
Atomic Physics
... technological applications thereof. For example, the fact that each element has its own characteristic “fingerprint” spectrum has contributed significantly to advances in material science and also in cosmology. ...
... technological applications thereof. For example, the fact that each element has its own characteristic “fingerprint” spectrum has contributed significantly to advances in material science and also in cosmology. ...
Transitions between highly excited states of an atom when a neutral
... conclusion: for transitions with change n-tn' of the principal quantum number there can occur a situation which is the inverse of I-mixing, i.e., the predominant contribution of the collisions of the neutrals with the core. This fact was established for the system H(n) He(ls2)as a result of the comp ...
... conclusion: for transitions with change n-tn' of the principal quantum number there can occur a situation which is the inverse of I-mixing, i.e., the predominant contribution of the collisions of the neutrals with the core. This fact was established for the system H(n) He(ls2)as a result of the comp ...
Electrical properties
... – This type of impurity is called an acceptor as it accepts an electron from the valence band and generates a hole – Energy level within the band gap is called an acceptor state – Holes are present in much higher concentrations than free electrons (p >> n) – Material is referred to as p-type because ...
... – This type of impurity is called an acceptor as it accepts an electron from the valence band and generates a hole – Energy level within the band gap is called an acceptor state – Holes are present in much higher concentrations than free electrons (p >> n) – Material is referred to as p-type because ...
Trapped-Electron Runaway Effect
... 2011; Paz-Soldan et al. 2014). It is clearly important to understand the behaviour of the runaway electrons in order to optimize a runaway electron mitigation strategy. The runaway electron population in tokamaks typically arises from the acceleration of electrons with large parallel velocities, on ...
... 2011; Paz-Soldan et al. 2014). It is clearly important to understand the behaviour of the runaway electrons in order to optimize a runaway electron mitigation strategy. The runaway electron population in tokamaks typically arises from the acceleration of electrons with large parallel velocities, on ...
Review of Atomic Structure
... A logical place for an electrical engineer or a physicist to begin his study of solid state physics is with the rudiments of quantum mechanics. Quantum mechanics was developed because classical mechanics failed to explain the behaviour of atoms. As an example, consider the hydrogen atom consisting o ...
... A logical place for an electrical engineer or a physicist to begin his study of solid state physics is with the rudiments of quantum mechanics. Quantum mechanics was developed because classical mechanics failed to explain the behaviour of atoms. As an example, consider the hydrogen atom consisting o ...
Chapter 2 Semiconductor Heterostructures
... The current flow in a forward biased pn device can be understood as follows. In equilibrium, the drift components of both the electron and hole currents balanced the respective diffusive components. When a forward bias is applied, the electric field in the junction is reduced and therefore the drift ...
... The current flow in a forward biased pn device can be understood as follows. In equilibrium, the drift components of both the electron and hole currents balanced the respective diffusive components. When a forward bias is applied, the electric field in the junction is reduced and therefore the drift ...
6 Weak Interactions
... always have an energy equal to the difference between the initial and final nuclear sthatate energies. Measurements showed, however, that the electron’s energy was variable and calorimetric measurements confirmed that some of the energy was being lost. So disturbing was this problem that Bohr even s ...
... always have an energy equal to the difference between the initial and final nuclear sthatate energies. Measurements showed, however, that the electron’s energy was variable and calorimetric measurements confirmed that some of the energy was being lost. So disturbing was this problem that Bohr even s ...
Chapter 12 - NCERT books
... The scattering data shown in Fig. 12.3 can be analysed by employing Rutherford’s nuclear model of the atom. As the gold foil is very thin, it can be assumed that α-particles will suffer not more than one scattering during their passage through it. Therefore, computation of the trajectory of an alpha ...
... The scattering data shown in Fig. 12.3 can be analysed by employing Rutherford’s nuclear model of the atom. As the gold foil is very thin, it can be assumed that α-particles will suffer not more than one scattering during their passage through it. Therefore, computation of the trajectory of an alpha ...
Atoms
... What particles are atoms made of? For some time, people thought that atoms were the smallest particles and could not be broken into anything smaller. Scientists now know that atoms are actually made from even smaller particles. There are three types: ...
... What particles are atoms made of? For some time, people thought that atoms were the smallest particles and could not be broken into anything smaller. Scientists now know that atoms are actually made from even smaller particles. There are three types: ...
Electric Charge
... • To keep a charge on the sphere, you can attach a ground to the sphere. A ground is a conducting path between an object and the earth to prevent an electric shock due to excess charge. • Earth is a conductor and can act as a source for extra electrons or as a sink for unwanted electrons. ...
... • To keep a charge on the sphere, you can attach a ground to the sphere. A ground is a conducting path between an object and the earth to prevent an electric shock due to excess charge. • Earth is a conductor and can act as a source for extra electrons or as a sink for unwanted electrons. ...
atoms - eVirtualGuru
... The scattering data shown in Fig. 12.3 can be analysed by employing Rutherford’s nuclear model of the atom. As the gold foil is very thin, it can be assumed that α-particles will suffer not more than one scattering during their passage through it. Therefore, computation of the trajectory of an alpha ...
... The scattering data shown in Fig. 12.3 can be analysed by employing Rutherford’s nuclear model of the atom. As the gold foil is very thin, it can be assumed that α-particles will suffer not more than one scattering during their passage through it. Therefore, computation of the trajectory of an alpha ...
