HENRI_POINCARé

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'Jules Henri Poincaré' (April 29, 1854July 17, 1912) (IPA: [][1]) was one of France's greatest mathematicians and theoretical physicists, and a philosopher of science. Poincaré is often described as a polymath, and in mathematics as ''The Last Universalist'', since he excelled in all fields of the discipline as it existed during his lifetime.
As a mathematician and physicist, he made many original fundamental contributions to pure and applied mathematics, mathematical physics, and celestial mechanics. He was responsible for formulating the Poincaré conjecture, one of the most famous problems in mathematics. In his research on the three-body problem, Poincaré became the first person to discover a chaotic deterministic system which laid the foundations of modern chaos theory. He is considered to be one of the founders of the field of topology.
Poincaré introduced the modern principle of relativity and was the first to present the Lorentz transformations in their modern symmetrical form. Poincaré discovered the remaining relativistic velocity transformations and recorded them in a letter to Lorentz in 1905. Thus he obtained perfect invariance of all of Maxwell's equations, the final step in the formulation of the theory of special relativity.
The Poincaré group used in physics and mathematics was named after him.

Contents
Life
Education
Career
Work
The three-body problem
Work on relativity
Local time
Inertia of energy
Lorentz transformation
Assessments
Character
Toulouse' characterization
Shortcomings
Honors
Publications
Philosophy
See also
Notes
References
Footnotes
General references
References to work on relativity
External links

Life


Poincaré was born on April 29, 1854 in Cité Ducale neighborhood, Nancy, France into an influential family (Belliver, 1956). His father Leon Poincaré (1828-1892) was a professor of medicine at the University of Nancy (Sagaret, 1911). His adored younger sister Aline married the spiritual philosopher Emile Boutroux. Another notable member of Jules' family was his cousin, Raymond, who would become the President of France, 1913 to 1920, and a fellow member of the Académie française.[2]
Education

During his childhood he was seriously ill for a time with diphtheria and received special instruction from his gifted mother, Eugénie Launois (1830-1897).
In 1862 Henri entered the Lycée in Nancy (now renamed the Lycée Henri Poincaré in his honour, along with the University of Nancy). He spent eleven years at the Lycée and during this time he proved to be one of the top students in every topic he studied. He excelled in written composition. His mathematics teacher described him as a "monster of mathematics" and he won first prizes in the concours général, a competition between the top pupils from all the Lycées across France. (His poorest subjects were music and physical education, where he was described as "average at best" (O'Connor et al., 2002). However, poor eyesight and a tendency towards absentmindedness may explain these difficulties (Carl, 1968). He graduated from the Lycée in 1871 with a Bachelor's degree in letters and sciences.
During the Franco-Prussian War of 1870 he served alongside his father in the Ambulance Corps.
Poincaré entered the École Polytechnique in 1873. There he studied mathematics as a student of Charles Hermite, continuing to excel and publishing his first paper (''Démonstration nouvelle des propriétés de l'indicatrice d'une surface'') in 1874. He graduated in 1875 or 1876. He went on to study at the École des Mines, continuing to study mathematics in addition to the mining engineering syllabus and received the degree of ordinary engineer in March 1879.
As a graduate of the École des Mines he joined the Corps des Mines as an inspector for the Vesoul region in northeast France. He was on the scene of a mining disaster at Magny in August 1879 in which 18 miners died. He carried out the official investigation into the accident in a characteristically thorough and humane way.
At the same time, Poincaré was preparing for his doctorate in sciences in mathematics under the supervision of Charles Hermite. His doctoral thesis was in the field of differential equations. Poincaré devised a new way of studying the properties of these equations. He not only faced the question of determining the integral of such equations, but also was the first person to study their general geometric properties. He realised that they could be used to model the behaviour of multiple bodies in free motion within the solar system. Poincaré graduated from the University of Paris in 1879.
The young Henri Poincaré

