|
1500 |
Babylonians establish the metric of flat 2-dimensional space
by observation, in their efforts to keep track of land for legal and economic
purposes. |
|
||||
|
-518 |
Pythagoras, a Greek educated by mystics in Egypt and Babylon,
founds community of men and women calling themselves mathematikoi, in
southern Italy. They believe that reality is in essence mathematical.
Pythagoras noted that vibrating lyre strings with harmonious notes have
lengths that are proportional by a whole number. The Pythagorean theorem
proves by reasoning what the Babylonians figured out by measurement 1000
years earlier. |
|
||||
|
-387 |
Plato, after traveling to Italy and learning about the
Pythagoreans, founds his Academy in Athens, and continues to develop the idea
that reality must be expressible in mathematical terms. But Athens at that
time has developed a notoriously misogynist culture. Unlike his role model
Pythagoras, whose school developed many women mathematikoi, Plato does not
allow women to participate. |
|
||||
|
-300 |
Euclid of Alexandria, a gifted teacher, produces Elements, one
of the top mathematics textbooks of recorded history, which organizes the
existing Mediterranean understanding of geometry into a coherent logical
framework. |
|
||||
|
-225 |
Ionian mathematician Apollonius writes Conics, and
introduces the terms ellipse, parabola and hyperbola to describe conic
sections. |
|
||||
|
-140 |
Nicaean mathematician and astronomer Hipparchus develops what
will be known as trigonometry. |
|
||||
|
150 |
The Almagest by Alexandrian astronomer and
mathematician Claudius Ptolemy asserts that the Sun and planets orbit around
the Earth in perfect circles. Ptolemy's work is so influential that will
become official church doctrine when the Christians later come to rule
Europe. |
|
||||
|
415 |
As a glorious 2000 years of ancient Mediterranean mathematics
and science comes to a close, Hypatia of Alexandria, a renowned teacher,
mathematician, astronomer, and priestess of Isis, is kidnapped from a public
religious procession and brutally murdered by a mob of angry Christian monks. |
|
||||
|
628 |
Hindu mathematician-astronomer Brahmagupta writes Brahma-
sphuta- siddhanta (The Opening of the Universe). Hindu mathematicians
develop numerals and start investigating number theory. |
|
||||
|
830 |
The spread of Islam leads to the spread of written Arabic
language. As ancient Greek and Hindu works are translated into Arabic, a
culture of mathematics and astronomy develops. The peak of this cultural
flowering is represented by Arabic mathematician Al-Khworizmi, working at the
House of Wisdom in Baghdad, who develops what will be known as algebra in his
work Hisab al-jabr w'al-muqabala. |
|
||||
|
1070 |
Iranian poet, mathematician and astronomer Omar Khayyam begins
his Treatise on Demonstration of Problems of Algebra, classifying
cubic equations that could be solved by conic sections. Khayyam was such a
brilliant poet that history has nearly forgotten that he was also a brilliant
scientist and mathematician. The moving finger writes... |
|
||||
|
1120 |
Adelard of Bath translates works of Euclid and Al-Khworizmi
into Latin and introduces them to European scholars. |
|
||||
|
1482 |
Euclid's Elements is
published using the revolutionary new technology of the printing press,
leading to a revolution in education and scholarship as information becomes
more difficult for authorities to control. |
|
||||
|
1543 |
Copernicus publishes De revolutionibus orbium coelestium
(On the revolutions of the heavenly spheres) asserting that the Earth and
planets revolve about the Sun. The Catholic Church has accorded an official
holy status to Ptolemy's geocentric Universe. Copernicus avoids prosecution
as a heretic by waiting until the end of his own life to publish his
controversial claims. |
|
||||
|
1589 |
Pisa University mathematics instructor Galileo Galilei studies
the motion of objects and begins a book De Motu (On Motion) which he
never finishes. |
|
||||
|
1602 |
Galileo observes that the period of a swinging pendulum is
independent of the amplitude of the swing. |
|
||||
|
1609 |
Johannes Kepler claims in the journal Astronomia Nova
