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{{Short description|Concept in quantum mechanics}}
{{Short description|Concept in quantum mechanics}}


{{Quantum book backlink|Conceptual and interpretations}}
{{Quantum book backlink|Conceptual and interpretations}}
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'''Wave–particle duality''' is the concept in [[Physics:Quantum mechanics|quantum mechanics]] that quantum entities exhibit particle-like or wave-like properties depending on the experimental circumstances.<ref name="Messiah">{{cite book | last=Messiah | first=Albert | title=Quantum Mechanics | publisher=North Holland, John Wiley & Sons | date=1966 | isbn=0486409244 | url=https://archive.org/details/quantummechanics0000mess/quantummechanics0000mess }}</ref><ref name="FeynmanIII">{{cite book | last1=Feynman | first1=Richard P. | last2=Leighton | first2=Robert B. | last3=Sands | first3=Matthew L. | title=The Feynman Lectures on Physics, Volume III: Quantum Mechanics | publisher=Addison-Wesley | date=2007 | isbn=978-0-201-02118-9 | url=https://www.feynmanlectures.caltech.edu/III_toc.html }}</ref> It expresses the failure of purely classical categories such as ‘‘particle’’ and ‘‘wave’’ to give a complete description of quantum objects.<ref name="Messiah" /><ref name="FeynmanIII" />
'''Wave–particle duality''' is the concept in [[Physics:Quantum mechanics|quantum mechanics]] that quantum entities exhibit particle-like or wave-like properties depending on the experimental circumstances.<ref name="Messiah">{{cite book | last=Messiah | first=Albert | title=Quantum Mechanics | publisher=North Holland, John Wiley & Sons | date=1966 | isbn=0486409244 | url=https://archive.org/details/quantummechanics0000mess/quantummechanics0000mess }}</ref><ref name="FeynmanIII">{{cite book | last1=Feynman | first1=Richard P. | last2=Leighton | first2=Robert B. | last3=Sands | first3=Matthew L. | title=The Feynman Lectures on Physics, Volume III: Quantum Mechanics | publisher=Addison-Wesley | date=2007 | isbn=978-0-201-02118-9 | url=https://www.feynmanlectures.caltech.edu/III_toc.html }}</ref> It expresses the failure of purely classical categories such as ‘‘particle’’ and ‘‘wave’’ to give a complete description of quantum objects.<ref name="Messiah" /><ref name="FeynmanIII" />


During the 19th and early 20th centuries, light was first understood as a wave and later shown to possess a particulate character, while electrons were initially treated as particles and later found to exhibit diffraction and interference. The term ''wave–particle duality'' arose to describe these apparently contradictory behaviors.
During the 19th and early 20th centuries, light was first understood as a wave and later shown to possess a particulate character, while electrons were initially treated as particles and later found to exhibit diffraction and interference. The term ''wave–particle duality'' arose to describe these apparently contradictory behaviors.
[[File:Double slit yellow.jpg|thumb|400px|Wave–particle duality in an electron double-slit experiment: electrons arrive as localized impacts, yet build up an interference pattern characteristic of waves.<ref name="Bach2013">{{cite journal | last1=Bach | first1=Roger | last2=Pope | first2=Damian | last3=Liou | first3=Sy-Hwang | last4=Batelaan | first4=Herman | title=Controlled double-slit electron diffraction | journal=New Journal of Physics | publisher=IOP Publishing | volume=15 | issue=3 | date=2013-03-13 | issn=1367-2630 | doi=10.1088/1367-2630/15/3/033018 | page=033018 | arxiv=1210.6243 | bibcode=2013NJPh...15c3018B | s2cid=832961 | url=https://iopscience.iop.org/article/10.1088/1367-2630/15/3/033018 }}</ref>]]
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[[File:Double slit yellow.jpg|thumb|280px|Quantum Wave–particle duality.]]
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== History ==
== History ==
In the late 17th century, [[Biography:Isaac Newton|Isaac Newton]] argued that light consisted of particles, whereas [[Biography:Christiaan Huygens|Christiaan Huygens]] proposed a wave theory of light.<ref>{{cite book | last=Huygens | first=Christiaan | title=Traité de la lumiere | publisher=Pieter van der Aa | location=Leiden | date=1690 }}</ref> In the early 19th century, [[Biography:Thomas Young (scientist)|Thomas Young]]'s interference experiments and [[Biography:François Arago|François Arago]]'s observation of the Poisson spot strongly supported the wave picture of light.
In the late 17th century, Isaac Newton argued that light consisted of particles, whereas Christiaan Huygens proposed a wave theory of light.<ref>{{cite book | last=Huygens | first=Christiaan | title=Traité de la lumiere | publisher=Pieter van der Aa | location=Leiden | date=1690 }}</ref> In the early 19th century, Thomas Young's interference experiments and François Arago's observation of the Poisson spot strongly supported the wave picture of light.