Career

Soon after, he was offered a post as junior lecturer in mathematics at Caen University, but he never fully abandoned his mining career to mathematics. He worked at the Ministry of Public Services as an engineer in charge of northern railway development from 1881 to 1885. He eventually became chief engineer of the Corps de Mines in 1893 and inspector general in 1910.
Beginning in 1881 and for the rest of his career, he taught at the University of Paris (the Sorbonne). He was initially appointed as the ''maître de conférences d'analyse'' (associate professor of analysis) (Sageret, 1911). Eventually, he held the chairs of Physical and Experimental Mechanics, Mathematical Physics and Theory of Probability, and Celestial Mechanics and Astronomy.
Also in that same year, Poincaré married Miss Poulain d'Andecy. Together they had four children: Jeanne (born 1887), Yvonne (born 1889), Henriette (born 1891), and Léon (born 1893).
In 1887, at the young age of 32, Poincaré was elected to the French Academy of Sciences. He became its president in 1906, and was elected to the Académie française in 1909.
In 1887 he won Oscar II, King of Sweden's mathematical competition for a resolution of the three-body problem concerning the free motion of multiple orbiting bodies. (See #The three-body problem section below)
In 1893 Poincaré joined the French Bureau des Longitudes, which engaged him in the synchronization of time around the world. In 1897 Poincaré backed an unsuccessful proposal for the decimalization of circular measure, and hence time and longitude (see Galison 2003). It was this post which led him to consider the question of establishing international time zones and the synchronization of time between bodies in relative motion. (See #Work on Relativity section below)
In 1899, and again more successfully in 1904, he intervened in the trials of Alfred Dreyfus. He attacked the spurious scientific claims of some of the evidence brought against Dreyfus, who was a Jewish officer in the French army charged with treason by anti-Semitic colleagues.
In 1912 Poincaré underwent surgery for a prostate problem and subsequently died from an embolism on July 17, 1912, in Paris. He was aged 58. He is buried in the Poincaré family vault in the Cemetery of Montparnasse, Paris.
The French Minister of Education, Claude Allegre, has recently (2004) proposed that Poincaré be reburied in the Panthéon in Paris, which is reserved for French citizens only of the highest honor.[3]

Work


Poincaré made many contributions to different fields of pure and applied mathematics such as: celestial mechanics, fluid mechanics, optics, electricity, telegraphy, capillarity, elasticity, thermodynamics, potential theory, quantum theory, theory of relativity and physical cosmology.
He was also a popularizer of mathematics and physics and wrote several books for the lay public.
Among the specific topics he contributed to are the following:

algebraic topology

the theory of analytic functions of several complex variables

the theory of abelian functions

algebraic geometry

★ Poincaré was responsible for formulating one of the most famous problems in mathematics. Known as the Poincaré conjecture, it is a problem in topology.

Poincaré recurrence theorem

Hyperbolic geometry

number theory

the three-body problem

the theory of diophantine equations

the theory of electromagnetism

the special theory of relativity

★ In an 1894 paper, he introduced the concept of the fundamental group.

★ In the field of differential equations Poincaré has given many results that are critical for the qualitative theory of differential equations, for example the Poincaré sphere and the Poincaré map.

★ Poincaré on "everybody's belief" in the ''Normal Law of Errors'' (see normal distribution for an account of that "law")
The three-body problem

The problem of finding the general solution to the motion of more than two orbiting bodies in the solar system had eluded mathematicians since Newton's time. This was known originally as the three-body problem and later the ''n''-body problem, where ''n'' is any number of more than two orbiting bodies. The ''n''-body solution was considered very important and challenging at the close of the nineteenth century. Indeed in 1887, in honor of his 60th birthday, Oscar II, King of Sweden, advised by Gösta Mittag-Leffler, established a prize for anyone who could find the solution to the problem. The announcement was quite specific:
In case the problem could not be solved, any other important contribution to classical mechanics would then be considered to be prizeworthy. The prize was finally awarded to Poincaré, even though he did not solve the original problem.
One of the judges, the distinguished Karl Weierstrass, said, ''"This work cannot indeed be considered as furnishing the complete solution of the question proposed, but that it is nevertheless of such importance that its publication will inaugurate a new era in the history of celestial mechanics."''
(The first version of his contribution even contained a serious error; for details see the article by Diacu). The version finally printed contained many important ideas which lead to the theory of chaos. The problem as stated originally was finally solved by Karl F. Sundman for ''n'' = 3 in 1912 and was generalised to the case of ''n'' > 3 bodies by Qiudong Wang in the 1990s.
Work on relativity