that the orbit of Mars is an ellipse with the Sun at one focus, and sweeps
out equal areas in equal time. He will later generalize these into his famous
Three Laws of Planetary Motion. |
|
||||
|
1609 |
Galileo makes his first telescope. His observations of the
moon show that it looks like a very large lumpy rock, not a divinely smooth
and perfect shining Platonic heavenly orb. This discovery has enormously
distressing cultural reverberations for Western culture and religion. |
|
||||
|
1614 |
Scottish theologian John Napier, who does mathematics as a
hobby, publishes his discovery of the logarithm in his work Mirifici
logarithmorum canonis descriptio. |
|
||||
|
1615 |
Kepler's mother, Frau Katharina Kepler, is accused of witchcraft
by a local prostitute. European witch hunting was at its peak during Kepler's
career, and witch hunting was supported by all levels of society, including
secular officials and intellectuals in universities. Kepler spends the next
several years making legal appeals and hiding his mother from legal
authorities seeking to torture her into confessing to witchcraft. Examining
an accused witch ad torturam was a standard court procedure
during this era. |
|
||||
|
1620 |
Under court order, Kepler's mother is kidnapped in the middle
of the night from her daughter's home and taken to prison. Kepler spends the
next year appealing to the duke of Württemberg to prevent his imprisoned
mother from being examined ad torturam. |
|
||||
|
1621 |
On September 28, Katharina Kepler is taken from her prison
cell into the torture room, shown the instruments of torture and ordered to
confess. She replies "Do with me what you want. Even if you were to
pull one vein after another out of my body, I would have nothing to
admit," and says the Lord's Prayer. She is taken back to prison. She
is freed on October 4 upon order of the duke, who rules that her refusal to
confess under threat of torture proves her innocence. He also orders her
accusers to pay the cost of her trial and imprisonment. |
|
||||
|
1622 |
After having spent most of the last seven years under the
legal threat of imminent torture, Katharina Kepler dies on April 13, still
being threatened with violence from those who insist she is a witch. |
|
||||
|
1624 |
Pope Urban VIII promises Galileo that he is allowed write
about Copernican heliocentrism if he treats it as an abstract proposition. |
|
||||
|
1628 |
Kepler uses Napier's logarithms to compute a set of
astronomical tables, the Rudolphine Tables, whose accuracy is so
impressive that it leads to the quiet acceptance of the heliocentric solar
system by everyone in the shipping industry. |
|
||||
|
1629 |
Basque mathematician Pierre de Fermat, the founder of modern
number theory, begins his brilliant career by reconstructing the work of
Apollonius on conic sections . Fermat and Descartes pioneer the application
of algebraic methods to solving problems in geometry. |
|
||||
|
1632 |
Galileo publishes Dialogue concerning the two greatest
world systems, which argues convincingly for the Copernican view that the
Earth and planets revolve around the Sun. |
|
||||
|
1633 |
The Inquisition calls Galieo to Rome to answer charges of
heresy against the Catholic Church. |
|
||||
|
1637 |
Descartes publishes his revolutionary Discours de la
méthode (Discourse on Method) containing three essays on the use of
reason to search for the truth. In the third essay Descartes describes
analytic geometry, and uses the letters (x,y,z) for the coordinate system
that will later bear his name. |
|
||||
|
1642 |
Galileo dies at his villa in Florence, still under house
arrest from charges of heresy. |
|
||||
|
1663 |
Cambridge mathematician Isaac Barrow delivers lectures on
modern methods of computing tangents that inspire his student Isaac Newton
towards developing calculus |
|
||||
|
1665 |
Newton's "miraculous years" in math and physics,
when he discovers the derivative, which he sees as a ratio of velocities
called fluxions, and the integral, which he sees as a fluent of
the fluxions. Newton shows that the fluent and fluxion are inversely
related, a result now called the Fundamental Theorem of Calculus.
