THE EXPLORATION OF MICROCOSM IN XX CENTURY

FROM THE RESEARCHES ON CATHODE RAYS TO THE STANDARD MODEL

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Webmaster & Author: Antonino Cucinotta
Graduate in Physics
Copyright 2002 - All rights reserved


THE EXPERIMENTS ON CATHODE RAYS

THE DISCOVERY OF X-RAYS ( 1895)

THE DISCOVERY OF THE NATURAL RADIOACTIVITY (1896)

THE DISCOVERY OF ELECTRON (1897)

THE MAX PLANCK QUANTIZATION HYPOTHESIS OF THE RADIANT ENERGY EMITTED BY A BLACK BODY ( 1900 )

THE SPECIAL RELATIVITY THEORY OF ALBERT EINSTEIN

EINSTEIN'S HYPOTHESIS OF PHOTONS PERMITS TO EXPLAIN THE PHOTOELECTRIC EFFECT ( 1905)

THE DISCOVERY OF THE ATOMIC NUCLEUS ( 1911 )

THE X-RAYS DIFFRACTION EXPERIMENTS AND THE STUDIES ON THE CRYSTAL LATTICES (1912-13)

BOHR-RUTHERFORD'S ATOMIC MODEL (1913)

DE BROGLIE'S WAVE-LIKE HYPOTHESIS OF THE MICRO-WORLD PARTICLES (1924)

SCHROEDINGER'S NON-RELATIVISTIC QUANTUM MECHANICS (1925)

HEISENBERG'S UNCERTAINTY PRINCIPLE (1926)

THE DISCOVERY OF THE ELECTRON SPIN ( 1927)

THE ELECTRON DIFFRACTION EXPERIMENTS(1927)

DIRAC'S RELATIVISTIC QUANTUM MECHANICS AND ANTIMATTER HYPOTHESIS (1928)

PAULI'S NEUTRINO HYPOTHESIS(1930)

THE DISCOVERY OF NEUTRON (1932)

ENRICO FERMI'S RESEARCHES ON NEUTRONS (1934-1938)

THE DISCOVERY OF THE URANIUM FISSION (1939 )

FROM THE RESEARCHES ON THE COSMIC RAYS TO THE HIGH ENERGY PHYSICS

THE FUNDAMENTAL PARTICLES OF MATTER: QUARKS AND LEPTONS

THE THREE GENERATIONS OF QUARKS AND LEPTONS IN THE STANDARD MODEL

THE FUNDAMENTAL FORCES OF NATURE AND THE STANDARD MODEL FORCE VECTORS

FROM THE STANDARD MODEL TO THE GREAT UNIFICATION THEORIES

ALBERT EINSTEIN'S THEORY OF THE SPECIAL RELATIVITY

In 1905 Albert Einstein extended to all the physical phenomena the relativity principle, that was formulated by Galileo for the mechanical phenomena and concerns the equivalence of all the inertial frames of reference, that is the not accelerate ones, as regards the acceleration of a body subiected to forces.
Einstein, after have assumed the invariability of the modulus of the velocity of light in any frame of reference, besides the (Lorentz's) transformation relations for spatial coordinates, necessary to describe a physical phenomenon in the transit from a inertial frame of reference to another, he considered the transformation of time, by introducing the concept of local time, that is the time measured by an observer in his own frame of reference, and by treating the time as the fourth co-ordinate in space-time.
From time relativization, that is a direct consequence of the finite and constant value of the velocity of light, derives the difference of the local duration of a physical phenomenon that is developing in an inertial frame of reference, in comparison with that appraised by another observer in an inertial frame of reference which is in rectilinear and uniform motion with respect to the first one.
As concerns dynamics, Einstein introduced the rest mass (mo), measured in a frame of reference in which a body is at rest, and the relativistic (or motion) mass m (v), that depends from the velocity (v) of the body referred to a generic inertial frame, in which it is in motion.
The relativistic mass depends on the velocity according to a law saying that a body with a non-zero rest mass, to be moving with the velocity of light, it needs an infinite kinetic energy.
In fact, because the mass is increasing with the velocity, it becomes infinite when the velocity is near to the value of the velocity of light, and therefore it is requested an infinite kinetic energy for v = c = 300000 Km/s.
The mass increase of a body is meaningful only when the velocity becomes comparable with the one of light.
Therefore, the field of the ideal verification of the m(v) law , is the one of subatomic particles, whose velocity is very near to the one of light.
Another ,very important consequence of relativistic effects, is the mass-energy conservation law, which implies the classical principles of the mass conservation and the one of energy conservation are unified in an only law, the so called mass-energy conservation law.
This law says that the variation of mass of a body, for an amount Dm = m-mo, is always associated to an emission or to an absorption of the energy DE = Dm c2.
This law allows to explain the operation of nuclear reactors, the origin and evolution of stars and all the interactions among elementary particles in high-energy physics experiments .