That picture was challenged by [[Physics:Planck's law|Planck's law]] for [[Astronomy:Black-body radiation|black-body radiation]], which required energy exchange in discrete quanta.<ref name="Planck1901">{{cite journal | last=Planck | first=Max | title=Ueber das Gesetz der Energieverteilung im Normalspectrum | journal=Annalen der Physik | volume=309 | issue=3 | pages=553–563 | date=1901 | language=de | doi=10.1002/andp.19013090310 | doi-access=free }}</ref> In 1905, [[Biography:Albert Einstein|Albert Einstein]] interpreted the [[Physics:Photoelectric effect|photoelectric effect]] using discrete light quanta, later called photons.<ref name="Einstein1905">{{cite journal | last=Einstein | first=Albert | title=Über einen die Erzeugung und Verwandlung des Lichtes betreffenden heuristischen Gesichtspunkt | journal=Annalen der Physik | volume=17 | issue=6 | pages=132–148 | date=1905 | doi=10.1002/andp.19053220607 | doi-access=free }}</ref> The case for particle-like light was greatly strengthened by [[Biography:Arthur Compton|Arthur Compton]]'s measurements of photon momentum in scattering experiments.<ref name="Whittaker2">{{cite book | last=Whittaker | first=Edmund T. | title=A history of the theories of aether & electricity. 2: The modern theories, 1900–1926 | publisher=Dover Publications | location=New York | date=1989 | isbn=978-0-486-26126-3 }}</ref>
That picture was challenged by Planck's law for black-body radiation, which required energy exchange in discrete quanta.<ref name="Planck1901">{{cite journal | last=Planck | first=Max | title=Ueber das Gesetz der Energieverteilung im Normalspectrum | journal=Annalen der Physik | volume=309 | issue=3 | pages=553–563 | date=1901 | language=de | doi=10.1002/andp.19013090310 | doi-access=free }}</ref> In 1905, [[Biography:Albert Einstein|Albert Einstein]] interpreted the photoelectric effect using discrete light quanta, later called photons.<ref name="Einstein1905">{{cite journal | last=Einstein | first=Albert | title=Über einen die Erzeugung und Verwandlung des Lichtes betreffenden heuristischen Gesichtspunkt | journal=Annalen der Physik | volume=17 | issue=6 | pages=132–148 | date=1905 | doi=10.1002/andp.19053220607 | doi-access=free }}</ref> The case for particle-like light was greatly strengthened by Arthur Compton's measurements of photon momentum in scattering experiments.<ref name="Whittaker2">{{cite book | last=Whittaker | first=Edmund T. | title=A history of the theories of aether & electricity. 2: The modern theories, 1900–1926 | publisher=Dover Publications | location=New York | date=1989 | isbn=978-0-486-26126-3 }}</ref>


For electrons, the historical sequence was reversed. Their charge-to-mass ratio and trajectories in electromagnetic fields supported a particle picture.<ref name="Thomson1897">{{cite journal | last=Thomson | first=J. J. | title=XL. Cathode Rays | journal=The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science | volume=44 | issue=269 | pages=293–316 | date=1897 | doi=10.1080/14786449708621070 }}</ref> In 1924, [[Biography:Louis de Broglie|Louis de Broglie]] proposed that matter has an associated wavelength, relating a particle’s momentum to a wave description.<ref name="Broglie">{{cite web | last=de Broglie | first=Louis Victor | title=On the Theory of Quanta | url=https://fondationlouisdebroglie.org/LDB-oeuvres/De_Broglie_Kracklauer.pdf | website=Foundation of Louis de Broglie }}</ref> This idea rapidly led to wave mechanics and the [[Physics:Schrödinger equation|Schrödinger equation]].<ref name="Schrodinger1926">{{cite journal | last=Schrödinger | first=E. | title=An Undulatory Theory of the Mechanics of Atoms and Molecules | journal=Physical Review | volume=28 | issue=6 | pages=1049–1070 | date=1926 | doi=10.1103/PhysRev.28.1049 | bibcode=1926PhRv...28.1049S }}</ref>
For electrons, the historical sequence was reversed. Their charge-to-mass ratio and trajectories in electromagnetic fields supported a particle picture.<ref name="Thomson1897">{{cite journal | last=Thomson | first=J. J. | title=XL. Cathode Rays | journal=The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science | volume=44 | issue=269 | pages=293–316 | date=1897 | doi=10.1080/14786449708621070 }}</ref> In 1924, Louis de Broglie proposed that matter has an associated wavelength, relating a particle’s momentum to a wave description.<ref name="Broglie">{{cite web | last=de Broglie | first=Louis Victor | title=On the Theory of Quanta | url=https://fondationlouisdebroglie.org/LDB-oeuvres/De_Broglie_Kracklauer.pdf | website=Foundation of Louis de Broglie }}</ref> This idea rapidly led to wave mechanics and the Schrödinger equation.<ref name="Schrodinger1926">{{cite journal | last=Schrödinger | first=E. | title=An Undulatory Theory of the Mechanics of Atoms and Molecules | journal=Physical Review | volume=28 | issue=6 | pages=1049–1070 | date=1926 | doi=10.1103/PhysRev.28.1049 | bibcode=1926PhRv...28.1049S }}</ref>