Newton also develops his ideas on optics and gravitation. He tries to publish
his work in 1671, but the publisher goes bankrupt. |
|
||||
|
1683 |
Jacob Bernoulli, who studied mathematics and astronomy against
the wishes of his career-minded parents, teaches Newtonian mechanics at the
University of Basel, and turns mathematical physics into a family business. |
|
||||
|
1684 |
Leibniz publishes the beginning of his work on differential
and integral calculus. He discovers the Fundamental Theorem of Calculus in
his own way. Leibniz originates most of the current calculus notation
including the integral sign. He portrays an integral as a sum of
infinitesimals, a concept rejected by Newton. |
|
||||
|
1687 |
Newton publishes Principia Mechanica after Edmund
Halley convinces Newton to write up his alleged proof that an inverse square
force law leads to elliptical orbits. Newton's Laws of Motion and Law of
Gravitation lead to the development of theoretical physics itself. This event
marks a permanent change in the relationship between human beings and the
Universe. |
|
||||
|
1693 |
Newton has a nervous breakdown after his close companion Fatio
De Duillier becomes ill and has to return to Switzerland. |
|
||||
|
1696 |
Brachistochrone
problem solved by Jacob and Johann Bernoulli, an early result in the calculus
of variations. |
|
||||
|
1712 |
Thanks to a campaign waged by Newton, a commission appointed
by Royal Society of London President Isaac Newton rules that Leibniz is
guilty of plagiarism against Newton in the discovery of calculus. English
mathematics and theoretical physics go into decline because those loyal to
Newton are hesitant to adopt Leibniz' infinitesimal and his clean,
intuitively appealing notation. |
|
||||
|
1736 |
Leonhard Euler begins the field of topology when he publishes
his solution of the Konigsberg Bridge problem. |
|
||||
|
1738 |
Hydrodynamics by Daniel Bernoulli |
|
||||
|
1748 |
The multitalented Euler begins the fields of mathematical
analysis and analytical mechanics with Introductio in analysin infinitorum.
Euler introduces the formula eix = cos x + i sin x |
|
||||
|
1758 |
Joseph-Louis Lagrange finds the complete general solution to
the Newtonian equations of motion for a vibrating string, which explains the
harmonic relations observed by Pythagoras 22 centuries ago. |
|
||||
|
1770 |
Hyperbolic trigonometry -- cosh, sinh -- is developed. |
|
||||
|
1772 |
Henry Cavendish, a wealthy but paranoid recluse, discovers
that the electrostatic force is described by an inverse square law similar to
gravity, but doesn't tell anyone in the science community. |
|
||||
|
1788 |
Lagrange further develops the analytical mechanics of Euler
when he publishes Mécanique Analytique, revealing Newtonian mechanics
to be a rich field of exploration for mathematicians. |
|
||||
|
1789 |
Aristocrat Charles-Augustin de Coulomb, hiding from the French
Revolution after the storming of the Bastille, shows that the electrostatic
force between electric charges was very well described by an inverse square
law, in full analogy with Newtonian gravity. This becomes known as Coulomb's
Law, even though Henry Cavendish was the first one to demonstrate it. |
|
||||
|
1793 |
Lagrange is arrested during the Reign of Terror, but is
rescued by Antoine-Laurent Lavoisier, the founder of modern chemistry.
Unfortunately, Lavoisier's career in chemistry is ended when he is taken to meet
Madame Guillotine on May 8, 1794. |
|
||||
|
1799 |
Pierre-Simon Laplace publishes his work Traité du Mécanique
Céleste (Treatise on Celestial Mechanics) using differential equations to
solve problems in planetary motion and fluid flow. |
|
||||
|
1807 |
After serving as a member of the Revolutionary Committee that
terrorized France, sent Coulomb into hiding, arrested Lagrange and
guillotined Lavoisier, a repentant Jean Baptiste Joseph Fourier causes
controversy with his memoir On the Propagation of Heat in Solid Bodies.
His former teachers Laplace and Lagrange object to his use of infinite
trigonometric series, which we now call Fourier series. Fourier later wins
the Paris Institute Mathematics Prize for solving the problem of heat
propagation, over the repeated objections of Laplace and Lagrange. |
|
|||
|
1817 |
Johann Karl Friedrich Gauss begins working on non-Euclidean
geometry, and lays the foundations of differential geometry, but doesn't
publish because he is afraid of the controversy that would result. |
|
|||
|
1820 |
Danish physicist Hans Christian Oersted studied the way an
electric current in a wire could move the magnetic needle of a compass, which
strongly suggested that electricity and magnetism were related somehow. |
|
|||
|
1823 |
Transylvanian mathematician János Bolyai, despite being warned
against it by his father, tosses out Euclid's Fifth Axiom and shows that
non-Euclidean geometry is possible. Gauss calls him a genius of the first
order, but then crushes the young man by telling him he discovered it years
ago but failed to publish due to his own fear of controversy. |
|
|||
|
1826 |
Elliptic functions are developed by Gauss, Jacobi and Abel. |
|
|||
|
1826 |
In his book Memoir on the Mathematical Theory of
Electrodynamic Phenomena, Uniquely Deduced from Experience. André Marie
Ampère gave a mathematical derivation of the magnetic force between two
parallel wires with electric current, what we now call Ampère's Law. |
|
|||
|
1827 |
Ohm's Law of electrical resistance is published in his book Die
galvanische Kette, mathematisch bearbeitet. |
|
|||
|
1827 |
Augustin-Louis Cauchy develops the calculus of residues,
beginning his work in mathematics that made complex analysis one of the most
important analytical tools of modern theoretical physics, including string
theory. |
|
|||
|
1828 |
Self-educated English mill worker George Green publishes his
work on the use of potential theory to solve partial differential equations,
and develops one of the most powerful mathematical technologies in
theoretical physics -- the Green function. |
|
|||
|
1829 |
Russian mathematician Nikolai Ivanovich Lobachevsky publishes
his independent discovery of non-Euclidean geometry in the Kazan Messenger.