EINSTEIN'S HYPOTHESIS OF PHOTONS PERMITS TO EXPLAIN THE PHOTOELECTRIC EFFECT (1905)

The photoelectric effect consists in emission of electrons by a metallic surface on which is exposed to a light flux.
The effect takes place easily using metals as cesium, whose conduction electrons is weakly tied to ions of crystal lattice, in such a mode that it is needful a modest quantity of energy (extraction work) to extract them from a metal.
It is observed that every metal is characterized from a threshold wavelength, over which the photoelectric effect doesn't take place, and that the maximum speed of photoelectrons doesn't depend on the illumination intensity of the metallic surface.
It is also observed that the intensity of the photoelectric current is directly proportional to the illumination intensity.
By the laws of classical physics it isn't possible to explain the characteristics of this phenomenon.
It is owing to Albert Einstein ( Nobel prize winner in 1921 ) the theory of the photoelectric effect, that is based on the hypothesis of photons.
In fact Einstein, assuming as a postulate the quantization of energy, introduced by Max Planck in the study of the thermal radiation emitted by the black body (an ideal body characterized from the maximum emitting and absorbing power of the thermal radiation ),
did the hypothesis that photoelectrons are extracted from the metal as a consequence of their collisions with electromagnetic energy packets E = hf = hc/l, the so-called photons or quanta of light, where h is Planck's constant,l is the wavelength and f is the frequency of the electromagnetic radiation absorbed by the metal.
In such a mode, the maximal kinetic energy K with which are emitted photoelectrons, is given by the difference between the energy E of the colliding photon and the extraction work W ,which is characteristic of each metal: K = E - W.
It is immediate to understand the existence of a threshold wavelength, if we thinks that extracting an electron needs a photon with an energy at least equal to E = hc/lo - W, where lois the threshold-wavelength.
The fact that the intensity of the photoelectric current is proportional to the illumination intensity, is explained easily by thinking that exists a 1:1 ratio between the number of emitted photoelectrons and the one of absorbed photons, and that a ray of light is much more intense, the greater is the number of photons associated to it.
The validity of photon hypothesis was confirmed experimentally after the discovery of Compton effect (1923) , consisting in scattering of X and g photons by a light weight atoms against which they collide, with a variation of photon energy.
It was observed for the first time in a cloud chamber (a Wilson chamber ) the scattering of photons by electrons weakly-tied to nucleus, with increasing of the wavelenght of scattered radiation with respect to the one of incident radiation.
The consequent energy diminution of photons is equal to the kinetic energy of the electrons scattered by collision with photons.
The existence of photons is a consequence of the wave-particle-like dualism observed for electromagnetic radiation: electromagnetic radiation behaves as an electromagnetic wave beam, when it is travelling in a region with spatial dimensions much great in comparison with the ones of atoms.
When instead are considered atomic phenomena , electromagnetic radiation behaves as a beam of particles,that is energy packets, that is photons,which move with the velocity of light and interact with subatomic particles according to the energy and momentum conservation laws.

THE DISCOVERY OF ATOMIC NUCLEUS ( 1911 )

The English physicist Rutherford, helped by Geiger and Marsden, by means of several famous experiences effected at Cambridge University and consisting in bombarding thin gold layers with a particles (helium nuclei), discovered that nearly the whole mass of an atom is concentrated in its nucleus, having a positive electric charge and surrounded by electrons orbiting around it.