Main articles: Lorentz ether theory

Local time

Poincaré's work at the Bureau des Longitudes on establishing international time zones led him to consider how clocks at rest on the Earth, which would be moving at different speeds relative to absolute space (or the "luminiferous aether"), could be synchronized. At the same time Dutch theorist Hendrik Lorentz was developing Maxwell's theory into a theory of the motion of charged particles ("electrons" or "ions"), and their interaction with radiation. He had introduced the concept of local time
:t^prime = t-vx^prime/c^2,; mathrm{where}; x^prime = x - vt
and was using it to explain the failure of optical and electrical experiments to detect motion relative to the aether (see Michelson-Morley experiment). Poincaré (1900) discussed Lorentz's "wonderful invention" of local time and remarked that it arose when moving clocks are synchronized by exchanging light signals assumed to travel with the same speed in both directions in a moving frame.[4] In "The Measure of Time" (Poincaré 1898), he discussed the difficulty of establishing simultaneity at a distance and concluded it can be established by convention. He also discussed the "postulate of the speed of light", and formulated the principle of relativity, according to which no mechanical or electromagnetic experiment can discriminate between a state of uniform motion and a state of rest.
Thereafter, Poincaré was a constant interpreter (and sometimes friendly critic) of Lorentz's theory. Poincaré as a philosopher, was interested in the "deeper meaning". Thus he interpreted Lorentz's theory in terms of the principle of relativity and in so doing he came up with many insights that are now associated with special relativity.
Marie Curie and Poincaré talk at the 1911 Solvay Conference.

Inertia of energy

In 1900 Henri Poincaré studied the conflict between the action/reaction principle and Lorentz ether theory. He tried to determine whether the center of gravity still moves with a uniform velocity when electromagnetic fields are included. He noticed that the action/reaction principle does not hold for matter alone, but that the electromagnetic field has its own momentum. The electromagnetic field energy behaves like a fictitious fluid ("fluide fictif") with a mass density of ''E/c²'' and velocity c. If the center of mass frame is defined by both the mass of matter ''and'' the mass of the fictitious fluid, and if the fictitious fluid is indestructible--it's neither created or destroyed--- then the motion of the center of mass frame remains uniform.
But electromagnetic energy can be converted into other forms of energy. So Poincaré assumed that there exists a non-electric energy fluid at each point of space, into which electromagnetic energy can be transformed and which also carries a mass proportional to the energy. In this way, the motion of the center of mass remains uniform. Poincaré said that one should not be too surprised by these assumptions, since they are only mathematical fictions.[5]
But Poincare's resolution led to a paradox when changing frames: if a Hertzian oscillator radiates in a certain direction, it will suffer a recoil from the inertia of the fictitious fluid. In the framework of Lorentz ether theory Poincare performed a Lorentz boost to the frame of the moving source. He noted that energy conservation holds in both frames, but that the law of conservation of momentum is violated. This would allow a perpetuum mobile, a notion which he abhorred. The laws of nature would have to be different in the frames of reference, and the relativity principle would not hold.
Poincaré came back to this topic in "Science and Hypothesis" (1902) and "The Value of Science" (1905). This time he rejected the possibility that energy carries mass: "... [the recoil] is contrary to the principle of Newton since our projectile here has no mass, it is not matter, it is energy". He also discussed two other unexplained effects: (1) non-conservation of mass implied by Lorentz's variable mass gamma m, Abraham's theory of variable mass and Kaufmann's experiments on the mass of fast moving electrons and (2) the non-conservation of energy in the radium experiments of Madame Curie.
It was Einstein's insight that a body losing energy as radiation or heat was losing mass of amount m = E/c^2 that resolved Poincare's paradox. The Hertzian oscillator loses mass in the emission process, and momentum is conserved in any frame. Einstein noted in 1906 that Poincaré's solution to the center of mass problem and his own were mathematically equivalent.[6]
Lorentz transformation

In 1905 Poincaré wrote to Lorentz[7] about Lorentz's paper of 1904, which Poincaré described as a "paper of supreme importance." In this letter he pointed out an error Lorentz had made when he had applied his transformation to one of Maxwell's equations, that for charge-occupied space, and also questioned the time dilation factor given by Lorentz. In a second letter to Lorentz,[8] Poincaré gave his own reason why Lorentz's time dilation factor was indeed correct after all: it was necessary to make the Lorentz transformation form a group and gave what is now known as the relativistic velocity-addition law. Poincaré later delivered a paper at the meeting of the Academy of Sciences in Paris on 5 June 1905 in which these issues were addressed. In the published version of that short paper he wrote

