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Physics

279 Einstein records classified as Physics in the supplied World History Database data.

Albert Einstein photographed in Princeton in 1947
Albert Einstein, Princeton, 1947. Photograph by Oren Jack Turner; Library of Congress image with no known restrictions. Wikimedia Commons source.

Birth of Albert Einstein

14 March 1879 ยท Ulm ยท United States of America ยท Physics

Albert Einstein is born in Ulm, Wรผrttemberg, Germany.

Capillarity Paper

1901 ยท Zurich ยท United States of America ยท Physics

Publishes his first scientific paper, examining molecular forces through capillary phenomena.

Swiss Citizenship

21 February 1901 ยท Zurich ยท United States of America ยท Physics

Einstein becomes a Swiss citizen after having been stateless since 1896.

Statistical Mechanics Paper I

1902 ยท Bern ยท United States of America ยท Physics

Publishes an early paper developing the kinetic theory of thermal equilibrium using statistical methods.

Swiss Patent Office Appointment

19 June 1902 ยท Bern ยท United States of America ยท Physics

Appointed Technical Expert, third class, at the Swiss Patent Office in Bern.

Foundations of Thermodynamics

1903 ยท Bern ยท United States of America ยท Physics

Publishes further work on the foundations of thermodynamics and statistical mechanics.

Radiation Energy Fluctuations

1904 ยท Bern ยท United States of America ยท Physics

Studies fluctuations in radiation energy, an important precursor to his later quantum work.

Gas Ionization Considered with Light Quanta

1905 ยท Bern ยท Switzerland ยท Physics

Einstein discussed photoionization as another possible application of localized radiation quanta, connecting the frequency of light with the energy needed to remove charged particles from matter.

Light Frequency Linked to Electron Energy

1905 ยท Bern ยท Switzerland ยท Physics

Einstein distinguished brightness from frequency by predicting that raising the frequency of incident light increases the energy of individual photoelectrons rather than merely increasing their number.

Light Intensity Linked to Photoelectron Number

1905 ยท Bern ยท Switzerland ยท Physics

Einstein's quantum account implied that increasing light intensity at fixed frequency mainly increases the number of available energy quanta and therefore the number of emitted electrons.

Light-Quantum Energy Frequency Relation Applied

1905 ยท Bern ยท Switzerland ยท Physics

Einstein applied the relation between quantum energy and radiation frequency to individual light quanta, giving each localized packet an energy proportional to its frequency.

Light-Quantum Hypothesis Introduced

1905 ยท Bern ยท Switzerland ยท Physics

Einstein proposed that under appropriate conditions electromagnetic radiation behaves as independently localized energy quanta, extending Planck's quantum relation from material oscillators to light itself.

Localized Radiation Energy Challenges Wave Picture

1905 ยท Bern ยท Switzerland ยท Physics

Einstein explicitly contrasted spatially localized light quanta with a purely continuous wave description, creating a fundamental tension that later developed into wave-particle duality.

Photoelectric Quantum Explanation

1905 ยท Bern ยท United States of America ยท Physics

Explains photoelectric emission by proposing that light transfers energy in discrete quanta to electrons.

Photoelectric Threshold Frequency Law

1905 ยท Bern ยท Switzerland ยท Physics

Einstein explained that photoelectron emission requires incident light above a material-dependent threshold frequency, regardless of how intense lower-frequency illumination becomes.

Photoelectron Maximum Energy Equation

1905 ยท Bern ยท Switzerland ยท Physics

Einstein related the maximum kinetic energy of emitted electrons to the incident light frequency minus the work required to free an electron from the material.

Radiation Entropy Compared with Particle Gas

1905 ยท Bern ยท Switzerland ยท Physics

Einstein compared the entropy of high-frequency radiation with that of a dilute gas and found a formal similarity that supported treating radiation energy as independently distributed quanta.

Stokes Rule Interpreted through Light Quanta

1905 ยท Bern ยท Switzerland ยท Physics

Einstein used the light-quantum hypothesis to interpret Stokes's rule for fluorescence, arguing that emitted light normally cannot carry a higher quantum energy than the absorbed radiation.

Photoelectric Effect Paper Submitted

17 March 1905 ยท Bern ยท United States of America ยท Physics

Sends his light-quantum paper to Annalen der Physik, using quanta to explain the photoelectric effect.

Doctoral Dissertation Submitted

30 April 1905 ยท Zurich ยท United States of America ยท Physics

Submits A New Determination of Molecular Dimensions as his doctoral dissertation at the University of Zurich.

Brownian Motion Paper Received

11 May 1905 ยท Bern ยท United States of America ยท Physics

Annalen der Physik receives Einstein's paper explaining Brownian motion through molecular collisions.

Special Relativity

30 June 1905 ยท Bern ยท United States of America ยท Physics

Submits On the Electrodynamics of Moving Bodies, establishing the special theory of relativity.

Doctorate Approved

27 July 1905 ยท Zurich ยท United States of America ยท Physics

The University of Zurich faculty unanimously approves Einstein's doctoral dissertation.

Mass-Energy Equivalence

27 September 1905 ยท Bern ยท United States of America ยท Physics

Submits the paper deriving the relation between mass and energy from special relativity.

Inertia of Energy Conservation

1906 ยท Bern ยท United States of America ยท Physics

Publishes a relativistic analysis linking conservation of centre-of-gravity motion with the inertia carried by energy, extending the implications of mass-energy equivalence.

Light Production and Absorption Paper

1906 ยท Bern ยท United States of America ยท Physics

Publishes work extending the light-quantum hypothesis to the production and absorption of radiation.

Matter-Radiation Energy Exchange Treated as Discrete

1906 ยท Bern ยท Switzerland ยท Physics

Einstein's continuing work on radiation treated elementary exchanges between matter and electromagnetic energy as discrete processes rather than continuously divisible transfers.

Planck Radiation Law Reinterpreted with Quanta

1906 ยท Bern ยท Switzerland ยท Physics

Einstein re-examined Planck's radiation theory and emphasized that its success could be understood more naturally if radiation exchanged energy with matter in finite quantum amounts.

Quantized Radiation Emission Reconsidered

1906 ยท Bern ยท Switzerland ยท Physics

Einstein examined how material resonators exchange energy with radiation and strengthened the case that emission as well as absorption must be connected with discrete quantum transfers.

Quantized Resonance Absorption Analysis

1906 ยท Bern ยท Switzerland ยท Physics

Einstein extended his quantum reasoning to resonant interactions between matter and radiation, treating absorption as an energy exchange constrained by discrete radiation quanta.

Doctorate Formally Awarded

15 January 1906 ยท Zurich ยท United States of America ยท Physics

The University of Zurich formally awards Einstein his doctorate in physics.