Experimental confirmation soon followed in the [[Physics:Davisson–Germer experiment|Davisson–Germer experiment]] and in the diffraction experiments of [[Biography:George Paget Thomson|George Paget Thomson]] and Alexander Reid, showing that electrons produce diffraction patterns characteristic of waves.<ref name="DG1927">{{cite journal | last1=Davisson | first1=C. | last2=Germer | first2=L. H. | title=Diffraction of Electrons by a Crystal of Nickel | journal=Physical Review | volume=30 | issue=6 | pages=705–740 | date=1927 | doi=10.1103/PhysRev.30.705 | doi-access=free }}</ref><ref name="ThomsonReid1927">{{cite journal | last1=Thomson | first1=G. P. | last2=Reid | first2=A. | title=Diffraction of Cathode Rays by a Thin Film | journal=Nature | volume=119 | issue=3007 | pages=890 | date=1927 | doi=10.1038/119890a0 | doi-access=free }}</ref>
Experimental confirmation soon followed in the Davisson–Germer experiment and in the diffraction experiments of George Paget Thomson and Alexander Reid, showing that electrons produce diffraction patterns characteristic of waves.<ref name="DG1927">{{cite journal | last1=Davisson | first1=C. | last2=Germer | first2=L. H. | title=Diffraction of Electrons by a Crystal of Nickel | journal=Physical Review | volume=30 | issue=6 | pages=705–740 | date=1927 | doi=10.1103/PhysRev.30.705 | doi-access=free }}</ref><ref name="ThomsonReid1927">{{cite journal | last1=Thomson | first1=G. P. | last2=Reid | first2=A. | title=Diffraction of Cathode Rays by a Thin Film | journal=Nature | volume=119 | issue=3007 | pages=890 | date=1927 | doi=10.1038/119890a0 | doi-access=free }}</ref>


== Classical waves and particles ==
== Classical waves and particles ==
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| image1      = Rippletanksource1plus2superpositionBnW.png
| image1      = Rippletanksource1plus2superpositionBnW.png
| alt1        = Wave interference in water due to two sources
| alt1        = Wave interference in water due to two sources
| caption1    = [[Physics:Wave interference|Wave interference]] in water from two sources.
| caption1    = Wave interference in water from two sources.
| image2      = Inclinedthrow.gif
| image2      = Inclinedthrow.gif
| caption2    = Classical trajectories for a mass thrown at an angle.
| caption2    = Classical trajectories for a mass thrown at an angle.
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| image4      = PositronDiscovery.png
| image4      = PositronDiscovery.png
| alt4        = Curved arc in a cloud chamber
| alt4        = Curved arc in a cloud chamber
| caption4    = A [[Physics:Cloud chamber|cloud chamber]] track of a [[Physics:Positron|positron]], showing particle-like motion.
| caption4    = A cloud chamber track of a positron, showing particle-like motion.
| footer      = '''Quantum systems exhibit both interference and localized detection events.'''
| footer      = '''Quantum systems exhibit both interference and localized detection events.'''
}}
}}
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== Observing photons as particles ==
== Observing photons as particles ==
For photons, the historical path ran in the opposite direction. Light was long understood as a wave, but the [[Physics:Photoelectric effect|photoelectric effect]] showed that energy transfer from light to matter occurs in discrete units.<ref name="Whittaker1">{{cite book | last=Whittaker | first=E. T. | title=A History of the Theories of Aether and Electricity: From the Age of Descartes to the Close of the Nineteenth Century | publisher=Longman, Green and Co. | date=1910 }}</ref><ref>{{cite journal | last=Wheaton | first=Bruce R. | title=Philipp Lenard and the Photoelectric Effect, 1889-1911 | journal=Historical Studies in the Physical Sciences | volume=9 | pages=299–322 | date=1978 | doi=10.2307/27757381 | jstor=27757381 }}</ref> Einstein proposed that light of frequency <math>f</math> is absorbed or emitted in quanta of energy
For photons, the historical path ran in the opposite direction. Light was long understood as a wave, but the photoelectric effect showed that energy transfer from light to matter occurs in discrete units.<ref name="Whittaker1">{{cite book | last=Whittaker | first=E. T. | title=A History of the Theories of Aether and Electricity: From the Age of Descartes to the Close of the Nineteenth Century | publisher=Longman, Green and Co. | date=1910 }}</ref><ref>{{cite journal | last=Wheaton | first=Bruce R. | title=Philipp Lenard and the Photoelectric Effect, 1889-1911 | journal=Historical Studies in the Physical Sciences | volume=9 | pages=299–322 | date=1978 | doi=10.2307/27757381 | jstor=27757381 }}</ref> Einstein proposed that light of frequency <math>f</math> is absorbed or emitted in quanta of energy


