or
the anti-conformist force
Described
in 1934 by the italian physicist Enrico Fermi, this interaction
is responsible for Beta radioactivity where a nucleon transforms into another
nucleon, on emitting an electron-antineutrino pair (or their antiparticles).
It is the weak force which maintains ties between these three particles
and it can be attractive in the case where the nucleon remains unchanged
or repulsive in provoking the transmutation between a neutron and a proton.
Lets point out that there exist two distinct varieties of b radioactivity.
To properly understand the effect of these two
distinct radioactivities which transform an atom into another, we take
the example of the radioactive atom Brome-35 which contains 80 nucleons
of which 35 are protons.
This interaction is more discrete than the others; it has an intensity
ten million times smaller than the strong interaction (hence its name weak)
and its range is the shortest of all: it acts at 10-18
metres, that is to say practically at the point of contact between
the two particles.
Yet the weak interaction is fundamental for us because it governs the
thermonuclear reactions of our Sun and of all of the stars: Without it,
no warmth and no life!
It is important to remember that the weak force applies to all fermions, that includes the elusive neutrinos which do not react to any of the other interactions.
The weak interaction is very eccentric because it separates itself from its three sisters on two points:
Intermediary
bosons
In contrast to the other bosons of zero mass, the virtual mediator particules of the weak interaction are around 100 times more massive than the proton! In addition, there are three of them:
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b-radioactivity is therefore explained by the emission of a W- boson by the d quark of a neutron. This d quark then changes flavour and becomes a u quark. The W- boson which is very unstable, materialises rapidly into an electron and an antineutrino. This reaction is illustrated by the following Feynman representation:
These intermediary bosons were discovered in 1983 at CERN in Geneva
by Carlo Rubbia.
Parity
violation
Parity is a "mirror" symmetry which inverts right and left.
Imagine
a spinning top and its image in a mirror: the two corresponding images
have in reality the two possible states; the top can be turning in two
directions.
Similarly, during an electromagnetic interaction, we observe the direction
of diffusion of a charged particle. We notice that this same action "invert
as in a mirror" is possible and realisable; thus electromagnetism is said
to be "invariant by parity".
This invariance also applies to gravitation and the strong interaction.
This symmetry seems evident and common sense: a phenomena seen in the mirror
could exist for real.
What a surprise it was for physicists in 1957 when they noted with astonishment
that the weak interaction violates this parity. Explanation:
The weak interaction can produce disintegrations with the emission
of neutrinos. Now these neutrinos have spin, as if they rotate around themselves.
If they turn anticlockwise, we say that they are "lefts". There should
then also exist a "mirror" reaction which produces "right" neutrinos. But
no! These right neutrinos don't exist and the mechanism at the origin
of this asymmetry remains unknown!
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Particles are great sentimentalists; they never stop succumbing to
4 types of attraction. One must confess that these are physical attractions!
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