{{cquote|1=The essential point, established by Lorentz, is that the equations of the electromagnetic field are not altered by a certain transformation (which I will call by the name of Lorentz) of the form:
::x^prime = kellleft(x + arepsilon t
ight),~t^prime = kellleft(t + arepsilon x
ight),~y^prime = ell y,~ z^prime = ell z,~k = 1/sqrt{1- arepsilon^2}.}}

and showed that the arbitrary function ellleft( arepsilon
ight) must be unity for all arepsilon (Lorentz had set ell = 1 by a different argument) to make the transformations form a group. In an enlarged version of the paper that appeared in 1906 Poincaré pointed out that the combination x^2+ y^2+ z^2- c^2t^2 is invariant, and he introduced the 4-vector notation for which Hermann Minkowski became known.
Einstein's first paper on relativity was published three months after Poincaré's short paper, but before Poincaré's longer version. It relied on the principle of relativity to derive the Lorentz transformations and used the same clock synchronization procedure that Poincaré (1900) had described, but was remarkable in that it contained no references at all. Poincaré never acknowledged Einstein's work on Special Relativity, but Einstein acknowledged Poincaré's in the text of a lecture in 1921 called ''Geometrie und Erfahrung''. Later Einstein commented on Poincaré as being one of the pioneers of relativity, saying "Lorentz had already recognized that the transformation named after him is essential for the analysis of Maxwell's equations, and Poincaré deepened this insight still further ..."
Assessments

Poincaré's work in the development of Special Relativity is well recognized (''e.g.'' Darrigol 2004), though most historians stress that despite many similarities with Einstein's work, the two had very different research agendas and interpretations of the work (see Galison 2003 and Kragh 1999). A minority go much further, such as the historian of science Sir Edmund Whittaker, who held that Poincaré and Lorentz were the true discoverers of Relativity (Whittaker 1953). Poincaré consistently credited Lorentz's achievements, ranking his own contributions as minor. Thus, he wrote:
"Lorentz has tried to modify his hypothesis so as to make it in accord with the hypothesis of complete impossibility of measuring absolute motion. ''He has succeeded in doing so'' in his article [Lorentz 1904]. The importance of the problem has made me take up the question again; the results that I have obtained agreement on ''all important points'' with those of Lorentz; ''I have been led only to modify or complete them on some points of detail''." (Poincaré 1905) [emphasis added].
In an address in 1909 on "The New Mechanics", Poincaré discussed the demolition of Newton's mechanics brought about by Max Abraham and Lorentz, without mentioning Einstein. In one of his last essays entitled "The Quantum Theory" (1913), when referring to the Solvay Conference, Poincaré again described special relativity as the "mechanics of Lorentz":
On the other hand, in a memoir written as a tribute to Poincaré after his death, Lorentz readily admitted the mistake he had made and credited Poincaré's achievements:
In summary, Poincaré regarded the mechanics as developed by Lorentz in order to obey the principle of relativity as the essence of the theory, while Lorentz stressed that perfect invariance was first obtained by Poincaré. The modern view is inclined to say that the group property and the invariance are the essential points.

Character


Poincaré's work habits have been compared to a bee flying from flower to flower. Poincaré was interested in the way his mind worked; he studied his habits and gave a talk about his observations in 1908 at the Institute of General Psychology in Paris. He linked his way of thinking to how he made several discoveries.
The mathematician Darboux claimed he was ''un intuitif'' (intuitive), arguing that this is demonstrated by the fact that he worked so often by visual representation. He did not care about being rigorous and disliked logic. He believed that logic was not a way to invent but a way to structure ideas and that logic limits ideas.
Toulouse' characterization

Poincaré's mental organization was not only interesting to Poincaré himself but also to Toulouse, a psychologist of the Psychology Laboratory of the School of Higher Studies in Paris. Toulouse wrote a book entitled ''Henri Poincaré'' (1910). In it, he discussed Poincaré's regular schedule:

★ He worked during the same times each day in short periods of time. He undertook mathematical research for four hours a day, between 10 a.m. and noon then again from 5 p.m. to 7 p.m.. He would read articles in journals later in the evening.

★ His normal work habit was to solve a problem completely in his head, then commit the completed problem to paper.

★ He was ambidextrous and nearsighted.

★ His ability to visualise what he heard proved particularly useful when he attended lectures since his eyesight was so poor that he could not see properly what his lecturers were writing on the blackboard.
However, these abilities were somewhat balanced by his shortcomings:

★ He was physically clumsy and artistically inept.

★ He was always in a rush and disliked going back for changes or corrections.