Molecular Dimensions Paper Published

8 February 1906 ยท Bern ยท United States of America ยท Physics

His revised dissertation on molecular dimensions is published in Annalen der Physik.

Patent Office Promotion

April 1906 ยท Bern ยท United States of America ยท Physics

Promoted to Technical Expert, second class, at the Swiss Patent Office.

Accelerated Clock Rate Argument

1907 ยท Bern ยท Switzerland ยท Physics

Using accelerated reference frames, Einstein concluded that clocks at different gravitational potentials should not run at identical rates, linking gravity directly with the measurement of time.

Accelerated Frames and Gravitation

1907 ยท Bern ยท United States of America ยท Physics

Extends special-relativistic reasoning to accelerated motion and concludes that gravitation must alter measurements of time, frequency and the propagation of light.

Equivalence Principle

1907 ยท Bern ยท United States of America ยท Physics

Recognises that a uniformly accelerated frame is locally equivalent to a homogeneous gravitational field, establishing the conceptual starting point for general relativity.

Free-Fall Frame Insight for Gravitation

1907 ยท Bern ยท Switzerland ยท Physics

Einstein recognised that an observer in sufficiently small free fall can describe local physics without an apparent gravitational force, an insight that became central to his equivalence principle.

Gravity and Light Propagation from Equivalence

1907 ยท Bern ยท Switzerland ยท Physics

Einstein's equivalence reasoning implied that a gravitational field must influence light propagation, opening a path from special relativity toward a relativistic theory of gravitation.

Quantum Theory of Specific Heat

1907 ยท Bern ยท United States of America ยท Physics

Applies quantum ideas to the specific heat of solids, an early success of quantum theory.

Privatdozent at Bern

1908 ยท Bern ยท United States of America ยท Physics

Begins teaching at the University of Bern as a Privatdozent.

Relativistic Electrodynamics with Laub

1908 ยท Bern ยท United States of America ยท Physics

Works with Jakob Laub on electromagnetic equations for moving bodies, reformulating electrodynamics in a way consistent with the special theory of relativity.

Relativity Principle Review

1908 ยท Bern ยท United States of America ยท Physics

Publishes a broad review of the relativity principle and its consequences, clarifying how the theory changes traditional concepts of space, time and dynamics.

Directional Momentum Assigned to Light Quanta

1909 ยท Salzburg ยท Switzerland ยท Physics

Einstein's radiation arguments associated localized quanta with directed momentum as well as energy, moving the light-quantum concept closer to the later photon picture.

Particle Contribution Identified in Radiation Fluctuations

1909 ยท Zurich ยท Switzerland ยท Physics

A second term in Einstein's fluctuation analysis had the form associated with independently moving energy quanta, strengthening his argument that radiation also possesses particle-like properties.

Radiation Fluctuation Formula Separates Two Terms

1909 ยท Zurich ยท Switzerland ยท Physics

Einstein derived a thermal-radiation fluctuation expression containing two distinct contributions, one with wave-like behaviour and another with the statistical form expected from independent quanta.

Radiation Pressure Fluctuations Analyzed

1909 ยท Zurich ยท Switzerland ยท Physics

Einstein studied statistical fluctuations in radiation pressure and used them to expose both continuous-wave and discrete-quantum aspects of thermal radiation.

Salzburg Address Defends Dual Radiation Structure

1909 ยท Salzburg ยท Switzerland ยท Physics

At the Salzburg meeting Einstein presented radiation as a problem requiring both electromagnetic waves and quantum-like localized events, highlighting a central unresolved issue of early quantum theory.

Salzburg Quantum Lecture

1909 ยท Salzburg ยท United States of America ยท Physics

Presents a major lecture arguing that radiation displays both wave-like and particle-like properties.

Thermal Radiation Statistics Support Quantum Picture

1909 ยท Zurich ยท Switzerland ยท Physics

Einstein used the statistical behaviour of black-body radiation to argue that purely classical wave theory could not account for all observed fluctuations in radiant energy.

University of Zurich Appointment

1909 ยท Zurich ยท United States of America ยท Physics

Becomes associate professor of theoretical physics at the University of Zurich.

Wave-Particle Duality Proposed for Radiation

1909 ยท Salzburg ยท Switzerland ยท Physics

Einstein argued that a future theory of light would need to combine wave structure with localized quantum structure instead of choosing only one classical description.

Critical Opalescence Theory

1910 ยท Zurich ยท United States of America ยท Physics

Explains critical opalescence using fluctuations near a liquid-gas critical point.

Einstein-Hopff Thermal Radiation Model Developed

1910 ยท Zurich ยท Switzerland ยท Physics

Einstein and Ludwig Hopf analysed a moving oscillator interacting with random thermal radiation to investigate the conditions required for matter and radiation to reach statistical equilibrium.

French Review of Relativity

1910 ยท Zurich ยท United States of America ยท Physics

Presents the principle of relativity and its consequences for modern physics to a wider European audience in a substantial French-language review.

Radiation Drag on Moving Oscillator Derived

1910 ยท Zurich ยท Switzerland ยท Physics

In the Einstein-Hopff treatment, motion through a thermal radiation field produced a friction-like drag on an oscillator, linking electromagnetic fluctuations with Brownian-style dynamics.

Thermal Radiation Equilibrium Conditions Tested

1910 ยท Zurich ยท Switzerland ยท Physics

The Einstein-Hopff analysis tested whether classical interactions between oscillators and radiation could reproduce a consistent equilibrium spectrum, revealing limitations of a purely classical treatment.

First Solvay Conference

1911 ยท Brussels ยท United States of America ยท Physics

Participates in the first Solvay Conference, discussing radiation and quantum theory with leading physicists.

Gravitational Redshift Prediction

1911 ยท Prague ยท United States of America ยท Physics

Derives the expectation that light climbing through a gravitational field should lose frequency, providing an early relativistic prediction of gravitational redshift.

Gravitational Time Dilation Prediction

1911 ยท Prague ยท Austria-Hungary ยท Physics

Einstein argued that clocks deeper in a gravitational field should run more slowly than clocks at higher gravitational potential, giving gravity a measurable effect on elapsed time.

Prague Gravitation Research Programme

1911 ยท Prague ยท United States of America ยท Physics

Uses his Prague professorship to intensify work on a relativistic theory of gravitation, concentrating on how acceleration, clocks and light behave in gravity.

Prague Paper on Gravitational Influence on Light

1911 ยท Prague ยท Austria-Hungary ยท Physics

Einstein published a study of how gravitation affects light, deriving observable consequences from the equivalence principle while his full theory of curved spacetime was still incomplete.

Professor at Prague

1911 ยท Prague ยท United States of America ยท Physics

Becomes professor of theoretical physics at the German University in Prague.