SOME EXAMPLES SHOWING BOTH THE MASS-INTO-ENERGY AND THE ENERGY-INTO-MASS CONVERSIONS

MASS CONVERSION INTO KINETIC ENERGY IN A THERMONUCLEAR REACTION OF FUSION

AN HIGH ENERGY COLLISION OF A DEUTERON ( deuterium nucleous = proton + neutron) AGAINST A TRITON (tritium nucleous = proton + 2 neutrons ) PRODUCING AN HELIUM NUCLEUS ( alpha particle = 2 protons + 2 neutrons ) AND A NEUTRON, WITH THE EMISSION OF A 17,8 Mev KINETIC ENERGY (MeV = Megaelettronvolt)




MASS CONVERSION INTO ELECTROMAGNETIC ENERGY

ANNIHILATION OF A PARTICLE-ANTIPARTICLE PAIR
( electron-positron, muon-antimuon, proton-antiproton )
NEAR AN ATOMIC NUCLEOUS ABSORBING THE MOMENTUM OF A PHOTON




ELECTROMAGNETIC ENERGY CONVERSION INTO MASS

CREATION OF A PARTICLE-ANTIPARTICLE PAIR
( electron-positron, muon-antimuon, proton-antiproton )
NEAR AN ATOMIC NUCLEOUS ABSORBING THE PHOTON MOMENTUM




X-RAYS DIFFRACTION EXPERIMENTS AND THE STUDIES ON THE CRYSTAL LATTICES ( 1912-13)

After discovery of X-rays and their wave-like nature,evidenced because they are deflected neither by electric nor magnetic fields, their wavelength had to be measured.
In 1913 the German physicist Max Von Laue ( Nobel prize winner in 1914 ) and the English physicists William Bragg and William Lawrence Bragg, father and son, (Nobel prize winners in 1915), by using crystals of vary types succeeded in getting some photographic images of the diffraction figures that were generated by interposing a crystal on the trajectory of X-rays.
W.H. Bragg and W.L. Bragg succeeded besides in measuring the wavelength and, after having improved the measure method of it by their invention of X-ray spectrometer, they were able to measure interatomic distances of many crystals, starting the X-ray diffractometry, which has a fundamental importance in studying the structure of matter.

THE BOHR-RUTHERFORD ATOMIC MODEL (1913)

Within the second decade of the twentieth century the physicists Rutherford, Bohr and Sommerfeld, developing Planck and Einstein's quantum theories about, respectively, the quantization of the electromagnetic radiation energy emitted by the black body, and the one of the electromagnetic energy absorbed by a metal emitting electrons by the photoelectric effect, they conceived the first quantum theory useful to calculate the wavelength of the optical and X-ray line spectra of hydrogen atom and of other one-electron atoms, that is helium and ionized lithium .
In particular the Danish physicist Bohr ( founder of the physics school at Copenaghen University and Nobel prize winner in 1922 ) , starting from the Rutherford's discovery of the atomic nucleous, proposed the first atomic model.
According to Bohr-Rutherford's model one atom is seen as a solar microscopic system to whicj can applied the laws of classical physics and some postulates to take account that, in the atomic micro-world, energy and angular momentum are quantized and that therefore their values are always multiples of an elementary quantity of energy ( E = h f ) or angular momentum L = nh/(2p) , where f is the frequency of the electromagnetic radiation,h is the universal Planck's constant and n is an integer number.
Bohr-Rutherford's model, improved by Sommerfeld by considering some relativistic effects, although is much elementary from a mathematical point of view, however it allows to calculate the energetic levels of one-electron atoms, but not the probability of transition of an electron between two energy levels, which is fundamental to calculate the relative intensity of the spectroscopic lines emitted or absorbed by atoms .