Years later, one of his physics students will become known to history as
Lenin's father. |
|
|||
|
1831 |
Evariste Galois develops the nascent group theory with his
work on the permutation group. |
|
|||
|
1831 |
Michael Faraday discovers magnetic induction, now known as
Faraday's Law, where moving magnetism creates electricity, and this result
increases support for the idea of a unified theory of electricity and
magnetism. |
|
|||
|
1829 |
French mathematician Joseph Liouville begins to work on
boundary value problems in partial differential equations, leading to
Sturm-Liouville theory. He then develops the study of conformal
transformations, and later proves the Liouville Theorem regarding the
invariance of the measure of phase space under what will later be called
Hamiltonian flow. |
|
|||
|
1834 |
William Rowan Hamilton applies his mathematical development of
characteristic functions in optics to mechanics and the enormous and potent
mathematical technology of Hamiltonian dynamics is born. |
|
|||
|
1840 |
Karl Weierstrass begins his work on elliptic functions. |
|
|||
|
1843 |
After a period of emotional distress and alcohol abuse,
Hamilton finally deduces the noncommutative multiplication rule for
quaternions. His first publication on the subject is to carve the quaternion
formula into a bridge. |
|
|||
|
1844 |
Hermann Grassmann develops exterior algebra and the
Grassmannian. |
|
|||
|
1851 |
Bernhard Riemann submits his Ph.D. thesis to his supervisor
Gauss. In his thesis he describes what is now called a Riemann surface, an
essential element in understanding string theory. |
|
|||
|
1854 |
George Boole develops Boolean logic in Laws of Thought. |
|
|||
|
1871 |
Norwegian mathematician Marius Sophus Lie publishes work on
Lie algebras, opening up the field of differential topology and paving the
way for gauge field theory 100 years later. |
|
|||
|
1873 |
James
Clerk Maxwell publishes a set of equations from which all of the observed
laws of electromagnetism could be derived through mathematics. These
equations turn out to have solutions that describe waves traveling through
space with a speed that agrees with the measured speed of light. |
|
|||
|
1874 |
Cantor invents set theory. |
|
|||
|
1878 |
William Clifford develops Clifford algebras from the work of
Grassmann and Hamilton. |
|
|||
|
1878 |
Arthur Cayley writes The theory of groups, where he
proved that every finite group can be represented as a group of permutations. |
|
|||
|
1883 |
Wilhelm Killing works on n-dimensional non-Euclidean geometry
and Lie algebras, work that later results in the concept of a Killing vector,
a powerful tool in differential geometry, quantum gauge field theory,
supergravity and and string theory. |
|
|||
|
1884 |
Heinrich Hertz rewrites Maxwell's Equations in a more
elegant notation where the symmetry between electricity and magnetism was
obvious. Hertz then creats the first radio waves and microwaves in his
laboratory and shows that these electromagnetic waves behaved just as
observable optical light behaved, proving that light was electromagnetic
radiation, as Maxwell had predicted. |
|
|||
|
1884 |
Ludwig Boltzmann makes a theoretical derivation of black body
radiation using Maxwell's equations and thermodynamics, confirming the 1879
result measured experimentally by Josef Stefan. Their result, the
Stefan-Boltzmann Law, is not quite right, and the correct solution in the