Light Deflection

June 1911 ยท Prague ยท United States of America ยท Physics

Predicts that gravity should bend starlight and proposes a solar-eclipse test.

Curved Spacetime Approach Takes Shape

1912 ยท Zurich ยท Switzerland ยท Physics

Einstein's Zurich work moved toward describing gravity through non-Euclidean spacetime geometry, connecting gravitational phenomena with the mathematical curvature of the metric.

Grossmann Tensor Collaboration

1912 ยท Zurich ยท United States of America ยท Physics

Collaborates closely with Marcel Grossmann, who guides him toward Ricci and Levi-Civita tensor calculus as the mathematical language for gravitation.

Metric Tensor Becomes Gravitational Variable

1912 ยท Zurich ยท Switzerland ยท Physics

Einstein increasingly identified the spacetime metric as the quantity that should represent gravitation, replacing the idea of gravity as an ordinary force field on fixed space and time.

Ricci Calculus Adopted for Gravity

1912 ยท Zurich ยท Switzerland ยท Physics

With Marcel Grossmann's mathematical guidance, Einstein began using Ricci and Levi-Civita tensor calculus as the formal machinery needed to describe a relativistic gravitational field.

Rotating Disk Reveals Non-Euclidean Geometry

1912 ยท Zurich ยท Switzerland ยท Physics

Einstein used the thought experiment of a rotating disk to show that ordinary Euclidean geometry need not describe measurements made in accelerated systems, strengthening the geometric approach to gravity.

Scalar Gravity Model Tested in Zurich

1912 ยท Zurich ยท Switzerland ยท Physics

Before settling on tensor field equations, Einstein explored restricted scalar descriptions of gravitation and tested whether they could preserve relativity while reproducing known gravitational effects.

Static Gravitational Field Theory

1912 ยท Zurich ยท United States of America ยท Physics

Develops field equations for a restricted static gravitational problem while searching for a theory that can extend relativity beyond inertial reference frames.

Tensor Calculus Collaboration

1912 ยท Zurich ยท United States of America ยท Physics

Works with Marcel Grossmann to master tensor calculus for a relativistic theory of gravitation.

Turn to Non-Euclidean Geometry

1912 ยท Zurich ยท United States of America ยท Physics

Realises that gravitation may require non-Euclidean geometry, redirecting the search for a relativistic gravity theory toward curved spacetime mathematics.

Variable Light Speed in Gravity

1912 ยท Zurich ยท United States of America ยท Physics

Explores a formulation in which the coordinate speed of light varies with gravitational potential, an intermediate step toward a geometric theory of gravity.

Zurich Notebook

1912 ยท Zurich ยท United States of America ยท Physics

Uses the Zurich Notebook to explore candidate gravitational field equations and differential geometry.

Zurich Notebook Tensor Calculations

1912 ยท Zurich ยท United States of America ยท Physics

Fills the Zurich Notebook with tensor calculations while testing candidate gravitational field equations and learning the differential geometry needed for a covariant theory.

ETH Zurich Professorship

1 October 1912 ยท Zurich ยท United States of America ยท Physics

Begins work as professor of theoretical physics at ETH Zurich.

Einstein-Grossmann Collaboration

1913 ยท Zurich ยท United States of America ยท Physics

Collaborates closely with Marcel Grossmann on the mathematical framework of gravitation.

Entwurf Field Equations Proposed

1913 ยท Zurich ยท Switzerland ยท Physics

The Entwurf collaboration introduced provisional field equations intended to connect the spacetime metric with matter, giving Einstein a concrete but still incomplete relativistic theory of gravitation.

Entwurf Theory

1913 ยท Zurich ยท United States of America ยท Physics

Publishes the Entwurf gravitational theory with Marcel Grossmann as an intermediate step toward general relativity.

Entwurf Theory Links Metric to Matter

1913 ยท Zurich ยท Switzerland ยท Physics

Einstein's developing theory treated the metric field as physically determined by matter and energy, moving the gravitational problem toward the geometry-source relationship later embodied in his final equations.

Entwurf Theory Published with Grossmann

1913 ยท Zurich ยท Switzerland ยท Physics

Einstein and Marcel Grossmann published the Entwurf theory, an intermediate gravitational framework that used tensor methods but did not yet possess the full general covariance of general relativity.

Hole Argument Used Against General Covariance

1913 ยท Zurich ยท Switzerland ยท Physics

Einstein developed the hole argument as a reason to distrust unrestricted general covariance, a position he later abandoned when completing general relativity in 1915.

Berlin Academy Appointment

1914 ยท Berlin ยท United States of America ยท Physics

Moves to Berlin for a senior research appointment and membership of the Prussian Academy of Sciences.

Covariance Problem in Gravitation

1914 ยท Berlin ยท United States of America ยท Physics

Publishes work refining the mathematical and covariance problems of his developing gravitational theory.

Covariance Restrictions Defended

1914 ยท Berlin ยท Germany ยท Physics

Einstein defended the restricted covariance of his provisional gravitational equations, believing at the time that broader coordinate freedom would prevent a unique physical description.

Einstein-Grossmann Covariance Analysis

1914 ยท Berlin ยท United States of America ยท Physics

Continues with Grossmann to examine covariance properties of their gravitational equations, exposing problems that eventually drive Einstein back toward general covariance.

Formal Entwurf Theory Presented in Berlin

1914 ยท Berlin ยท Germany ยท Physics

Einstein gave a systematic mathematical presentation of the Entwurf gravitational theory after moving to Berlin, clarifying its field equations, coordinate restrictions and physical assumptions.

Formal Foundations of General Relativity

1914 ยท Berlin ยท United States of America ยท Physics

Publishes a detailed formal treatment of the developing gravitational theory, presenting its mathematical structure before he restores fully general covariance.

Gravitational Conservation Laws Reconsidered

1914 ยท Berlin ยท Germany ยท Physics

Einstein investigated how energy and momentum conservation should be formulated when the gravitational field itself participates in the dynamics of spacetime.

Manifesto to Europeans

1914 ยท Berlin ยท United States of America ยท Physics

Co-signs a pacifist appeal opposing wartime nationalism among European intellectuals.

Nordstrom Gravitation Recast with Fokker

1914 ยท Berlin ยท United States of America ยท Physics

With Adriaan Fokker, reformulates Nordstrom's competing gravitation theory using tensor methods, clarifying how relativistic gravity could be expressed geometrically.

Rotating Coordinates Test the Entwurf Theory

1914 ยท Berlin ยท Germany ยท Physics

Einstein examined rotating coordinate systems as a demanding consistency test for the Entwurf equations, exposing difficulties that contributed to his later rejection of the provisional theory.

