whether they are of positive or negative energy and contrary to what is often stated in the literature. Positronic solutions are obtained by charge conjugation. From the expectation value of the Dirac Hamiltonian (23) and from consideration of the interaction Lagrangian (16) relativistic charge and current density are readily identified as... [Pg.390]

Figure 3 The MALDI-TOF mass spectrum of the chymotrypsin conjugate with a ST-PHPMA-NHNH2 fraction = 1,400). The peaks 1, 2, and 3 are the double-charged, single-charged conjugate, and single-charged double conjugate aggregate, respectively. Figure 3 The MALDI-TOF mass spectrum of the chymotrypsin conjugate with a ST-PHPMA-NHNH2 fraction = 1,400). The peaks 1, 2, and 3 are the double-charged, single-charged conjugate, and single-charged double conjugate aggregate, respectively.
Proton removal for the purpose of preparing negatively charged conjugate bases in conditions suitable for direct NMR observation may be effected on exposure of the free amine to strongly basic conditions such as potassium amide in liquid ammonia for ben-zazonine (5c) and potassium mirror in THF for aza[13]annulene (37a). [Pg.727]

Once formed, the source dipole is a broken symmetry [2] in the vacuum s energy flux along the lines experimentally shown by Wu et al. in 1957 [35]. As Lee points out, the asymmetry between opposite signs of electric charge is called C violation, or charge conjugation violation, or sometimes particle-antiparticle asymmetry. As Nobelist Lee [2] further states, Since non-obser-vables imply symmetry, these discoveries of asymmetry must imply observables. ... [Pg.663]

Another type of symmetry of importance in elementary particle physics is that entitled charge conjugation. This principle slates that if each particle in a given isolated system is replaced by its corresponding anliparticle, then no difference can be observed. For example, if. in a hydrogen atom, the proton is replaced by an anti-proton and the electron is replaced hy a positron, then this antimatter atom will behave exactly like an ordinary atom, so long as it does not come inlo contact with ordinary atoms. [Pg.433]

However, the symmetry of the situation can be restored if we interchange the words right and "left in the description of the experiment at the same time that we exchange each particle with its antiparticle. In the above experiment, this is equivalent to replacing the word clockwise with counterclockwise. When this is done, the positrons arc emitted in the downward direction, just as the electrons m the original experiment. The laws of nature are thus found to be invariant to the simultaneous application of charge conjugation and mirror inversion. [Pg.1211]

Time reversal invariance describes the fact that in reactions between elementary particles, it does not make any difference if the direction of the time coordinate is reversed. Since all reactions are invariant to simultaneous application of mirror inversion, charge conjugation, and time reversal, the combination of all three is called CPT symmetry and is considered to be a very fundamental symmetry of nature. [Pg.1211]

CH3NH2 > NH3.89 Water falls between diethylamine and ammonia. The observed order jsjrenerally consistent theory that the charged conjugate... [Pg.155]

So diat charge is conserved, anionic bases upon reaction with a proton give neutral conjugate acids neutral bases upon reaction with a proton give positively charged conjugate acids. Occasionally shared pairs of electrons can be given up to a proton such as when olefins react with acids. In such cases n electrons are die electron pair which forms a bond to the proton. [Pg.48]

An electron can bind to positronium to form Ps, provided that the two electrons are in a singlet spin state. This system, and its charge conjugate counterpart consisting of two positrons and one electron, was... [Pg.362]


See other pages where Charge conjugation is mentioned: [Pg.177]    [Pg.155]    [Pg.123]    [Pg.545]    [Pg.624]    [Pg.707]    [Pg.7]    [Pg.853]    [Pg.258]    [Pg.240]    [Pg.278]    [Pg.157]    [Pg.181]    [Pg.176]    [Pg.219]    [Pg.226]    [Pg.255]    [Pg.382]    [Pg.222]    [Pg.631]    [Pg.254]    [Pg.705]    [Pg.433]    [Pg.658]    [Pg.125]    [Pg.188]    [Pg.4]    [Pg.10]    [Pg.36]    [Pg.330]    [Pg.331]    [Pg.363]   
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Charge Carrier Transport in Conjugated Polymers

Charge Storage States in Conjugated Polymers

Charge Transfer in Conjugated Polymers

Charge Transport in Conjugated Polymers

Charge carriers in conjugated polymers

Charge conjugated polymers

Charge conjugation invariance

Charge conjugation-parity-time

Charge distribution conjugation

Charge luminescent conjugated polymers

Charge transport in conjugated

Conjugate bases negative charges

Conjugated charge transport

Conjugated interfacial charge separation

Conjugated polymers charge carriers

Conjugated polymers charge transfer processes

Conjugated polymers charge transport

Conjugated polymers photoinduced charge transfer

Conjugated systems charge distribution

Electrical Conductivity and Charges on Conjugated Chains

Invariance with respect to charge conjugation

Negatively charge conjugates

Operators charge conjugation

Poly charge-conjugation symmetric

Principles, symmetry charge conjugation

Symmetry charge-conjugation

The Nature of Charge Carriers in Conjugated Polymers

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