DE BROGLIE'S WAVE-LIKE HYPOTHESIS FOR THE MICRO-WORLD PARTICLES (1924)

The French physicist De Broglie (Nobel prize winner in 1929), extending to matter the wave-particle-like dualism introduced by Einstein's hypothesis of photons, proposed to associate with a particle with mass M , that is moving with velocity V, the wavelength
l = h /(MV), where h is Planck's constant.
This hypothesis allows to attribute to every material particle a wave-like nature,that is the more significant, the smaller is the particle momentum p = MV.
Therefore the wave-like effects results negligible if the mass of a particle is much greater of the one of micro-world particles forming atoms.

SCHROEDINGER'S NON-RELATIVISTIC QUANTUM MECHANICS (1925)

The elementary atomic model of Bohr-Rutherford represented only a provisional theoretical approach in waiting for an atomic complete theory .
The German physicist Erwin Schroedinger (Nobel prize winner 1933 ), assuming as a starting point the wave-like hypothesis of matter, built a quantum theory of the atom based on an equation suitable to describe the wave-like behaviour of atomic electrons.
Schroedinger's equation, originally conceived to describe the material waves associate to electrons, was reinterpretataed by Max Born ( Nobel prize winner 1954 ) as the probability-wave equation.
Therefore the Schroedinger equation ,when it is applied to an electron microsystem with one, two or many electrons (a atom,a molecule or a crystal ), admits as a solution the so-called wave function, a function of the spatial coordinates, from which can be calculated the density of probability to find an electron in a generic point of space around nucleous.
Schroedinger's equation admits physically acceptable solutions (eigenfunctions) only for some particular values of energy, the so-called eigenvalues, that coincide, for example in the case of hydrogen atom, with the energetic levels of its only electron.
Likewise, by applying the wave equation to a molecule or to a crystal, it is gotten a wave function (eigenfunction), from which can be calculated the molecular electronic density or the crystalline one.
The quantum mechanics of Schroedinger, said even wave-mechanics, is a complete theory, as it permits to calculate both the energy levels of the electrons in atoms, molecules and crystals, and the probability of transition between two quantum states.
The wave equation can be applied to any elementary particle that is moving in a force field, in particular, around an atomic nucleus, to calculate the energy levels of nucleons, protons and neutrons subjected to the potential energy of the nuclear forces.

HEISENBERG'S UNCERTAINTY PRINCIPLE (1927)

The German physicist Werner Heisenberg (Nobel prize winner 1932 ), independently from Schroedinger's work, formulated the quantum mechanics assuming as a fundamental its uncertainty principle and elaborating a mathematical approach based on the matrixes (the matrix quantum mechanics).
Every observable physical quantity , that is energy, position, momentum, angular momentum , is described by an operator represented as a matrix, with results that are formally analogous to the ones of Schroedinger'equation.
The uncertainty principle, that in the matrix mechanics functions as the wave-like De Broglie hypothesis in Schroedinger's quantum mechanics, affirms that the uncertainties (errors) associated with the simultaneous measure of two complementary physical quantities (position and momentum or energy and time ), are each other inversely proportional:

Dx . Dpx ~= h/(2p) ;
DE . Dt ~= h/(2 p),where h is the Planck constant.
In other words, if by an experiment one determines, for example, the momentum of a particle, with a very small error Dpx , the corresponding error Dx made in the simultaneous measure of the co-ordinate x of the particle is much great, and it is inversely proportional to Dpx.

THE DISCOVERY OF ELECTRON SPIN (1927)