Einstein-de Haas Effect

1915 ยท Berlin ยท United States of America ยท Physics

Publishes experimental work with Wander de Haas linking magnetism to angular momentum.

Return to General Covariance

1915 ยท Berlin ยท Germany ยท Physics

Einstein abandoned key restrictions of the Entwurf approach and returned to generally covariant tensor equations, beginning the final rapid reconstruction of his gravitational theory.

Gottingen Relativity Lectures

June 1915 ยท Gottingen ยท United States of America ยท Physics

Lectures in Gottingen on his gravitational theory, presenting the unfinished framework to leading mathematicians while he approaches the final generally covariant equations.

November 4 Covariant Gravity Equations

4 November 1915 ยท Berlin ยท Germany ยท Physics

Einstein presented new gravitational field equations to the Prussian Academy that restored much broader covariance and marked the first of his decisive November 1915 communications.

Restricted Covariance Equations

4 November 1915 ยท Berlin ยท United States of America ยท Physics

Presents revised gravitational field equations to the Prussian Academy during his final push toward general relativity.

November 11 Vacuum Field Equations

11 November 1915 ยท Berlin ยท Germany ยท Physics

Einstein refined his field equations under a trace condition and showed how the revised framework could approach fully covariant gravitation in regions outside matter.

Second November Field Equations

11 November 1915 ยท Berlin ยท United States of America ยท Physics

Presents improved gravitational equations to the Prussian Academy and moves substantially closer to the generally covariant form completed later that month.

Unimodular Gravitation Equations

11 November 1915 ยท Berlin ยท United States of America ยท Physics

Presents another formulation of gravitation using a restricted coordinate condition with unit determinant.

Final Generally Covariant Field Equations

25 November 1915 ยท Berlin ยท United States of America ยท Physics

Presents the final generally covariant gravitational field equations to the Prussian Academy, completing the mathematical core of general relativity.

General Relativity Field Equations

25 November 1915 ยท Berlin ยท United States of America ยท Physics

Presents the final generally covariant gravitational field equations to the Prussian Academy.

November 25 Matter-Coupled Field Equations

25 November 1915 ยท Berlin ยท Germany ยท Physics

Einstein presented the final generally covariant field equations including their coupling to matter, completing the mathematical core of general relativity.

Absorption Probability Coefficient Defined

1916 ยท Berlin ยท Germany ยท Physics

Einstein represented the probability of an atom absorbing incident radiation and moving to a higher energy state with a coefficient proportional to the surrounding radiation density.

Atomic Transition Probabilities Introduced

1916 ยท Berlin ยท Germany ยท Physics

Einstein formulated radiation processes in terms of probabilities for transitions between atomic energy states, creating a statistical framework for absorption and emission.

Detailed Balance Applied to Matter and Radiation

1916 ยท Berlin ยท Germany ยท Physics

Einstein required upward and downward atomic transitions to balance in thermal equilibrium, using that condition to connect transition probabilities with the equilibrium radiation spectrum.

Energy Conservation in General Relativity

1916 ยท Berlin ยท United States of America ยท Physics

Develops the treatment of energy and momentum in the gravitational field, addressing how conservation laws operate within the generally covariant theory.

Foundation of General Relativity

1916 ยท Berlin ยท United States of America ยท Physics

Publishes a systematic presentation of the general theory of relativity and its field equations.

General Relativity Review Article Published

1916 ยท Berlin ยท Germany ยท Physics

Einstein published a comprehensive exposition of general relativity that assembled the geometric framework, field equations and physical consequences into a systematic theory.

Geodesic Motion Described in Curved Spacetime

1916 ยท Berlin ยท Germany ยท Physics

Einstein's mature theory described freely falling bodies as following the straightest possible world-lines through curved spacetime rather than being pulled by a Newtonian gravitational force.

German Physical Society Presidency

1916 ยท Berlin ยท United States of America ยท Physics

Serves as president of the German Physical Society during the consolidation of general relativity.

Gravitational Energy Flux Treated with Pseudotensor

1916 ยท Berlin ยท Germany ยท Physics

Einstein developed a gravitational energy-momentum construction to discuss how changing gravitational fields can transport energy despite the special conservation difficulties of general relativity.

Gravitational Waves Propagate at Light Speed

1916 ยท Berlin ยท Germany ยท Physics

Einstein's wave analysis showed that physical gravitational disturbances in the relativistic theory propagate through empty space at the speed of light.

Hamilton Principle for General Relativity

1916 ยท Berlin ยท United States of America ยท Physics

Formulates general relativity using Hamilton's variational principle, providing a compact mathematical route to the gravitational field equations and their conservation properties.

Kottler Equivalence Hypothesis Response

1916 ยท Berlin ยท United States of America ยท Physics

Responds to Friedrich Kottler's criticism of the equivalence hypothesis, defending the conceptual basis on which his route from special to general relativity depended.

Nonlinearity of Gravitational Field Established

1916 ยท Berlin ยท Germany ยท Physics

Einstein's field equations made gravity nonlinear, so the gravitational field contributes to the dynamics instead of behaving as a simple superposition of independent Newtonian forces.

Planck Spectrum Recovered from Transition Statistics

1916 ยท Berlin ยท Germany ยท Physics

Einstein showed that his statistical rules for absorption, spontaneous emission and induced emission can reproduce Planck's black-body radiation law under thermal equilibrium.

Quantum Theory of Radiation

1916 ยท Berlin ยท United States of America ยท Physics

Develops a quantum theory of radiation introducing transition probabilities later represented by Einstein coefficients.

Spontaneous Emission Probability Defined

1916 ยท Berlin ยท Germany ยท Physics

Einstein introduced a coefficient describing the probability that an excited atom will emit radiation spontaneously and fall to a lower energy state.

Stimulated Emission Probability Coefficient Defined

1916 ยท Berlin ยท Germany ยท Physics

Einstein introduced a second radiation-dependent transition probability in which incident radiation stimulates an excited atom to emit additional radiation.

Stress-Energy Identified as Source of Curvature

1916 ยท Berlin ยท Germany ยท Physics

General relativity connected spacetime curvature with the energy, momentum and stresses of matter, making the physical contents of the universe sources of the gravitational geometry.

Weak-Field Gravitational Waves Derived

1916 ยท Berlin ยท Germany ยท Physics

Einstein linearised the gravitational field equations in the weak-field limit and identified wave-like disturbances capable of propagating through spacetime.

Schwarzschild Solution Presented to Academy

13 January 1916 ยท Berlin ยท United States of America ยท Physics

Communicates Karl Schwarzschild's exact solution of the new field equations to the Prussian Academy, demonstrating that general relativity admits important exact solutions.

