in Brussels, a gathering of the world's top physicists. Dirac is in the centre of the middle row, seated behind
Albert Einstein. (front row 4th from left),
Erwin Schrödinger (front row 2nd from right) at
Dublin Institute for Advanced Studies in 1942 Dirac discovered the
relativistic equation for the electron, which now bears his name. The remarkable notion of an antiparticle to each fermion particle – e.g. the positron as antiparticle to the electron – stems from his equation. He is credited as being the one to create
quantum field theory, which underlies all theoretical work on sub-atomic or "elementary" particles today, work that is fundamental to our understanding of the forces of nature, alongside creating quantum electrodynamics and coining the term. Throughout his career, Dirac was motivated by the principles of
mathematical beauty, with
Peter Goddard stating that "Dirac cited mathematical beauty as the ultimate criterion for selecting the way forward in theoretical physics". Dirac was recognised for being mathematically gifted, as during his time in university, academics had affirmed that Dirac had an "ability of the highest order in mathematical physics", with
Ebenezer Cunningham stating that Dirac was "quite the most original student I have met in the subject of mathematical physics". Therefore, Dirac was known for his "astounding physical intuition combined with the ability to invent new mathematics to create new physics". Dirac's attention was drawn to a mysterious mathematical relationship, at first sight unintelligible, that Heisenberg had established. Several weeks later, back in Cambridge, Dirac suddenly recognised that this mathematical form had the same structure as the
Poisson brackets that occur in the
classical dynamics of particle motion. From his new understanding, he developed a quantum theory based on
non-commuting dynamical variables. This led him to the most profound and significant general formulation of quantum mechanics to date. His novel formulation using
Dirac brackets allowed him to obtain the
quantisation rules in a
novel and more illuminating manner. For this work, published in 1926, Dirac received a PhD from Cambridge.
Fermi–Dirac statistics Shortly after
Wolfgang Pauli proposed his
Pauli exclusion principle (that two electrons cannot occupy the same quantum energy level),
Enrico Fermi and Dirac This applies to systems consisting of many identical
spin-1/2 particles, or
fermions (i.e. that obey the Pauli exclusion principle), e.g. electrons in solids and liquids, and importantly to the field of conduction in
semiconductors.
Dirac equation In 1928, building on 2×2 spin matrices which he purported to have discovered independently of
Wolfgang Pauli's work on non-relativistic
spin systems (Dirac told
Abraham Pais, "I believe I got these [matrices] independently of Pauli and possibly Pauli got these independently of me."), he proposed the
Dirac equation as a
relativistic equation of motion for the
wave function of the
electron. This work led Dirac to predict the existence of the
positron, the electron's
antiparticle, which he interpreted in terms of what came to be called the
Dirac sea. The positron was observed by
Carl Anderson in 1932. Dirac's equation also contributed to explaining the origin of
quantum spin as a relativistic phenomenon. The necessity of
fermions (matter) being created and destroyed in
Enrico Fermi's 1934 theory of
beta decay led to a reinterpretation of Dirac's equation as a "classical"
field equation for any
point particle of spin
ħ/2, itself subject to quantisation conditions involving
anti-commutators. Thus reinterpreted, in 1934 by
Werner Heisenberg, as a (quantum) field equation accurately describing all elementary matter particles – today
quarks and
leptons – this
Dirac field equation is as central to theoretical physics as the
Maxwell,
Yang–Mills and
Einstein field equations. Dirac is regarded as the founder of
quantum electrodynamics, being the first to use that term. He also introduced the idea of
vacuum polarisation in the early 1930s. This work was key to the development of quantum mechanics by the next generation of theorists, in particular
Julian Schwinger,
Richard Feynman,
Sin-Itiro Tomonaga and
Freeman Dyson in their formulation of quantum electrodynamics. Dirac's
The Principles of Quantum Mechanics, published in 1930, is a landmark in the
history of science. It quickly became one of the standard textbooks on the subject and is still used today. In that book, Dirac incorporated the previous work of Heisenberg on
matrix mechanics and of
Erwin Schrödinger on
wave mechanics into a single mathematical formalism that associates measurable quantities to operators acting on the
Hilbert space of vectors that describe the state of a
physical system. The book also introduced the
Dirac delta function. Following his 1939 article, he also included the
bra–ket notation in the third edition of his book, thereby contributing to its universal use nowadays.