next century will mark the beginning of quantum theory. |
|
|||
|
1887 |
Michelson and Morley measure the Earth's velocity through the
ether to be zero, strongly suggesting that there is no ether, and that the
velocity of light is the same for all observers, a result whose full
implications have changed the world forever. |
|
|||
|
1894 |
Elie Cartan classifies simple Lie algebras |
|
|||
|
1895 |
Henri Poincaré publishes Analysis Situs, and gives
birth to the field of algebraic topology. |
|
|||
|
1897 |
Electron discovered by J.J. Thompson. |
|
|||
|
1899 |
Hendrik Lorentz becomes the third person, after Voigt and
FitzGerald, to write down the relativistic coordinate transformations that
will bear his name. The Lorentz transformations leave the speed of light invariant,
as suggested by the Michelson-Morley experiment. |
|
|||
|
1899 |
David Hilbert's Grundlagen der Geometrie (Foundations
of Geometry) is published, putting modern geometry on a solid rigorous
foundation. |
|
|||
|
Max Planck makes his quantum hypothesis -- that energy
is carried by indistinguishable units called quanta, rather than
flowing in a pure continuum. This hypothesis leads to a successful derivation
of the black body radiation law, now called Planck's Law, although in 1901
the quantum hypothesis as yet had no experimental support. The unit of
quantum action is now called Planck's constant. |
|
||||
|
1905 |
Swiss patent clerk Albert Einstein proposes Planck's quantum
hypothesis as the physics underlying the photoelectric effect. Planck wins
the Nobel Prize in 1918, and Einstein in 1921, for developing quantum theory,
one of the two most important developments in 20th century physics. |
||||
|
1905 |
Einstein publishes his simple, elegant Special Theory of
Relativity, making mincemeat of his competition by relying on only two ideas:
1. The laws of physics are the same in all inertial frames, and 2. The speed
of light is the same for all inertial observers. |
||||
|
1905 |
Poincaré shows that Lorentz transformations in space and time
plus rotations in space form a group, which comes to be known as the Lorentz
group. The Lorentz group plus translations in space form a group called the
Poincaré group. |
||||
|
1907 |
Minkowski publishes Raum und Zeit (Space and Time), and
establishes the idea of a spacetime continuum |
||||
|
1909 |
Hilbert's work on integral equations later leads to the
concept of a Hilbert space in quantum mechanics |
||||
|
1915 |
Emmy Noether publishes Noether's Theorem, discovering
the relationship between symmetries and conserved currents that was crucial
to the later development of quantum gauge field theory and string theory |
||||
|
1915 |
Einstein, with Hilbert in stiff competition, publishes his
stunning General Theory of Relativity, and is lucky enough to be able to find
observational support for his theory right away, in the perihelial advance of
Mercury, and the deflection of starlight by the Sun. |
||||
|
1916 |
German astrophysicist Karl Schwarzschild, serving on the
Russian front in WWI, mails Einstein his paper on the Schwarzschild metric
and Einstein presents it at a meeting of the Prussian Academy of Sciences.
Six months and another major paper later, Schwarzschild dies of illness on
the front. |
||||
|
1921 |
Theodor Kaluza follows Einstein's advice and publishes his
highly unorthodox ideas about unifying gravity with electromagnetism by
adding an extra dimension of space that is compactified into a small circle.