Atomic Recoil Required by Photon Momentum

1917 ยท Berlin ยท Germany ยท Physics

By assigning momentum to individual radiation quanta, Einstein concluded that atoms must recoil when they emit or absorb directed packets of light.

Random Emission Directions Linked to Molecular Motion

1917 ยท Berlin ยท Germany ยท Physics

Einstein showed that randomly directed quantum emission events contribute to molecular momentum fluctuations and must be balanced statistically in thermal equilibrium.

Stimulated Emission

1917 ยท Berlin ยท United States of America ยท Physics

Formulates stimulated emission in his quantum theory of radiation, a principle later fundamental to lasers.

Stimulated Emission Predicted from Thermal Equilibrium

1917 ยท Berlin ยท Germany ยท Physics

Einstein's equilibrium analysis required an induced emission process in which incident radiation increases the probability that an excited atom emits matching radiation.

Gravitational Wave Energy Calculation Corrected

1918 ยท Berlin ยท Germany ยท Physics

Einstein revisited his gravitational-wave analysis and corrected the treatment of radiated energy, removing misleading wave modes from the earlier calculation.

Mach Principle Formulation

1918 ยท Berlin ยท United States of America ยท Physics

Publishes a foundational discussion of general relativity in which he explicitly names Mach's principle and distinguishes it from the equivalence and relativity principles.

Mass Quadrupole Identified as Leading Radiation Source

1918 ยท Berlin ยท Germany ยท Physics

Einstein showed that the leading gravitational radiation from an isolated slow-moving system is governed by changes in its mass quadrupole moment rather than by a simple mass dipole.

Quadrupole Radiation Formula

1918 ยท Berlin ยท United States of America ยท Physics

Derives the quadrupole formula for gravitational radiation, relating emitted wave power to changing mass distributions in accelerating systems.

Zurich Guest Lectures

1918 ยท Zurich ยท United States of America ยท Physics

Returns to Zurich for guest lectures while continuing work on relativity and quantum theory.

International Scientific Fame

1919 ยท Berlin ยท United States of America ยท Physics

Becomes internationally famous after eclipse observations are widely reported as confirming general relativity.

The Times Relativity Explanation

28 November 1919 ยท London ยท United States of America ยท Physics

Publishes an accessible explanation of relativity in The Times, describing the conceptual differences between the special and general theories for a broad audience.

Anti-Relativity Campaign

1920 ยท Berlin ยท United States of America ยท Physics

Publicly confronts organized attacks on relativity amid growing political and antisemitic hostility.

Spacetime Ether Reinterpreted in Leiden

1920 ยท Leiden ยท Netherlands ยท Physics

In his Leiden address Einstein argued that general relativity gives spacetime physical properties while rejecting the mechanical luminiferous ether required by nineteenth-century theories of light.

Ether and Relativity Leiden Address

May 1920 ยท Leiden ยท United States of America ยท Physics

Delivers his Leiden inaugural lecture on ether and relativity, arguing that general relativity permits a physical spacetime structure without a mechanical luminiferous ether.

Ether and Relativity Lecture

5 May 1920 ยท Leiden ยท United States of America ยท Physics

Delivers the lecture Ether and the Theory of Relativity, redefining the concept in gravitational terms.

Bad Nauheim Relativity Debate

September 1920 ยท Bad Nauheim ยท United States of America ยท Physics

Publicly debates critics including Philipp Lenard at the German scientists' meeting in Bad Nauheim, defending the physical basis and interpretation of relativity.

Leiden Special Professorship

27 October 1920 ยท Leiden ยท United States of America ยท Physics

Begins official duties as special professor at Leiden University.

General Relativity Foundation Supplement

1921 ยท Berlin ยท United States of America ยท Physics

Publishes a proposed addition to the foundations of general relativity, continuing his effort to strengthen the conceptual and mathematical basis of gravitational field theory.

Hebrew University Fundraising Tour

1921 ยท United States ยท United States of America ยท Physics

Uses his first American visit to support fundraising for the future Hebrew University of Jerusalem.

Nobel Prize

1921 ยท Stockholm ยท United States of America ยท Physics

Receives the Nobel Prize in Physics for contributions to theoretical physics, particularly his explanation of the law governing the photoelectric effect.

Nobel Prize in Physics

1921 ยท Berlin ยท United States of America ยท Physics

Awarded the 1921 Nobel Prize in Physics for theoretical physics, especially the law of the photoelectric effect.

Princeton Stafford Little Lectures

1921 ยท Princeton ยท United States of America ยท Physics

Delivers four Stafford Little Lectures explaining special and general relativity.

Geometry and Experience Lecture

January 1921 ยท Berlin ยท United States of America ยท Physics

Explains how geometry acquires physical meaning through measurement and discusses the relationship between mathematical geometry and the spacetime structure of general relativity.

First Arrival in New York

2 April 1921 ยท New York ยท United States of America ยท Physics

Arrives in New York during his first visit to the United States, including lectures and fundraising.

Early Unified Field Program

1922 ยท Berlin ยท United States of America ยท Physics

Begins sustained attempts to combine gravitation and electromagnetism within a single field framework.

Japan Lecture Tour

1922 ยท Japan ยท United States of America ยท Physics

Travels through Japan giving lectures and public talks on relativity and modern physics.

Photoelectric Law Highlighted in Nobel Citation

1922 ยท Berlin ยท Germany ยท Physics

The Nobel citation singled out Einstein's quantitative law of the photoelectric effect, giving formal recognition to a result rooted in his 1905 light-quantum hypothesis.

The Meaning of Relativity

1922 ยท Princeton ยท United States of America ยท Physics

The Meaning of Relativity is published from the four lectures Einstein delivered at Princeton in May 1921.

The Meaning of Relativity Published

1922 ยท Princeton ยท United States of America ยท Physics

Publishes The Meaning of Relativity from his Princeton lectures, giving a systematic account of special relativity, tensor methods, gravitation and cosmological applications.

Paris Relativity Lecture Series

April 1922 ยท Paris ยท United States of America ยท Physics

Presents relativity to French scientific audiences during a highly publicised Paris visit, explaining both the special theory and the geometric theory of gravitation.

Einstein-Bergson Time Debate

6 April 1922 ยท Paris ยท United States of America ยท Physics

Debates Henri Bergson over the meaning of time, confronting philosophical objections to the operational treatment of simultaneity in special relativity.

Nobel Award Announced for Photoelectric Law

9 November 1922 ยท Berlin ยท Germany ยท Physics

The Royal Swedish Academy of Sciences announced Einstein as the recipient of the reserved 1921 Nobel Prize in Physics, emphasizing his discovery of the law of the photoelectric effect.

Einstein Misses Stockholm Ceremony during Japan Journey

10 December 1922 ยท Japan ยท Germany ยท Physics

Einstein was travelling in Asia when the 1921 Physics Prize was presented in Stockholm, so he did not attend the December ceremony honouring his photoelectric work.