In 1922 the German physicists Stern (Nobel prize winner 1943 ) and Gerlach, while studying the effect of a non-uniform magnetic field on silver atoms, to verify the quantization of the atomic magnetic moment associated with the angular momentum of electrons, they discovered that a well collimated beam of non-ionized Ag atoms, crossing the space between the polar expansions of a magnet, that is shaped in such a mode to get a non-uniform field, to apply to atomic magnetic moments a force instead a torque, is divided in two beams, in such a mode that isn,t foreseen by classical physics, according to which the beam should spread in many elementary beams distributed with continuity in a certain angle, nor by quantum theory, according to which it should spread to form some beams oriented in a discreet number of directions.
The experiment was repeated in 1927 from Phipps and Taylor with non-ionized hydrogen atoms and without a magnetic moment, as they were in the ground state , that is with the least energy and the angular momentum equal to zero, and it was observed even in such conditions the dual splitting of the beam, that couldn't be determined by the magnetic moment associated with the orbital angular moment of the electrons, because it was equal to zero.
The experiment was explained by admitting the existence of an associate magnetic moment to an intrinsic angular momentum of electron, not foreseen by the classical physics nor from the non-relativistic quantum mechanics of Schroedinger.
The intrinsic angular momentum of an electron may be seen as a microscopic spinning top, that takes the name of "spin" .
Electron spin and the one of other particles ( protons, neutrons,etc...
) is a moment of intrinsic rotation which is typical of quantum mechanics and whose existence is able to be justified only within a relativistic quantum theory, as the one elaborated by the English physicist P.A.M. Dirac in 1928.

THE DIFFRACTION EXPERIMENTS WITH ELECTRONS (1927)

The physicists Clinton Davisson and George Thomson (Nobel prize winners in 1937 ), experimenting electron scattering by nickel crystals, were able to get some diffraction figures analogous to that gotten by Laue with X-rays, and got so the first experimental evidence of the validity of the De Broglie wave-like hypothesis .
In some following experiments, performed from other physicists with gold layers and crystals of several types, were gotten some photographic imagines of diffraction rings quite similar to that gotten by using X-rays.
The experiments of Davisson and Thomson confirmed the existence of the wave-particle-like dualism of the matter, besides the one observed for electromagnetic radiation.
Therefore, besides the X-ray diffractometry there is the electron diffractometry, that has today a fundamental importance in the researches on the structure of the matter, that is based on measures of the electronic density in crystals.
We remember that the ion and electron microscopes use the wave-like properties of ions and electrons respectively, to produce diffraction images of biological tissues and various materials.

DIRAC'S RELATIVISTIC QUANTUM MECHANICS AND THE ANTIMATTER HYPOTHESIS ( 1928)

The quantum mechanics ( wavemechanichs ) based on Schroedinger's equation doesn't take account of Einstein's theory of the special relativity, and therefore it cannot explain all the properties of the elementary particles that constitute the matter, when the velocities that are considered, are not negligible in comparison with the ones of light.
For example, any characteristics of the optical and X-ray line-spectra emitted by atoms cannot be explained within the Schroedinger theory , that don't take account of Einstein's space-time and of the transformation rules of the space-time coordinates in the transit from a inertial frame of reference to another one that is moving in comparison with the first with a rectilinear and uniform motion.
A relativistic formulation of quantum mechanics was developed by the English physicist Paul Adrien Maurice Dirac (Nobel prize winner in 1933 ), that wrote a relativistic wave equation that is invariant with respect to the relativistic transformations of the space-time co-ordinates.
The fundamental characteristics of the equation introduced by Dirac consisted in including naturally the spin of the particles, as a direct consequence of the relativistic formalism, and in assigning to a particle two possible values of energy, different only for the sign.
The interpretation proposed by Dirac for the states with a negative energy associated to an elementary particle, it is based on the hypothesis of the existence of the relative antiparticle, that is of an antiparticle having a mass equal to the one of the particle and an electric charge of opposite polarity.
The first experimental evidence of the existence of a particle-antiparticle pair was obtained in the years 1932-33, when Anderson ( Nobel prize winner in 1936 ), Blackett ( Nobel prize winner in 1948 ) and Occhialini, while studying the showers of the secondary particles produced by the cosmic rays in the earth atmosphere, discovered the antiparticle of the electron, the positron or positive electron.
. Some years after ( 1955 ), the Italian physicist Emilio Segrč (Nobel prize winner in 1959), while concluding a series of experiments effected with the cyclotron by 6,2 GeV of the Berkeley University, succeeded in producing antiproton, furnishing a further, bright confirmation of the validity of Dirac's relativistic quantum mechanics.

AN ELEMENTARY PARTICLE SCREENED BY VIRTUAL PARTICLE-ANTIPARTICLE PAIRS

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