Influence of thin film on the electrical properties of pulsed plasmas
... decay times of ions should be the same as the decay times of electrons. Figure 4 shows also the discharge times of the voltage ΔVf of the capacitors C on the both electrodes. It can be seen that the decay times of ne are behaving in the same way as the discharge times of the capacitor. Since we assu ...
... decay times of ions should be the same as the decay times of electrons. Figure 4 shows also the discharge times of the voltage ΔVf of the capacitors C on the both electrodes. It can be seen that the decay times of ne are behaving in the same way as the discharge times of the capacitor. Since we assu ...
Oxidation Numbers and Ionic Compounds
... 3. We can figure out for sure what type of bond will form between atoms by looking at electronegativities. a. An ionic bond will form between atoms who’s electronegativities differ by (more/less than) ___________. b. A covalent bond will form between atoms who’s electronegativities differ by (more/l ...
... 3. We can figure out for sure what type of bond will form between atoms by looking at electronegativities. a. An ionic bond will form between atoms who’s electronegativities differ by (more/less than) ___________. b. A covalent bond will form between atoms who’s electronegativities differ by (more/l ...
Zeeman effect and magnetic resonance
... Landé-factor g spin g j is nearly the same as the Landé-factor of a free electron. The theoretically expected value for the Landé-factor of the DPPH specimen can be obtained when inserting the values for L ( L 0 ) and S ( S 12 ) in equation (12). One gets: ...
... Landé-factor g spin g j is nearly the same as the Landé-factor of a free electron. The theoretically expected value for the Landé-factor of the DPPH specimen can be obtained when inserting the values for L ( L 0 ) and S ( S 12 ) in equation (12). One gets: ...
4.2 The Structure of an Atom
... an atom is balanced by a negative charge. That means the atomic number of an element also equals the number of electrons in an atom of that element. • Hydrogen has an atomic number of 1, so a hydrogen atom has 1 electron. • Sulfur has an atomic number of 16, so a sulfur atom has 16 electrons. ...
... an atom is balanced by a negative charge. That means the atomic number of an element also equals the number of electrons in an atom of that element. • Hydrogen has an atomic number of 1, so a hydrogen atom has 1 electron. • Sulfur has an atomic number of 16, so a sulfur atom has 16 electrons. ...
Interplay of AharonovBohm and Berry Phases for a Quantum Cloud
... distance L apart. Two extreme cases are easily solved. When the distance between the solenoids is much larger than the size of the atom, we can move the atom in the vicinity of one of the solenoids without the electron cloud touching the other solenoid. In this case, the atom collects a phase of 7~ ...
... distance L apart. Two extreme cases are easily solved. When the distance between the solenoids is much larger than the size of the atom, we can move the atom in the vicinity of one of the solenoids without the electron cloud touching the other solenoid. In this case, the atom collects a phase of 7~ ...
Electron

The electron is a subatomic particle, symbol e− or β−, with a negative elementary electric charge. Electrons belong to the first generation of the lepton particle family, and are generally thought to be elementary particles because they have no known components or substructure. The electron has a mass that is approximately 1/1836 that of the proton. Quantum mechanical properties of the electron include an intrinsic angular momentum (spin) of a half-integer value in units of ħ, which means that it is a fermion. Being fermions, no two electrons can occupy the same quantum state, in accordance with the Pauli exclusion principle. Like all matter, electrons have properties of both particles and waves, and so can collide with other particles and can be diffracted like light. The wave properties of electrons are easier to observe with experiments than those of other particles like neutrons and protons because electrons have a lower mass and hence a higher De Broglie wavelength for typical energies.Many physical phenomena involve electrons in an essential role, such as electricity, magnetism, and thermal conductivity, and they also participate in gravitational, electromagnetic and weak interactions. An electron generates an electric field surrounding it. An electron moving relative to an observer generates a magnetic field. External magnetic fields deflect an electron. Electrons radiate or absorb energy in the form of photons when accelerated. Laboratory instruments are capable of containing and observing individual electrons as well as electron plasma using electromagnetic fields, whereas dedicated telescopes can detect electron plasma in outer space. Electrons have many applications, including electronics, welding, cathode ray tubes, electron microscopes, radiation therapy, lasers, gaseous ionization detectors and particle accelerators.Interactions involving electrons and other subatomic particles are of interest in fields such as chemistry and nuclear physics. The Coulomb force interaction between positive protons inside atomic nuclei and negative electrons composes atoms. Ionization or changes in the proportions of particles changes the binding energy of the system. The exchange or sharing of the electrons between two or more atoms is the main cause of chemical bonding. British natural philosopher Richard Laming first hypothesized the concept of an indivisible quantity of electric charge to explain the chemical properties of atoms in 1838; Irish physicist George Johnstone Stoney named this charge 'electron' in 1891, and J. J. Thomson and his team of British physicists identified it as a particle in 1897. Electrons can also participate in nuclear reactions, such as nucleosynthesis in stars, where they are known as beta particles. Electrons may be created through beta decay of radioactive isotopes and in high-energy collisions, for instance when cosmic rays enter the atmosphere. The antiparticle of the electron is called the positron; it is identical to the electron except that it carries electrical and other charges of the opposite sign. When an electron collides with a positron, both particles may be totally annihilated, producing gamma ray photons.