:<math>E = hf</math>
:<math>E = hf</math>


where <math>h</math> is the [[Physics:Planck constant|Planck constant]].<ref name="Einstein1905" /> This relation explains why electrons are emitted only when the photon frequency exceeds a threshold set by the material’s [[Physics:Work function|work function]]. Increasing the light intensity below that threshold does not liberate electrons, whereas increasing the photon frequency above threshold increases the maximum kinetic energy of emitted electrons.
where <math>h</math> is the Planck constant.<ref name="Einstein1905" /> This relation explains why electrons are emitted only when the photon frequency exceeds a threshold set by the material’s work function. Increasing the light intensity below that threshold does not liberate electrons, whereas increasing the photon frequency above threshold increases the maximum kinetic energy of emitted electrons.


Further evidence for photon-like behavior came from [[Physics:Compton scattering|Compton scattering]], where X-rays exchange momentum with electrons in a way consistent with particle collisions.<ref name="Whittaker2" /> Thus light exhibits interference and diffraction characteristic of waves, while also carrying discrete energy and momentum characteristic of particles.
Further evidence for photon-like behavior came from Compton scattering, where X-rays exchange momentum with electrons in a way consistent with particle collisions.<ref name="Whittaker2" /> Thus light exhibits interference and diffraction characteristic of waves, while also carrying discrete energy and momentum characteristic of particles.