★ He never spent a long time on a problem since he believed that the subconscious would continue working on the problem while he consciously worked on another problem.
In addition, Toulouse stated that most mathematicians worked from principles already established while Poincaré was the type that started from basic principle each time. (O'Connor et al., 2002)
His method of thinking is well summarized as:
''Habitué à négliger les détails et à ne regarder que les cimes, il passait de l'une à l'autre avec une promptitude surprenante et les faits qu'il découvrait se groupant d'eux-mêmes autour de leur centre étaient instantanément et automatiquement classés dans sa mémoire.'' (He neglected details and jumped from idea to idea, the facts gathered from each idea would then come together and solve the problem.) (Belliver, 1956)
Shortcomings

While a brilliant researcher, Poincaré's abilities to critique work in his field were limited, evidenced in what are considered Poincaré's decision-failures. For example, Poincaré was resistant to contributions from mathematicians like Georg Cantor and underestimated mathematical work that was highly relevant to fields such as economics and finance. In 1900 Poincaré misvalued Louis Bachelier's thesis "The Theory of Speculation", saying: "M. Bachelier has evidenced an original and precise mind [but] the subject is somewhat remote from those our other candidates are in the habit of treating." (Bernstein, 1996, p.199-200) However, Bachelier's work explained what was then the French government's pricing options on French Bonds and anticipated many of the pricing theories in financial markets used even today. As such, Poincaré's life interests and work can be interpreted as following what was the popular, socially demanded research at the time, rather than what is ontologically true.

Honors


'Awards'

★ Oscar II, King of Sweden's mathematical competition (1887)

American Philosophical Society 1899

Gold Medal of the Royal Astronomical Society of London (1900)

Matteucci Medal 1905

French Academy of Sciences 1906

Académie Française 1909

Bruce Medal (1911)
'Named after him'

Poincaré Prize (Mathematical Physics International Prize)

Annales Henri Poincaré (Scientific Journal)

★ Poincaré Seminar (nicknamed "Bourbaphy")

Poincaré crater (on the Moon)

Asteroid 2021 Poincaré

Publications


Poincaré's major contribution to algebraic topology was ''Analysis situs'' (1895), which was the first real systematic look at topology.
He published two major works that placed celestial mechanics on a rigorous mathematical basis:

★ ''New Methods of Celestial Mechanics'' ISBN 1563961172 (3 vols., 1892-99; Eng. trans., 1967)

★ ''Lessons of Celestial Mechanics''. (1905-10).
In popular writings he helped establish the fundamental popular definitions and perceptions of science by these writings:

★ ''Science and Hypothesis'', 1901. (complete text online)

★ ''The Value of Science'', 1905. (For more, see the French version.)

★ ''Science and Method'', 1908.

★ ''Dernières pensées'' (Eng., "Last Thoughts"); Edition Ernest Flammarion, Paris, 1913.

Philosophy


Poincaré had the opposite philosophical views of Bertrand Russell and Gottlob Frege, who believed that mathematics was a branch of logic. Poincaré strongly disagreed, claiming that intuition was the life of mathematics. Poincaré gives an interesting point of view in his book ''Science and Hypothesis'':
:''For a superficial observer, scientific truth is beyond the possibility of doubt; the logic of science is infallible, and if the scientists are sometimes mistaken, this is only from their mistaking its rule.''
Poincaré believed that arithmetic is a synthetic science. He argued that Peano's axioms cannot be proven non-circularly with the principle of induction (Murzi, 1998), therefore concluding that arithmetic is ''a priori'' synthetic and not analytic. Poincaré then went on to say that mathematics cannot be deduced from logic since it is not analytic. His views were the same as those of Kant (Kolak, 2001). However Poincaré did not share Kantian views in all branches of philosophy and mathematics. For example, in geometry, Poincaré believed that the structure of non-Euclidean space can be known analytically.