Kaluza-Klein compactification will become a rich subject of exploration in
particle theory 60 years later. |
||||
|
1925 |
Werner Heisenberg shows that his quantized probability
operators form a non-commutative algebra. Born and Jordan point out to him
that this is a matrix algebra, and the matrix formulation of quantum
mechanics is born. He gets the Nobel Prize in 1932. |
||||
|
1924 |
Louis duc de Broglie proposes the particle-wave duality of the
electron in his doctoral thesis at the Sorbonne. He gets the Nobel Prize in
1929. |
||||
|
1926 |
After learning of the work of de Broglie, Erwin Schrödinger
develops his wave equation version of quantum mechanics, and unravels its
relationship to the matrix formulation of quantum mechanics by Heisenberg. He
shares the Nobel Prize with Dirac in 1933. |
||||
|
1926 |
Young Cambridge math student Paul Dirac discovers the operator
algebra behind Heisenberg's Uncertainty Principle for his doctoral thesis. |
||||
|
1927 |
Heisenberg discovers the Uncertainty Principle that bears his
name. |
||||
|
1928 |
Dirac introduces a relativistic quantum equation for the
electron, an equation now known as the Dirac equation. His equation
predicts the discovery of the positron, and he shares the Nobel Prize with
Schrodinger in 1933. |
||||
|
1928 |
Werner Heisenberg, Hermann Weyl and Eugene Wigner begin an
exploration of symmetry groups in quantum mechanics that has far-reaching
consequences. |
||||
|
1929 |
Edwin Hubble, with the help of his mule driver Humason,
observes the redshift of distant galaxies and concludes that the Universe is
expanding. |
||||
|
1931 |
Einstein stops using the cosmological constant to keep the
Universe from expanding. |
||||
|
1931 |
Dirac shows that the existence of magnetic monopoles would
lead to electric charge quantization. |
||||
|
1931 |
Georges De Rham goes to work on his famous theorem in
cohomology and characteristic classes, results that would become very
important in string theory. |
||||
|
1935 |
Young physicist Subramahnyan Chandrasekhar is attacked by
famous astronomer Arthur Eddington for his report that there is a stellar
mass limit beyond which collapse to what we now call a black hole is
inevitable. Chandrasekhar wins the Nobel Prize in 1983 for his work on
stellar evolution. |
||||
|
1938 |
Wigner constructs a class of irreducible unitary
representations of the Lorentz group |
||||
|
1939 |
Elements de Mathematique, by Nicholas Bourbaki, pseudonym
for a group of young mathematicians at the Ecole Normale in Paris, is begun.
This extended set of works aims to set down in writing what is no longer in
doubt, but rather on a boring and rigorous footing, in modern mathematics. |
||||
|
1943 |
Chinese mathematician Shiing-Shen Chern begins his work on
characteristic classes and fiber bundles that will become an important tool
for understanding quantum gauge theories and string theory. |
||||
|
1948 |
Richard Feynman, Julian Schwinger and Tomonaga Shin'ichiro
report that the divergent integrals that plague the quantum gauge field
theory of electrodynamics (QED) can be sensibly dealt with through the
process of renormalization. |
||||
|
1953 |
Based on particle scattering data, Murray Gell-Mann suggests
that there is a new quantum number, called hypercharge, which we now call
stangeness and recognize as a part of the quark model coming from the strange
quark. Gell-Mann receives the Nobel Prize in 1969 for his work on the quark
model. |
||||
|
1954 |
Gell-Mann and Francis Low develop the idea that the physical
content of a quantum theory should be invariant under a change of scale in
the theory. This is called renormalization group, and it turns out to
constrain quantum field theories enough to make it a very powerful tool for
analyzing asymptotic behavior of quantum theories. |
||||
|
1954 |
C.N. Yang and R. Mills develop non-Abelian gauge invariance,
an idea that takes 17 years to gain acceptance, and then revolutionizes
particle physics. |
||||
|
1954 |
Eugenio
Calabi conjectures the existence of a Kähler manifold with a Ricci-flat
metric with a vanishing first Chern class, and a given complex structure and
Kähler class. This funny-sounding stuff will eventually become of major
importance in understanding superstring theory. |
||||
|
1964 |
Cambridge mathematician Roger Penrose proves that a black hole
spacetime must contain behind the black hole event horizon a singularity
where spacetime physics ceases to make good sense. |
||||
|
1964 |
Gell-Mann and George Zweig independently propose fundamental
particles that Gell-Mann succeeds in naming "quarks". |
||||
|
1964 |
Peter Higgs, Francois Englert and R. Brout suggest a method of
breaking quantum gauge symmetry that is later called the Higgs mechanism. |
||||
|
1967 |
In his paper A Model of Leptons, Steven Weinberg relies
on Lie group theory combined with quantum field theory to explain the weak