[[File:Photoelectric_effect_in_a_solid_-_diagram.svg|thumb|400px|The photoelectric effect demonstrates the quantized transfer of energy from light to matter.]]
[[File:Photoelectric_effect_in_a_solid_-_diagram.svg|thumb|400px|The photoelectric effect demonstrates the quantized transfer of energy from light to matter.]]
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== Duality with other properties ==
== Duality with other properties ==
Wave–particle duality is part of a broader quantum pattern in which classical attributes do not remain cleanly separated. [[Physics:Angular momentum|Angular momentum]], for example, is often pictured as a particle-like quantity, but electromagnetic waves can carry orbital angular momentum when arranged in vortex beams.<ref>{{cite journal | last1=Allen | first1=L. | last2=Beijersbergen | first2=M. W. | last3=Spreeuw | first3=R. J. C. | last4=Woerdman | first4=J. P. | title=Orbital angular momentum of light and the transformation of Laguerre-Gaussian laser modes | journal=Physical Review A | volume=45 | issue=11 | pages=8185–8189 | date=1992 | doi=10.1103/PhysRevA.45.8185 | pmid=9906912 }}</ref> Likewise, electron waves can be prepared with large orbital angular momentum and still display diffraction, interference, and magnetic interactions associated with particle properties.<ref>{{cite journal | last1=Verbeeck | first1=J. | last2=Tian | first2=H. | last3=Schattschneider | first3=P. | title=Production and application of electron vortex beams | journal=Nature | volume=467 | issue=7313 | pages=301–304 | date=2010 | doi=10.1038/nature09366 | pmid=20844532 | s2cid=2970408 }}</ref><ref>{{cite journal | last1=Tavabi | first1=A. H. | last2=Rosi | first2=P. | last3=Roncaglia | first3=A. | last4=Rotunno | first4=E. | last5=Beleggia | first5=M. | last6=Lu | first6=P.-H. | last7=Belsito | first7=L. | last8=Pozzi | first8=G. | last9=Frabboni | first9=S. | last10=Tiemeijer | first10=P. | last11=Dunin-Borkowski | first11=R. E. | last12=Grillo | first12=V. | title=Generation of electron vortex beams with over 1000 orbital angular momentum quanta using a tunable electrostatic spiral phase plate | journal=Applied Physics Letters | volume=121 | issue=7 | date=2022 | doi=10.1063/5.0093411 | arxiv=2203.00477 | s2cid=247187983 }}</ref>
Wave–particle duality is part of a broader quantum pattern in which classical attributes do not remain cleanly separated. Angular momentum, for example, is often pictured as a particle-like quantity, but electromagnetic waves can carry orbital angular momentum when arranged in vortex beams.<ref>{{cite journal | last1=Allen | first1=L. | last2=Beijersbergen | first2=M. W. | last3=Spreeuw | first3=R. J. C. | last4=Woerdman | first4=J. P. | title=Orbital angular momentum of light and the transformation of Laguerre-Gaussian laser modes | journal=Physical Review A | volume=45 | issue=11 | pages=8185–8189 | date=1992 | doi=10.1103/PhysRevA.45.8185 | pmid=9906912 }}</ref> Likewise, electron waves can be prepared with large orbital angular momentum and still display diffraction, interference, and magnetic interactions associated with particle properties.<ref>{{cite journal | last1=Verbeeck | first1=J. | last2=Tian | first2=H. | last3=Schattschneider | first3=P. | title=Production and application of electron vortex beams | journal=Nature | volume=467 | issue=7313 | pages=301–304 | date=2010 | doi=10.1038/nature09366 | pmid=20844532 | s2cid=2970408 }}</ref><ref>{{cite journal | last1=Tavabi | first1=A. H. | last2=Rosi | first2=P. | last3=Roncaglia | first3=A. | last4=Rotunno | first4=E. | last5=Beleggia | first5=M. | last6=Lu | first6=P.-H. | last7=Belsito | first7=L. | last8=Pozzi | first8=G. | last9=Frabboni | first9=S. | last10=Tiemeijer | first10=P. | last11=Dunin-Borkowski | first11=R. E. | last12=Grillo | first12=V. | title=Generation of electron vortex beams with over 1000 orbital angular momentum quanta using a tunable electrostatic spiral phase plate | journal=Applied Physics Letters | volume=121 | issue=7 | date=2022 | doi=10.1063/5.0093411 | arxiv=2203.00477 | s2cid=247187983 }}</ref>


[[File:Focused Laguerre-Gaussian beam.webm|thumb|400px|A focused Laguerre–Gaussian beam carrying orbital angular momentum.]]
[[File:Quantum_book1_wave_particle_duality_yellow.png|thumb|400px|A focused Laguerre–Gaussian beam carrying orbital angular momentum.]]


== Which-slit experiments ==
== Which-slit experiments ==
In “which-slit” or “which-way” experiments, detectors are placed so that the path taken by a quantum particle can be inferred. Quantum mechanics predicts that when path information becomes available, the interference pattern disappears because coherence between the alternatives is lost.<ref name="FeynmanIII" /> Many realizations of this idea, including delayed-choice experiments, confirm the same principle: path information and interference visibility are mutually constrained.<ref>{{cite journal | last1=Ma | first1=Xiao-song | last2=Kofler | first2=Johannes | last3=Zeilinger | first3=Anton | title=Delayed-choice gedanken experiments and their realizations | journal=Reviews of Modern Physics | volume=88 | issue=1 | page=015005 | date=2016 | doi=10.1103/RevModPhys.88.015005 | arxiv=1407.2930 | s2cid=34901303 }}</ref>
In “which-slit” or “which-way” experiments, detectors are placed so that the path taken by a quantum particle can be inferred. Quantum mechanics predicts that when path information becomes available, the interference pattern disappears because coherence between the alternatives is lost.<ref name="FeynmanIII" /> Many realizations of this idea, including delayed-choice experiments, confirm the same principle: path information and interference visibility are mutually constrained.<ref>{{cite journal | last1=Ma | first1=Xiao-song | last2=Kofler | first2=Johannes | last3=Zeilinger | first3=Anton | title=Delayed-choice gedanken experiments and their realizations | journal=Reviews of Modern Physics | volume=88 | issue=1 | page=015005 | date=2016 | doi=10.1103/RevModPhys.88.015005 | arxiv=1407.2930 | s2cid=34901303 }}</ref>