See also




Poincaré–Bendixson theorem

Poincaré–Birkhoff–Witt theorem

Poincaré half-plane model

Poincaré symmetry

Poincaré–Hopf theorem

Poincaré metric

Poincaré duality

Poincaré group

Poincaré map

Institut Henri Poincaré, Paris

History of special relativity

Relativity priority disputes

Notes


H. E. Ives (1952) wrote that Einstein's derivation was a tautology due to Einstein's use of approximations, and credited Planck (1907) with the first correct derivation of E = mc^2 in Einstein's meaning. In response J. Riseman and I. G. Young (1953) defended Einstein's derivation and physical insight, and Ives (1953) replied.
Lorentz (1904) had written x^prime = kell x^{primeprime}, t^{prime} = ell t/k - kell wx^{primeprime}/c^2, k^2 = c^2/left(c^2-w^2
ight). Later in the paper he deduced that ell = 1. Lorentz's x^{primeprime} was, in Poincaré's notation, equal to x - wt. Eliminating x^{primeprime} and putting arepsilon = -w/c yields the Lorentz transformations as Poincaré wrote them.

References


Footnotes

1. [1] Poincaré pronunciation example at Bartleby.com
2. The Internet Encyclopedia of Philosophy Jules Henri Poincaré article by Mauro Murzi - accessed November 2006.
3. http://www.lexpress.fr/idees/tribunes/dossier/allegre/dossier.asp?ida=430274
4. http://eprint.uq.edu.au/archive/00002307/
5. . Reprinted in Poincaré, Oeuvres, tome IX, S. 464-488
6.
7. http://web.archive.org/web/20050224225212/http://www.univ-nancy2.fr/poincare/chp/text/lorentz3.xml
8. http://web.archive.org/web/20050224225216/http://www.univ-nancy2.fr/poincare/chp/text/lorentz4.html

General references


Bell, Eric Temple, 1986. ''Men of Mathematics'' (reissue edition). Touchstone Books. ISBN 0671628186.

★ Belliver, André, 1956. ''Henri Poincaré ou la vocation souveraine''. Paris: Gallimard.

★ Bernstein, Peter L, 1996. "Against the Gods: A Remarkable Story of Risk". (p. 199-200). John Wiley & Sons.

★ Boyer, B. Carl, 1968. ''A History of Mathematics: Henri Poincaré'', John Wiley & Sons.

★ Olivier Darrigol (2004): "The Mystery of the Einstein-Poincaré Connection". Isis: Vol.95, Issue 4; pg. 614, 14 pgs

★ Ewald, William B., ed., 1996. ''From Kant to Hilbert: A Source Book in the Foundations of Mathematics'', 2 vols. Oxford Uni. Press. Contains among others:

Grattan-Guinness, Ivor, 2000. ''The Search for Mathematical Roots 1870-1940. Princeton Uni. Press.

★ Gray, Jeremy, 1986. ''Linear differential equations and group theory from Riemann to Poincaré'', Birkhauser

★ Kolak, Daniel, 2001. ''Lovers of Wisdom'', 2nd ed. Wadsworth.

★ Murzi, 1998. "Henri Poincaré".

★ O'Connor, J. John, and Robertson, F. Edmund, 2002, "Jules Henri Poincaré". University of St. Andrews, Scotland.

Peterson, Ivars, 1995. ''Newton's Clock: Chaos in the Solar System'' (reissue edition). W H Freeman & Co. ISBN 0716727242.

★ Poincaré, Henri. 1894. "On the nature of mathematical reasoning," 972-81.

★ ________. 1898. "On the foundations of geometry," 982-1011.

★ ________. 1900. "Intuition and Logic in mathematics," 1012-20.

★ ________. 1905-06. "Mathematics and Logic, I-III," 1021-70.

★ ________. 1910. "On transfinite numbers," 1071-74.

★ Sageret, Jules, 1911. ''Henri Poincaré''. Paris: Mercure de France.

★ Toulouse, E.,1910. ''Henri Poincaré''. - (Source biography in French)
References to work on relativity


★ Einstein, A. (1905) "Zur Elektrodynamik Bewegter Körper", ''Annalen der Physik'', '17', 891. English translation

★ Einstein, A. (1915) "Erklärung der Periheldrehung des Merkur aus der allgemainen Relativitätstheorie", ''Sitzungsberichte der Preussischen Akademie der Wissenschaften zu Berlin'', 799-801

★ Einstein, A. (1916) "Die Grundlage der allgemeinen Relativitätstheorie", ''Annalen der Physik'', 49
Galison, P. (2003) Einstein's Clocks, Poincare's Maps.

★ Giannetto, Enrico (1998) "The Rise of Special Relativity: Henri Poincaré's Works Before Einstein", ''Atti del XVIII congresso di storia della fisica e dell'astronomia

Galison, Peter Louis (2003) ''Einstein's Clocks, Poincaré's Maps: Empires of Time''. New York: W.W. Norton. ISBN 0393020010

★ Hasenöhrl, F. (1907) ''Wien Sitz.'' 'CXVI' 2a, p.1391

★ Ives, H. E. (1952) "Derivation of the Mass-Energy Relationship", ''J. Optical Society America'', '42', pp. 540-543.