nuclear and electromagnetic forces in a single theory, using the Higgs
mechanism to give mass to the weak bosons. Adbus Salam and Sheldon Glashow
share the Nobel Prize with Weinberg in 1979 for Electroweak Theory. |
||||
|
1967 |
Sidney Coleman and Jeffrey Mandula prove that well-behaved
particle scattering theories can't have symmetry algebras that relate
particles of different spin. But the strict consequences of the
Coleman-Mandula Theorem were avoided by the supersymmetry algebras that were
discovered a few years later. |
||||
|
1968 |
Michael Atiyah and Isadore Singer begin their work on The
Index of Elliptic Operators. They prove the Atiyah-Singer index theorem,
a powerful mathematical result that will later be used extensively in
theoretical physics. |
||||
|
1968 |
Gabriele Veneziano begins modern string theory with his paper
on the dual resonance model of the strong interactions. |
||||
|
1970 |
Yoichiro Nambu, Leonard Susskind, and Holger Nielsen
independently discover that the dual resonance model devised by Veneziano is
based on the quantum mechanics of relativistic vibrating strings, and string
theory begins. |
||||
|
1971 |
Gerard 't Hooft publishes his proof that the electroweak gauge
theory of Weinberg is renormalizable and a new chapter in theoretical physics
begins -- the age of quantum gauge field theory. |
||||
|
1971 |
Pierre Ramond, André Neveu and John Schwarz develop a string
theory with fermions and bosons. Gervais and Sakita show that this theory
obeys what turns out to be a supersymmetry algebra in two dimensions. |
||||
|
1971 |
Ken Wilson publishes work using the renormalization group to
understand the quantum behavior of systems undergoing phase transitions, this
opens up the study of critical phenomena in particle physics and leads to
greater understading of quark confinement. Wilson wins the Nobel Prize in
1981. |
||||
|
1971 |
Soviet physicists Yuri Gol'fand and E. Likhtman extend the
Poincaré algebra into a superalgebra and discover supersymmetry in four
spacetime dimensions. |
||||
|
1973 |
David Gross, David Politzer, Frank Wilczek and Gerard 't Hooft
arrive at the conclusion that the coupling constant in non-abelian quantum
gauge theories vanishes at high energy. This is called asymptotic freedom and
is one of the major results in the history of quantum gauge field theory. |
||||
|
1973 |
Quantum field theories with spacetime supersymmetry in four
spacetime dimensions are discovered by Julius Wess and Bruno Zumino. |
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|
1974 |
Stephen Hawking combines quantum field theory with classical
general relativity and predicts that black holes radiate through particle
emission, behave as thermodynamic objects, and decay with a finite lifetime
into objects that we don't yet understand. |
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|
1974 |
Magnetic monopole solutions of non-Abelian gauge field
theories are found separately by 't Hooft and Moscow physicist Alexander
Polyakov. |
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|
1974 |
Joel Scherk and John Schwarz propose string theory as a theory
of quantum gravity, an idea that takes ten years to be widely appreciated. |
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|
1974 |
Howard Georgi and Sheldon Glashow propose SU(5) for a
"Grand Unified Theory" (GUT) of all forces except gravity, the
theory predicts that protons could decay. |
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|
1975 |
Instanton solutions of Yang-Mills equations are discovered by
Belavin, Polyakov, A. Schwarz and Tyupkin. This is exciting because
instantons can tell us about non-perturbative physics that is not
approachable by other means of calculation. |
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|
1976 |
Shing-Tung Yau proves the Calabi conjecture and discovers the
Calabi-Yau space, an important development for later progress in string
theory. |
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|
1980 |
Alan Guth puts forward the idea of an inflationary phase of
the early Universe, before the Big Bang. |
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|
1981 |
Michael Green and John Schwarz develop superstring theory. |
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|
1981 |
After Schoen and Yau do it in a more traditional manner, Ed
Witten uses supersymmetry to prove the positive mass conjecture. |
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|
1982 |
Mathematician Karen Uhlenbeck shows that Yang-Mills instantons
discovered by physicists can be used as a powerful analytical tool in
abstract mathematics. |
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|
1983 |
Witten and Luis Alvarez-Gaumé derive general formulas for
gauge and gravitational anomalies in quantum field theories in any dimension.