A standard optical realization uses a [[Physics:Mach–Zehnder interferometer|Mach–Zehnder interferometer]]. A beam is split into two paths and later recombined. When the second beam splitter is present, the outputs depend on interference between the two paths. When it is removed, each output reveals path information and the interference effect vanishes.<ref>{{cite journal | last1=Schneider | first1=Mark B. | last2=LaPuma | first2=Indhira A. | title=A simple experiment for discussion of quantum interference and which-way measurement | journal=American Journal of Physics | volume=70 | issue=3 | pages=266–271 | date=2002 | doi=10.1119/1.1450558 | url=https://digital.grinnell.edu/islandora/object/grinnell%3A47/datastream/OBJ/download/A_Simple_Experiment_for_Discussion_of_Quantum_Interference_and_Which-Way_Measurement.pdf }}</ref>
A standard optical realization uses a Mach–Zehnder interferometer. A beam is split into two paths and later recombined. When the second beam splitter is present, the outputs depend on interference between the two paths. When it is removed, each output reveals path information and the interference effect vanishes.<ref>{{cite journal | last1=Schneider | first1=Mark B. | last2=LaPuma | first2=Indhira A. | title=A simple experiment for discussion of quantum interference and which-way measurement | journal=American Journal of Physics | volume=70 | issue=3 | pages=266–271 | date=2002 | doi=10.1119/1.1450558 | url=https://digital.grinnell.edu/islandora/object/grinnell%3A47/datastream/OBJ/download/A_Simple_Experiment_for_Discussion_of_Quantum_Interference_and_Which-Way_Measurement.pdf }}</ref>


[[File:Mach Zehnder interferometer schematic diagram.jpg|thumb|400px|A Mach–Zehnder interferometer illustrates the relation between path information and interference.]]
[[File:Mach Zehnder interferometer schematic diagram.jpg|thumb|400px|A Mach–Zehnder interferometer illustrates the relation between path information and interference.]]

Latest revision as of 12:22, 20 May 2026



← Back to Conceptual and interpretations
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Next : Complementarity principle →

Wave–particle duality is the concept in quantum mechanics that quantum entities exhibit particle-like or wave-like properties depending on the experimental circumstances.[1][2] It expresses the failure of purely classical categories such as ‘‘particle’’ and ‘‘wave’’ to give a complete description of quantum objects.[1][2]

During the 19th and early 20th centuries, light was first understood as a wave and later shown to possess a particulate character, while electrons were initially treated as particles and later found to exhibit diffraction and interference. The term wave–particle duality arose to describe these apparently contradictory behaviors.

Quantum Wave–particle duality.

History

In the late 17th century, Isaac Newton argued that light consisted of particles, whereas Christiaan Huygens proposed a wave theory of light.[3] In the early 19th century, Thomas Young's interference experiments and François Arago's observation of the Poisson spot strongly supported the wave picture of light.

That picture was challenged by Planck's law for black-body radiation, which required energy exchange in discrete quanta.[4] In 1905, Albert Einstein interpreted the photoelectric effect using discrete light quanta, later called photons.[5] The case for particle-like light was greatly strengthened by Arthur Compton's measurements of photon momentum in scattering experiments.[6]

For electrons, the historical sequence was reversed. Their charge-to-mass ratio and trajectories in electromagnetic fields supported a particle picture.[7] In 1924, Louis de Broglie proposed that matter has an associated wavelength, relating a particle’s momentum to a wave description.[8] This idea rapidly led to wave mechanics and the Schrödinger equation.[9]

Experimental confirmation soon followed in the Davisson–Germer experiment and in the diffraction experiments of George Paget Thomson and Alexander Reid, showing that electrons produce diffraction patterns characteristic of waves.[10][11]

Classical waves and particles

In classical physics, waves and particles are distinct models with different mathematical descriptions. Classical waves obey wave equations, extend through space, diffract, and interfere. Examples include water waves, sound waves, and radio waves. Classical particles follow trajectories specified by position and velocity, and in the absence of forces they move in straight lines. Planets, sand grains, and bullets are well described by particle models.