★ Ives, H. E. (1953) "Note on 'Mass-Energy Relationship'", ''J. Optical Society America'', '43', 619.

★ Keswani, G. H. (1965-6) "Origin and Concept of Relativity, Parts I, II, III", ''Brit. J. Phil. Sci.'', v'15-17'.

★ Kragh, Helge. (1999) ''Quantum Generations: A History of Physics in the Twentieth Century.'' Princeton, N.J. : Princeton University Press.

★ Langevin, P. (1905) "Sur l'origine des radiations et l'inertie électromagnétique", ''Journal de Physique Théorique et Appliquée'', '4', pp.165-183.

★ Langevin, P. (1914) "Le Physicien" in ''Henri Poincaré Librairie'' (Felix Alcan 1914) pp. 115-202.

★ Lewis, G. N. (1908) ''Philosophical Magazine'', 'XVI', 705

★ Logunov, A, (2005) Book "Henri Poincaré and Relativity Theory", Nauka, Moscow, ISBN 5-02-033964-4

★ Lorentz, H. A. (1899) "Simplified Theory of Electrical and Optical Phenomena in Moving Systems", ''Proc. Acad. Science Amsterdam'', 'I', 427-43.

★ Lorentz, H. A. (1904) "Electromagnetic Phenomena in a System Moving with Any Velocity Less Than That of Light", ''Proc. Acad. Science Amsterdam'', 'IV', 669-78.

★ Lorentz, H. A. (1911) ''Amsterdam Versl.'' 'XX', 87

★ Lorentz, H.A. (1921) 1914 manuscripts "Deux memoires de Henri Poincaré," ''Acta Mathematica 38'', p.293.

★ Macrossan, M. N. (1986) "A Note on Relativity Before Einstein", ''Brit. J. Phil. Sci''., '37', pp.232-34.

★ Planck, M. (1907) ''Berlin Sitz.'', 542

★ Planck, M. (1908) ''Verh. d. Deutsch. Phys. Ges.'' 'X', p218, and ''Phys. ZS'', 'IX', 828

★ Poincaré, H. (1897) "The Relativity of Space", article in English translation

★ Poincaré, H. (1898) "La mesure du Temps", reprinted in "La valeur de la science", Ernest Flammarion, Paris.

★ Poincaré, H. (1900) "La Theorie de Lorentz et la Principe de Reaction", ''Archives Neerlandaises'', 'V', 252-78.

★ Poincaré, H. (1905) "La valeur de la Science"

★ Poincaré, H. (1904) "L'état actuel et l'avenir de la physique mathématique", ''Bulletin des sciences mathématiques 28(1904)'', 302-324 (Congress of Arts and Science, St. Louis, September 24, 1904)

★ Poincaré, H. (1905) "Sur la dynamique de l'electron", ''Comptes Rendues'', '140', 1504-8.

★ Poincaré, H. (1906) "Sur la dynamique de l'electron", Rendiconti del Circolo matematico di Palermo, t.21, 129-176.

★ Poincaré, H. (1913) ''Mathematics and Science: Last Essays'', Dover 1963 (translated from ''Dernières Pensées'' posthumously published by Ernest Flammarion, 1913)

★ Riseman, J. and I. G. Young (1953) "Mass-Energy Relationship", ''J. Optical Society America'', '43', 618.

★ Whittaker, E. T (1953) ''A History of the Theories of Aether and Electricity: Vol 2 The Modern Theories 1900-1926. Chapter II: The Relativity Theory of Poincaré and Lorentz'', Nelson, London.

External links









Science and Hypothesis (complete text online - in English)

A review of Poincaré's life and mathematical achievements - from the University of Tennessee at Martin, USA.

A timeline of Poincaré's life University of Nancy (in French).

Bruce Medal page

Henri Poincaré, His Conjecture, Copacabana and Higher Dimensions

BBC In Our Time -- discussion of the Poincaré conjecture, November 2, 2006, hosted by Melvynn Bragg ★ class=wikiexternal target=_blank>/http://www.bbc.co.uk/radio4/history/inourtime/inourtime.shtml See Internet Archive

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