Quantum electrodynamics Dirac's
quantum electrodynamics (QED) included terms with infinite
self-energy. A workaround known as
renormalisation was developed, but Dirac never accepted this. "I must say that I am very dissatisfied with the situation", he said in 1975, "because this so-called 'good theory' does involve neglecting infinities which appear in its equations, neglecting them in an arbitrary way. This is just not sensible mathematics. Sensible mathematics involves neglecting a quantity when it is small – not neglecting it just because it is infinitely great and you do not want it!" His refusal to accept renormalisation resulted in his work on the subject moving increasingly out of the mainstream.
Shin'ichirō Tomonaga,
Schwinger and
Feynman mastered this approach, producing a QED with unprecedented accuracy, resulting in formal recognition by being awarded the 1965 Nobel Prize in Physics. In the 1950s in his search for a better QED, Paul Dirac developed the Hamiltonian theory of constraints based on lectures that he delivered at the 1949
International Mathematical Congress in Canada. Dirac had also solved the problem of putting the
Schwinger–Tomonaga equation into the Schrödinger representation and given explicit expressions for the
scalar meson field (
spin zero pion or
pseudoscalar meson), the vector meson field (spin one rho meson), and the electromagnetic field (spin one massless boson, photon).
Magnetic monopoles In 1931, Dirac proposed that the existence of a single magnetic monopole in the universe would suffice to explain the quantisation of electrical charge. No such monopole has been detected, despite numerous attempts and preliminary claims. (See also:
Searches for magnetic monopoles.)
War work Dirac contributed to the
Tube Alloys project, the British programme to research and construct atomic bombs during
World War II. Dirac made fundamental contributions to the process of
uranium enrichment and the
gas centrifuge.
Gravity Dirac quantised the gravitational field. In his 1959 lecture at the
Lindau Meetings, Dirac discussed why
gravitational waves have "physical significance". Dirac predicted gravitational waves would have well defined energy density in 1964. Dirac reintroduced the term "
graviton" in a number of lectures in 1959, noting that the energy of the gravitational field should come in quanta.
Cosmology Dirac contributed to
cosmology, putting forth his
large numbers hypothesis.
String theory Dirac is seen as having anticipated
string theory, with his work on the
Dirac membrane and
Dirac–Born–Infeld action, both of which he proposed in a 1962 paper, along with other contributions. He also developed a general theory of the quantum field with dynamical constraints,
Other work Dirac wrote an influential paper in 1933 regarding the
Lagrangian in quantum mechanics. The paper served as the basis for
Julian Schwinger and his
quantum action principle, and laid the foundations for
Richard Feynman's development of a completely new approach to quantum mechanics, the
path integral formulation. In a 1963 paper, Dirac initiated the study of field theory on
anti-de Sitter space (AdS). The paper contains the mathematics of combining special relativity with the quantum mechanics of quarks inside hadrons, and lays the foundations of
two-mode squeezed states that are essential to
modern quantum optics, though Dirac did not realize it at the time. Dirac previously worked on AdS during the 1930s, publishing a paper in 1935. In 1930,
Victor Weisskopf and
Eugene Wigner published their famous and now standard calculation of spontaneous radiation emission in atomic and molecular physics. Remarkably, in a letter to
Niels Bohr in February 1927, Dirac had come to the same calculation, but he did not publish it. In 1938, Dirac renormalized the mass in the theory of Abraham-Lorentz electron, leading to the
Abraham–Lorentz–Dirac force, which is the relativistic-classical electron model; however, this model has solutions that suggest force increase exponentially with time.
Fermi's golden rule, the formula for computing quantum transitions in time dependent systems, declared a "golden rule" by
Enrico Fermi, was derived by Dirac. Dirac was the one to initiate the development of
time-dependent perturbation theory in his early work on semi-classical atoms interacting with an electromagnetic field. Dirac, with
Werner Heisenberg,
John Archibald Wheeler, Richard Feynman, and
Freeman Dyson ultimately developed this concept into an invaluable tool for modern physics, used in the calculation of the properties of any physical system and a wide array of phenomena. == Career ==