Kyoto Relativity Lecture

14 December 1922 ยท Kyoto ยท United States of America ยท Physics

Explains how he developed the theory of relativity in a lecture at Kyoto University.

Affine Field Theory

1923 ยท Berlin ยท United States of America ยท Physics

Explores an affine field theory as a possible extension of general relativity, seeking a unified geometric description of gravitation and electromagnetism.

General Relativity Academy Paper

1923 ยท Berlin ยท United States of America ยท Physics

Publishes a further Prussian Academy paper on general relativity, revisiting technical aspects of the theory after its rapid international acceptance.

Leiden Research Stay

1923 ยท Leiden ยท United States of America ยท Physics

Spends an extended period in Leiden amid political threats in Germany, continuing scientific work.

Barcelona Relativity Lectures

February 1923 ยท Barcelona ยท United States of America ยท Physics

Begins his Spanish visit with lectures in Barcelona, presenting relativity to scientists and helping stimulate wider discussion of modern theoretical physics in Spain.

Jerusalem Relativity Lecture

7 February 1923 ยท Jerusalem ยท United States of America ยท Physics

Lectures in French on relativity during his visit to British Mandate Palestine.

Jerusalem German Lecture

13 February 1923 ยท Jerusalem ยท United States of America ยท Physics

Gives a second Jerusalem lecture on relativity, this time in German.

Madrid Relativity Lectures

March 1923 ยท Madrid ยท United States of America ยท Physics

Gives several Madrid lectures on relativity and theoretical physics to university, academy and scientific audiences during his celebrated Spanish tour.

Zaragoza Relativity Lectures

March 1923 ยท Zaragoza ยท United States of America ยท Physics

Concludes his Spanish scientific tour with lectures in Zaragoza that further disseminate the concepts and mathematical outlook of relativity.

Madrid Academy Corresponding Membership

4 March 1923 ยท Madrid ยท United States of America ยท Physics

Becomes a corresponding member of the Royal Academy of Exact, Physical and Natural Sciences in Madrid.

Madrid Honorary Doctorate

8 March 1923 ยท Madrid ยท United States of America ยท Physics

Receives an honorary doctorate in science from the University of Madrid.

Nobel Lecture

11 July 1923 ยท Gothenburg ยท United States of America ยท Physics

Delivers his Nobel lecture on fundamental ideas and problems of relativity.

Bose Counting Recasts Planck Radiation Law

1924 ยท Berlin ยท Germany ยท Physics

Einstein recognized that Bose's counting method obtained Planck's spectrum by treating light quanta statistically without relying on the classical independent-particle counting used for ordinary gases.

Bose Light-Quantum Manuscript Reaches Einstein

1924 ยท Berlin ยท Germany ยท Physics

Satyendra Nath Bose sent Einstein a manuscript deriving Planck's radiation law by a new statistical counting method applied directly to indistinguishable light quanta.

Bose Paper Translation

1924 ยท Berlin ยท United States of America ยท Physics

Translates Satyendra Nath Bose's paper on Planck's law into German and arranges its publication.

Bose-Einstein Condensation Prediction

1924 ยท Berlin ยท United States of America ยท Physics

Predicts that ideal bosonic particles can accumulate in the lowest quantum state at low temperature.

Bose-Einstein Statistics

1924 ยท Berlin ยท United States of America ยท Physics

Extends Bose's statistical method from photons to particles of an ideal gas.

Einstein Translates Bose Photon Statistics Paper

1924 ยท Berlin ยท Germany ยท Physics

Einstein translated Bose's manuscript on the quantum statistics of radiation into German after recognizing the importance of its treatment of light quanta.

Photon Indistinguishability Gains Statistical Role

1924 ยท Berlin ยท Germany ยท Physics

Bose's method, promoted by Einstein, treated light quanta as statistically indistinguishable objects, an idea that became fundamental to quantum statistics.

BKS Statistical Conservation Challenged by Photon Picture

1925 ยท Berlin ยท Germany ยท Physics

Einstein continued to favour exact energy and momentum conservation in individual radiation processes rather than the merely statistical conservation proposed by the Bohr-Kramers-Slater approach.

Einstein Extends Radiation Duality Analogy to Matter

1925 ยท Berlin ยท Germany ยท Physics

Einstein drew an analogy between the wave-particle duality he had identified for radiation and the emerging wave description of material particles, reinforcing the broader quantum duality concept.

Quantum Mechanics Critique Begins

1925 ยท Berlin ยท United States of America ยท Physics

Engages critically with the emerging matrix and wave formulations of quantum mechanics.

Second Quantum Gas Paper

1925 ยท Berlin ยท United States of America ยท Physics

Publishes further work on the quantum theory of the ideal monatomic gas.

South America Lecture Tour

1925 ยท South America ยท United States of America ยท Physics

Tours Argentina, Uruguay and Brazil, giving lectures and meeting scientific and civic audiences.

Unified Gravitation and Electromagnetism Paper

1925 ยท Berlin ยท United States of America ยท Physics

Publishes a unified field theory of gravitation and electricity, beginning a long programme to extend relativity into a single classical field framework.

Buenos Aires Relativity Lectures

April 1925 ยท Buenos Aires ยท United States of America ยท Physics

Lectures in Buenos Aires on relativity and modern theoretical physics, bringing his account of spacetime and gravitation to large South American audiences.

Montevideo Relativity Lectures

April 1925 ยท Montevideo ยท United States of America ยท Physics

Visits Montevideo and discusses relativity with university and public audiences, extending the international circulation of his gravitational and spacetime ideas.

Rio de Janeiro Relativity Lectures

May 1925 ยท Rio de Janeiro ยท United States of America ยท Physics

Speaks in Rio de Janeiro during his South American tour, explaining relativity while participating in debates about theoretical science and its wider significance.

Copley Medal

30 November 1925 ยท London ยท United States of America ยท Physics

Awarded the Royal Society's Copley Medal for relativity and contributions to quantum theory.

Canal-Ray Radiation Coherence Test Proposed

1926 ยท Berlin ยท Germany ยท Physics

Einstein proposed experiments on light emitted by moving canal-ray atoms to test how quantum emission events could coexist with the coherence properties expected from wave optics.

Kaluza Five-Dimensional Theory Reconsidered

1926 ยท Berlin ยท United States of America ยท Physics

Reconsiders Theodor Kaluza's five-dimensional approach after developments by Oskar Klein, seeing new possibilities for unifying gravitation and electromagnetism geometrically.

Rupp Radiation Experiments

1926 ยท Berlin ยท United States of America ยท Physics

Collaborates with Emil Rupp on proposed tests of whether atomic radiation behaves as waves or quanta.