Quantum systems do not fit neatly into either classical category. The wavefunction evolves according to a wave equation, but measurements yield discrete detection events associated with particles. The probability of finding a quantum object at a given location is determined by the squared magnitude of a complex probability amplitude.[1] Thus many repeated particle detections can build up an interference pattern that reflects wave-like evolution.

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Electrons behaving as waves and particles

The electron double-slit experiment is one of the clearest demonstrations of wave–particle duality.[2][12] Electrons emitted toward two narrow slits form a diffraction pattern when one slit is open and an interference pattern when both slits are open. At high intensity the detector records a smooth pattern, but when the beam intensity is reduced so that electrons arrive one at a time, each detection appears as an individual localized dot. Over time, those dots accumulate into the same interference pattern predicted by wave mechanics.[12]

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This combination of localized impacts and wave-like interference is not limited to electrons. Comparable interference has been demonstrated for atoms and large molecules, showing that wave–particle duality is a general feature of quantum matter.[13]

Observing photons as particles

For photons, the historical path ran in the opposite direction. Light was long understood as a wave, but the photoelectric effect showed that energy transfer from light to matter occurs in discrete units.[14][15] Einstein proposed that light of frequency f is absorbed or emitted in quanta of energy

E=hf

where h is the Planck constant.[5] This relation explains why electrons are emitted only when the photon frequency exceeds a threshold set by the material’s work function. Increasing the light intensity below that threshold does not liberate electrons, whereas increasing the photon frequency above threshold increases the maximum kinetic energy of emitted electrons.

Further evidence for photon-like behavior came from Compton scattering, where X-rays exchange momentum with electrons in a way consistent with particle collisions.[6] Thus light exhibits interference and diffraction characteristic of waves, while also carrying discrete energy and momentum characteristic of particles.

The photoelectric effect demonstrates the quantized transfer of energy from light to matter.
In Compton scattering, a photon transfers momentum to a target, displaying particle-like behavior.

Duality with other properties

Wave–particle duality is part of a broader quantum pattern in which classical attributes do not remain cleanly separated. Angular momentum, for example, is often pictured as a particle-like quantity, but electromagnetic waves can carry orbital angular momentum when arranged in vortex beams.[16] Likewise, electron waves can be prepared with large orbital angular momentum and still display diffraction, interference, and magnetic interactions associated with particle properties.[17][18]

A focused Laguerre–Gaussian beam carrying orbital angular momentum.

Which-slit experiments

In “which-slit” or “which-way” experiments, detectors are placed so that the path taken by a quantum particle can be inferred. Quantum mechanics predicts that when path information becomes available, the interference pattern disappears because coherence between the alternatives is lost.[2] Many realizations of this idea, including delayed-choice experiments, confirm the same principle: path information and interference visibility are mutually constrained.[19]

A standard optical realization uses a Mach–Zehnder interferometer. A beam is split into two paths and later recombined. When the second beam splitter is present, the outputs depend on interference between the two paths. When it is removed, each output reveals path information and the interference effect vanishes.[20]

A Mach–Zehnder interferometer illustrates the relation between path information and interference.

Significance

Wave–particle duality does not mean that quantum objects alternate between being literal classical waves and literal classical particles. Rather, quantum theory assigns them a state described by a wavefunction or probability amplitude, while measurements yield discrete outcomes associated with quanta. The apparent duality reflects the limits of classical language and the need for a distinctly quantum description.[1][2]

See also

Table of contents (198 articles)

Index

Full contents

9. Quantum optics and experiments (5) Back to index
Experimental quantum physics: qubits, dilution refrigerators, quantum communication, and laboratory systems.
Experimental quantum physics: qubits, dilution refrigerators, quantum communication, and laboratory systems.
14. Plasma and fusion physics (8) Back to index
Conceptual illustration of plasma physics in a fusion context, showing magnetically confined ionized gas in a tokamak and the collective behavior governed by electromagnetic fields and transport processes.
Conceptual illustration of plasma physics in a fusion context, showing magnetically confined ionized gas in a tokamak and the collective behavior governed by electromagnetic fields and transport processes.