They show that the gravitational anomalies cancel in type IIB superstring
theory. |
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|
1983 |
Mathematics graduate student Simon Donaldson discovers exotic
4-manifolds, using instanton techniques learned in part from Uhlenbeck. |
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|
1984 |
Michael Green and John Schwarz show that superstring theory is
free from quantum anomalies if the spacetime dimension is 10 and the quantum
gauge symmetry is SO(32) or E8 times E8. |
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|
1984 |
Gross, Harvey, Martinec and Rohm find another class of
anomaly-free superstring theories, and call it the heterotic string theory. |
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|
1985 |
Candelas, Strominger, Horowitz and Witten propose the use of
Calabi-Yau spaces for the extra dimensions in heterotic string theory. |
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|
1991 |
Connes and Lott develop non-commutative geometry, which will
find its way into the heart of string theorists at the turn of the
millennium. |
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|
1993 |
In search of an understanding of black hole entropy, 't Hooft suggests the idea that the
information in a 3+1-dimensional system cannot be greater than what is need
to store it as an image in 2+1 dimensions. Susskind generalizes this idea and
applies it to string theory in his paper The World as a Hologram, and the Holographic
Principle is born. |
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|
1994 |
Nathan Seiberg and Ed Witten discover
electric-magnetic duality in N=2 supersymmetric gauge theory in four
spacetime dimensions, with very important applications in both mathematics
and string theory. |
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|
1995 |
Witten and Townsend introduce the idea of Type IIA
superstring theory as a special limit of 11-dimensional supergravity theory with
quantized membranes. This begins the M-theory revolution in superstring
theory, and leads people to ponder the role of spacetime in string theory. |
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|
1995 |
Andrew Wiles, with help from Richard Taylor, completes a
rigorous proof of Fermat's Last Theorem. |
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|
1995 |
Joseph Polchinski ignites the D-brane
revolution in string theory with his paper describing extended objects in
string theory formed by dual open strings with Dirichlet boundary conditions. |
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|
1996 |
In their paper Microscopic Origin of Black Hole
Entropy, Andy Strominger and Cumrun Vafa use D-branes to count the
quantum states of an extreme black hole and their result matches the
Bekenstein-Hawking value. This stimulates new respect for string theory from
the relativity community. |
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|
1997 |
Juan Maldacena finds that string theory in a
background of five-dimensional anti-de Sitter space times a five-sphere obeys
a duality relationship with superconformal field theory in four spacetime
dimensions. The result, called AdS-CFT duality, opens up a new era of exploration
in string theory. |
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|
Here is a
very brief outline of the development of string theory, the details of which
will eventually fill many large volumes written by many people directly and
indirectly involved in this rich and fascinating story. |
|
|
1921 |
|
|
|
Electromagnetism can be derived from gravity in a unified
theory if there are four space dimensions instead of three, and the fourth is
curled into a tiny circle. Kaluza and Klein made this discovery independently
of each other. |
|
1970 |
|
|
|
Three particle theorists independently realize that the dual
theories developed in 1968 to describe the particle spectrum also describe
the quantum mechanics of oscillating strings. This marks the official birth
of string theory. |
|
1971 |
|
|
|
Supersymmetry is invented in two contexts at once: in ordinary
particle field theory and as a consequence of introducing fermions into
string theory. It holds the promise of resolving many problems in particle
theory, but requires equal numbers of fermions and bosons, so it cannot be an
exact symmetry of Nature. |
|
1974 |
|
|
|
String theory using closed strings fails to describe hadronic
physics because the spin 2 excitation has zero mass. Oops, that makes it an
ideal candidate for the missing theory of quantum gravity!! This marks the
advent of string theory as a proposed unified theory of all four observed
forces in Nature. |
|
1976 |
|
|
|
Supersymmetry is added to gravity, making supergravity. This
progress is especially important to string theory, where gravity can't be
separated from the spectrum of excitations. |
|
1980 |
|
|
|
String theory plus supersymmetry yields an excitation spectrum
that has equal numbers of fermions and bosons, showing that string theory can
be made totally supersymmetric. The resulting objects are called
superstrings. |
|
1984 |
|
|
|
This was the year for string theory! Deadly anomalies that
threatened to make the theory senseless were discovered to cancel each other
when the underlying symmetries in the theory belong two special groups.
Finally string theory is accepted by the mainstream physics community as an
actual candidate theory uniting quantum mechanics, particle physics and
gravity. |
|
1991- |
|
|
|
Interesting work on stringy black holes in higher dimensions
leads to a revolution in understanding how different versions of string
theory are related through duality transformations. This unlocks a surge of
progress towards a deeper nonperturbative picture of string theory. |
|
1996 |
|
|
|
Using Einstein relativity and Hawking radiation, there were
hints in the past that black holes have thermodynamic properties that need to
be understood microscopically. A microscopic origin for black hole
thermodynamics is finally achieved in string theory. String theory sheds
amazing light on the entire perplexing subject of black hole quantum
mechanics. |