Schrodinger Wave Mechanics Discussion

1926 ยท Berlin ยท United States of America ยท Physics

Studies and discusses Schrรถdinger's wave mechanics while questioning its physical interpretation.

Bohr-Einstein Quantum Debate

1927 ยท Brussels ยท United States of America ยท Physics

Challenges Niels Bohr with thought experiments testing the completeness of quantum mechanics.

Fifth Solvay Conference

1927 ยท Brussels ยท United States of America ยท Physics

Participates in the fifth Solvay Conference and debates the interpretation of quantum mechanics.

General Relativity and Law of Motion

1927 ยท Berlin ยท United States of America ยท Physics

With Jakob Grommer, investigates whether the motion of particles can be derived from the gravitational field equations rather than imposed as a separate law.

Motion from Field Equations

1927 ยท Berlin ยท United States of America ยท Physics

Investigates with Jakob Grommer whether particle motion can follow directly from gravitational field equations.

Kaluza Theory Academy Papers

February 1927 ยท Berlin ยท United States of America ยท Physics

Presents Academy papers on Kaluza's connection between gravitation and electricity, deriving important aspects of the five-dimensional unified-field framework.

Distant Parallelism Geometry

1928 ยท Berlin ยท United States of America ยท Physics

Introduces a geometry that preserves distant parallelism, adopting teleparallel structures as a new mathematical basis for attempts to unify gravity and electromagnetism.

Teleparallel Unified Field Programme

1928 ยท Berlin ยท United States of America ยท Physics

Develops the teleparallel unified-field programme, replacing ordinary Riemannian geometry with tetrad-based structures intended to encompass gravitation and electromagnetism together.

Teleparallel Unified Field Theory

1928 ยท Berlin ยท United States of America ยท Physics

Develops a unified-field approach using distant parallelism, also called teleparallel geometry.

Tetrad Fields Introduced for Unified Gravitation

1928 ยท Berlin ยท Germany ยท Physics

Einstein adopted tetrad fields and distant parallelism as a new geometric language in an attempt to place gravitation and electromagnetism inside one unified classical field theory.

Helen Dukas Becomes Assistant

13 April 1928 ยท Berlin ยท United States of America ยท Physics

Employs Helen Dukas as his secretary and assistant, beginning a long professional association.

Unified Field Theory and Hamilton Principle

1929 ยท Berlin ยท United States of America ยท Physics

Publishes a unified field formulation based on distant parallelism and Hamilton's principle, continuing his search for equations joining gravitational and electromagnetic fields.

Unified Field Theory Publication

1929 ยท Berlin ยท United States of America ยท Physics

Publishes a widely publicized unified-field theory based on teleparallel geometry.

Max Planck Medal

28 June 1929 ยท Berlin ยท United States of America ยท Physics

Receives the inaugural Max Planck Medal for outstanding achievement in theoretical physics.

Space and Ether Harnack House Lecture

December 1929 ยท Berlin ยท United States of America ยท Physics

Lectures at Harnack House on the problem of space and ether, revisiting how relativity changes the physical interpretation of spacetime and field structure.

Escaping Photon Used to Challenge Energy-Time Uncertainty

1930 ยท Brussels ยท Belgium ยท Physics

Einstein argued that measuring the mass loss of a timed photon box could in principle determine both the photon's energy and its emission time more precisely than quantum uncertainty allowed.

Exact Static Unified-Field Solutions

1930 ยท Berlin ยท United States of America ยท Physics

Publishes work with Walther Mayer giving exact static solutions of unified-field equations, testing whether the programme can represent physically meaningful configurations.

First Caltech Winter Visit

1930 ยท Pasadena ยท United States of America ยท Physics

Begins an extended academic visit to the California Institute of Technology.

Photon Box Thought Experiment Presented

1930 ยท Brussels ยท Belgium ยท Physics

At the Solvay Conference Einstein proposed a box-and-clock thought experiment intended to challenge the energy-time uncertainty relation by weighing a box before and after a photon escaped.

Riemann Metric and Distant Parallelism

1930 ยท Berlin ยท United States of America ยท Physics

Further develops spaces combining a Riemann metric with distant parallelism, refining the geometric machinery behind his teleparallel unified-field theory.

Sixth Solvay Conference

1930 ยท Brussels ยท United States of America ยท Physics

Attends the sixth Solvay Conference and continues discussions on quantum theory and field physics.

Unified Field Equation Compatibility

1930 ยท Berlin ยท United States of America ยท Physics

Examines the compatibility of equations in the unified-field programme, addressing mathematical consistency before the theory can be regarded as physically viable.

ETH Zurich Honorary Doctorate

7 November 1930 ยท Zurich ยท United States of America ยท Physics

Receives an honorary Doctor of Science degree from ETH Zurich.

Caltech Relativity and Cosmology Visit

December 1930 ยท Pasadena ยท United States of America ยท Physics

Begins an extended visit to Caltech where relativity, cosmology and unified-field questions form an important part of his discussions with American physicists and astronomers.

Oxford Rhodes Lectures

1931 ยท Oxford ยท United States of America ยท Physics

Gives three Rhodes Memorial Lectures on relativity, cosmology and his latest work in theoretical physics.

Oxford Honorary Doctorate

23 May 1931 ยท Oxford ยท United States of America ยท Physics

Receives an honorary Doctor of Science degree from the University of Oxford.

Unified Gravitation and Electricity Theory

1932 ยท Berlin ยท United States of America ยท Physics

Publishes another unified theory of gravitation and electricity, continuing to test alternative geometrical structures beyond the standard equations of general relativity.

Leopoldina Membership

17 March 1932 ยท Halle ยท United States of America ยท Physics

Becomes a member of the German Academy of Natural Scientists Leopoldina.

Permanent Move to Princeton

1933 ยท Princeton ยท United States of America ยท Physics

Settles in the United States after the Nazi rise to power and joins the Institute for Advanced Study.

Renounces German Citizenship

1933 ยท Belgium ยท United States of America ยท Physics

Renounces German citizenship after the Nazi seizure of power while retaining Swiss citizenship.

Leaves Prussian Academy

28 March 1933 ยท Belgium ยท United States of America ยท Physics

Resigns from the Prussian Academy of Sciences after deciding not to return to Nazi Germany.

Glasgow Origins of General Relativity Lecture

June 1933 ยท Glasgow ยท United States of America ยท Physics

Lectures in Glasgow on the origins and development of general relativity, recounting the physical ideas that led from equivalence to curved spacetime.

On the Method of Theoretical Physics

1934 ยท Princeton ยท United States of America ยท Physics

Publishes reflections on how fundamental theoretical physics develops from principles and mathematical structure.

