Quantum physics 1

or

Light on the photon







Introduction
 

Quantum theory is used by physicists to take account of phenomena which happen at the microsopic scale of particles.

The intrinsic power of this physics is considerable. It has potential to be used by nuclear physicists, atomic physicists, material physicists and even astrophysicist. To date, no experiment has come to contradict its predictions, strange though they are. Quantum physics uses concepts which don't always have a counterpart in daily life, you mustn't be surprised if certain of these predictions run strenuously counter to common sense.

Albert Einstein, for example, never accepted certain consequences of quantum theory: see how he pokes out his tongue!
 


 

Why "quantum"?
 

Quantum physics literally means "the physics of quanta" (= latin plural of "quantum" which means quantity).
This new word appeared in the physics register on the 14th December 1900 thanks to a revolutionary paper read out before the Prussian Academy of Sciences by the german Max Planck: He postulated the original idea according to which, the energy exchanges between light and matter cannot happen except in discrete packets, which he called quanta. He then renounced the sacred law of continuity, the pillar of classical physics.
 


 

What is "classical" and continuous light ?
 

Not so easy to represent such an immaterial concept!
At the end of the XIXth century, James Maxwell defined light as being a beam of electromagnetic waves moving at a constant speed in the vacuum: the famous speed c of 300.000 kilometers per second.
As easy as it is to imagine a wave running across the surface of water and sound as being a vibration in air, the concept of an electromagnetic wave (as being an oscillation of the electric and associated magnetic field) can leave us perplexed. How can we imagine these fields working so intimitely together? What is there to support this oscillation in a vacuum?

Light is always characterised by its frequency or its wavelength. Visible light is in fact nothing but a narrow window on the whole of the spectrum of electromagnetic waves (which also include gamma rays, X rays, ultraviolet, infrared and radio waves).See ( spectrum)
 


 

Photonic and quantic light
 

After Max Planck, this radically new notion of "quantic light" would be taken up in 1905 by Albert Einstein who supported the idea that the energy of light is in some ways "granularised". This "grain of electricity" would be named photon in 1926: A new particle is born, a non-material particle without mass.
Each photon of a radiation (light, radio waves, X rays...) carries a quantum of energy characteristic of its frequency (frequency of visible light = colour).

Quantum physics then associates a wave and a particle. This association would be generalised from this to all particles, and notably the electron.
But how to reconcile a continuum (waves) with the discontinuous (particles)?
This all comes down to the wave-particle duality paradox.
 


 

Wave-particle duality
 

The most important question that quantum physics has been compelling to address, concerns the manner in which to represent physical objects and their properties. The old physics, known as classical, distinguished two types of fundamental entities:

Quantum physics doesn't hold on to this classification, convenient as it is. The objects which it considers are neither particles, nor waves, but "something else".

The following analogy should help us:

Look at a cylinder from two different angles, a cylinder appears sometimes as a circle, sometimes as a rectangle. When in fact it is neither one nor the other.
Thats the way the photon, the electron and all elementary particles are, thus the image of a particle is but one facet of a more complex entity.

This precise point can pose a very troubling philosophical problem: Objective reality (if it exists independantly of the human spirit), is it accessible? Or are we condemned to observe nothing but a world of deceptive appearances?
 


 

Where's light come from?
 

Quantum physics allows us to better understand how light is emitted by matter...
The world of the atom according to Niels Bohr was a model at the frontier of two ages: the classical age, pre-quantum and the quantum world. But it already explained the mechanism of the emission of light by an atom.
 

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This emission is explained then by the jump which an electron makes from an orbit E2 to an orbit E1. During this jump towards this less energetic orbit E1 (an inner orbit), the electron will lose part of its energy in the form of a photon emitted outwards.
 

The energy of this photon, E2 - E1, will be a whole number multiple (the famous quantification of light) of the value hn.





Conversely, an atoms electron could absorb a photon of a given energy and thus jump from a less energetic orbit to a more energetic orbit: It will thus become more excited than normal because it is in a more energetic orbit. It is in becoming less excited that it should subsequently re-emit a photon.

Quantum theory stipulates that not all electronic orbits are allowed. Orbits are not permitted unless, in jumping from one orbit to another, an electron can emit or absorb a photon with an energy which is an exact multiple of the famous value hn. It's this quantic discontinuity of the energy exchange which enforces a disconuity in the orbits which are permitted. Each permitted electronic orbit will therefore be quantified and characterised by the quantum numbers (4 numbers designated n, l, m t s).
For example, the number n is called the principal quantum number. It designates the number of the electron layer also designated by the letters K, L, M, O, P, Q.
 


The visible spectrum
 

Each atom can only emit a precise and characteristic set of colours: Each colour of light is in fact a particular frequency (and therefore a level of energy) of a photon. All of the possible jumps between orbits which an electron can make within a given atom translate into the emission (or absorption) of a characteristic spectrum of light: Here we have a veritable identity card for a given type of atom. It's because of this readily identifiable spectrum that we can know which atoms exist in stars in the firmament. Their light is captured by telescopes, analysed and compared with the spectrums of hydrogen, helium etc...