References

  1. ↑ 1.0 1.1 1.2 1.3 Messiah, Albert (1966). Quantum Mechanics. North Holland, John Wiley & Sons. ISBN 0486409244. https://archive.org/details/quantummechanics0000mess/quantummechanics0000mess. 
  2. ↑ 2.0 2.1 2.2 2.3 2.4 Feynman, Richard P.; Leighton, Robert B.; Sands, Matthew L. (2007). The Feynman Lectures on Physics, Volume III: Quantum Mechanics. Addison-Wesley. ISBN 978-0-201-02118-9. https://www.feynmanlectures.caltech.edu/III_toc.html. 
  3. ↑ Huygens, Christiaan (1690). Traité de la lumiere. Leiden: Pieter van der Aa. 
  4. ↑ Planck, Max (1901). "Ueber das Gesetz der Energieverteilung im Normalspectrum" (in de). Annalen der Physik 309 (3): 553–563. doi:10.1002/andp.19013090310. 
  5. ↑ 5.0 5.1 Einstein, Albert (1905). "Über einen die Erzeugung und Verwandlung des Lichtes betreffenden heuristischen Gesichtspunkt". Annalen der Physik 17 (6): 132–148. doi:10.1002/andp.19053220607. 
  6. ↑ 6.0 6.1 Whittaker, Edmund T. (1989). A history of the theories of aether & electricity. 2: The modern theories, 1900–1926. New York: Dover Publications. ISBN 978-0-486-26126-3. 
  7. ↑ Thomson, J. J. (1897). "XL. Cathode Rays". The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science 44 (269): 293–316. doi:10.1080/14786449708621070. 
  8. ↑ de Broglie, Louis Victor. "On the Theory of Quanta". https://fondationlouisdebroglie.org/LDB-oeuvres/De_Broglie_Kracklauer.pdf. 
  9. ↑ Schrödinger, E. (1926). "An Undulatory Theory of the Mechanics of Atoms and Molecules". Physical Review 28 (6): 1049–1070. doi:10.1103/PhysRev.28.1049. Bibcode: 1926PhRv...28.1049S. 
  10. ↑ Davisson, C.; Germer, L. H. (1927). "Diffraction of Electrons by a Crystal of Nickel". Physical Review 30 (6): 705–740. doi:10.1103/PhysRev.30.705. 
  11. ↑ Thomson, G. P.; Reid, A. (1927). "Diffraction of Cathode Rays by a Thin Film". Nature 119 (3007): 890. doi:10.1038/119890a0. 
  12. ↑ 12.0 12.1 Cite error: Invalid <ref> tag; no text was provided for refs named Bach2013
  13. ↑ Arndt, Markus; Hornberger, Klaus (2014). "Testing the limits of quantum mechanical superpositions". Nature Physics 10 (4): 271–277. doi:10.1038/nphys2863. 
  14. ↑ Whittaker, E. T. (1910). A History of the Theories of Aether and Electricity: From the Age of Descartes to the Close of the Nineteenth Century. Longman, Green and Co.. 
  15. ↑ Wheaton, Bruce R. (1978). "Philipp Lenard and the Photoelectric Effect, 1889-1911". Historical Studies in the Physical Sciences 9: 299–322. doi:10.2307/27757381. 
  16. ↑ Allen, L.; Beijersbergen, M. W.; Spreeuw, R. J. C.; Woerdman, J. P. (1992). "Orbital angular momentum of light and the transformation of Laguerre-Gaussian laser modes". Physical Review A 45 (11): 8185–8189. doi:10.1103/PhysRevA.45.8185. PMID 9906912. 
  17. ↑ Verbeeck, J.; Tian, H.; Schattschneider, P. (2010). "Production and application of electron vortex beams". Nature 467 (7313): 301–304. doi:10.1038/nature09366. PMID 20844532. 
  18. ↑ Tavabi, A. H.; Rosi, P.; Roncaglia, A.; Rotunno, E.; Beleggia, M.; Lu, P.-H.; Belsito, L.; Pozzi, G. et al. (2022). "Generation of electron vortex beams with over 1000 orbital angular momentum quanta using a tunable electrostatic spiral phase plate". Applied Physics Letters 121 (7). doi:10.1063/5.0093411. 
  19. ↑ Ma, Xiao-song; Kofler, Johannes; Zeilinger, Anton (2016). "Delayed-choice gedanken experiments and their realizations". Reviews of Modern Physics 88 (1): 015005. doi:10.1103/RevModPhys.88.015005. 
  20. ↑ Schneider, Mark B.; LaPuma, Indhira A. (2002). "A simple experiment for discussion of quantum interference and which-way measurement". American Journal of Physics 70 (3): 266–271. doi:10.1119/1.1450558. https://digital.grinnell.edu/islandora/object/grinnell%3A47/datastream/OBJ/download/A_Simple_Experiment_for_Discussion_of_Quantum_Interference_and_Which-Way_Measurement.pdf. 


Author: Harold Foppele

Source attribution: Physics:Quantum Wave–particle duality

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