Josiah Willard Gibbs Lecture

28 December 1934 ยท Pittsburgh ยท United States of America ยท Physics

Delivers the Gibbs Lecture on an elementary proof of the equivalence of mass and energy.

Bridge Geometry Connects Two Spacetime Sheets

1935 ยท Princeton ยท United States of America ยท Physics

The Einstein-Rosen construction joined two copies of a spacetime solution through a geometric bridge, creating an early mathematical example of what later literature called a wormhole.

Einstein-Rosen Bridge

1935 ยท Princeton ยท United States of America ยท Physics

With Nathan Rosen, studies bridge solutions in general relativity connecting two sheets of spacetime.

Einstein-Rosen Bridge Proposed as Particle Model

1935 ยท Princeton ยท United States of America ยท Physics

Einstein and Nathan Rosen constructed a bridge geometry from solutions of the gravitational field equations while exploring whether particles could be represented without ordinary singularities.

EPR Paper

15 May 1935 ยท Princeton ยท United States of America ยท Physics

Einstein, Podolsky and Rosen publish their argument that quantum mechanics may not provide a complete description of physical reality.

Franklin Medal

15 May 1935 ยท Philadelphia ยท United States of America ยท Physics

Receives the Franklin Medal in recognition of his work in relativity and the photoelectric effect.

Gravitational Wave Debate

1936 ยท Princeton ยท United States of America ยท Physics

Einstein and Nathan Rosen initially question whether exact gravitational waves exist, then recognise that a troublesome singularity is a coordinate effect rather than a physical obstruction.

Gravitational-Wave Manuscript with Rosen

1936 ยท Princeton ยท United States of America ยท Physics

With Nathan Rosen, submits a manuscript questioning gravitational waves, then revises the analysis after recognising that a problematic singularity arose from the coordinates used.

US Declaration of Intention

15 January 1936 ยท Trenton ยท United States of America ยท Physics

Files a declaration of intention to become a citizen of the United States.

Einstein-Infeld-Hoffmann Collaboration

1937 ยท Princeton ยท United States of America ยท Physics

Works with Leopold Infeld and Banesh Hoffmann on deriving equations of motion from general relativity.

Einstein-Rosen Waves

January 1937 ยท Princeton ยท United States of America ยท Physics

Einstein and Rosen publish a corrected treatment of cylindrical gravitational waves, demonstrating that exact wave solutions can exist within general relativity.

EIH Method Derives Gravitational Motion

1938 ยท Princeton ยท United States of America ยท Physics

With Leopold Infeld and Banesh Hoffmann, Einstein developed an approximation in which the motion of gravitating bodies follows from the relativistic field equations rather than from a separately imposed force law.

Einstein-Infeld-Hoffmann Equations

1938 ยท Princeton ยท United States of America ยท Physics

Publishes work deriving approximate equations of motion for gravitating bodies from general relativity.

Evolution of Physics Published

1938 ยท Princeton ยท United States of America ยท Physics

Publishes The Evolution of Physics with Leopold Infeld for a broad readership.

The Evolution of Physics Relativity Exposition

1938 ยท Princeton ยท United States of America ยท Physics

With Leopold Infeld, publishes The Evolution of Physics, explaining the conceptual transition from classical mechanics and fields to relativity and modern physics.

United States Citizenship

1 October 1940 ยท Trenton ยท United States of America ยท Physics

Becomes a United States citizen while retaining Swiss citizenship.

Einstein-Pauli Non-Singular Field Result

1941 ยท Princeton ยท United States of America ยท Physics

With Wolfgang Pauli, proves a restrictive result on non-singular stationary solutions of the relativistic gravitational field equations with nonzero total mass.

Generalization of Relativistic Gravitation

1945 ยท Princeton ยท United States of America ยท Physics

Publishes a generalization of the relativistic theory of gravitation, continuing his attempt to construct a unified classical field theory extending general relativity.

Elementary Mass-Energy Derivation

1946 ยท Princeton ยท United States of America ยท Physics

Publishes an elementary derivation of the equivalence of mass and energy, revisiting one of the central physical consequences that emerged from special relativity.

General Field Theory Draft

1946 ยท Princeton ยท United States of America ยท Physics

Presents a new draft of field equations for his continuing general field theory program.

Generalized Theory of Gravitation

1 January 1948 ยท Princeton ยท United States of America ยท Physics

Publishes a generalized theory of gravitation in Reviews of Modern Physics, presenting another stage of his sustained search for a unified geometric field theory.

Autobiographical Notes

1949 ยท Princeton ยท United States of America ยท Physics

Publishes Autobiographical Notes, reflecting on the development of his scientific ideas and philosophy.

Autobiographical Relativity Reconstruction

1949 ยท Princeton ยท United States of America ยท Physics

In his Autobiographical Notes, reconstructs the intellectual path from special relativity through the equivalence principle to general relativity and later unified-field research.

Later Unified Field Review

1950 ยท Princeton ยท United States of America ยท Physics

Presents and revises his mature attempts to construct a unified classical field theory.

Out of My Later Years

1950 ยท Princeton ยท United States of America ยท Physics

Publishes a collection of essays on science, society, philosophy and public affairs.

Revised English Relativity Edition

1950 ยท Princeton ยท United States of America ยท Physics

A revised English edition of his relativity exposition appears, updating the presentation of special and general relativity for a postwar scientific readership.

Scientific American Generalized Gravitation Article

1 April 1950 ยท Princeton ยท United States of America ยท Physics

Explains his latest generalized theory of gravitation in Scientific American, placing the work within his long search for a unified foundation of field physics.

Unified Field Equations Refinement

1951 ยท Princeton ยท United States of America ยท Physics

Refines asymmetric-field approaches intended to combine gravitation and electromagnetism.

Presidency of Israel Declined

18 November 1952 ยท Princeton ยท United States of America ยท Physics

Declines the offer to become president of Israel, citing lack of aptitude and experience for official duties.

Unified Field Theory Criticism Response

1953 ยท Princeton ยท United States of America ยท Physics

Publishes a response to criticism of unified field theory, defending the mathematical programme through which he hoped to extend relativistic field physics.

Asymmetric Relativistic Field Algebra

1954 ยท Princeton ยท United States of America ยท Physics

With Bruria Kaufman, studies algebraic properties of the asymmetric field in a relativistic unified theory, refining the mathematical structure of his late programme.

Einstein-Kaufman General Relativistic Equations

1955 ยท Princeton ยท United States of America ยท Physics

With Bruria Kaufman, develops a new form of general relativistic field equations, one of the final technical products of Einstein's lifelong geometric programme.

Death of Albert Einstein

18 April 1955 ยท Princeton ยท United States of America ยท Physics

Albert Einstein dies in Princeton, New Jersey, aged 76.