Migdal–Watson approach to final-state interactions
E1062837
UNEXPLORED
The Migdal–Watson approach to final-state interactions is a theoretical method in nuclear and particle physics that factors strong interaction effects into scattering amplitudes to describe how particles interact after the primary reaction has occurred.
All labels observed (1)
| Label | Occurrences |
|---|---|
| Migdal–Watson approach to final-state interactions canonical | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T13809666 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
NED1
Entity disambiguation (via context triple)
gpt-5-mini-2025-08-07
Target entity: Migdal–Watson approach to final-state interactions Context triple: [Arkady Migdal, knownFor, Migdal–Watson approach to final-state interactions]
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A.
Born approximation in scattering theory
The Born approximation in scattering theory is a perturbative method used in quantum mechanics to approximate scattering amplitudes by treating the interaction potential as a small perturbation to a free-particle wave.
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B.
Lippmann–Schwinger equation
The Lippmann–Schwinger equation is an integral equation in quantum scattering theory that reformulates the Schrödinger equation to describe how incoming waves are transformed into scattered waves by a potential.
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C.
The Photoproduction of Positive and Negative Pions in Hydrogen and Deuterium
"The Photoproduction of Positive and Negative Pions in Hydrogen and Deuterium" is Martin Perl’s doctoral thesis, an experimental particle physics study of how high-energy photons produce charged pions when interacting with hydrogen and deuterium targets.
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D.
Yukawa meson theory
Yukawa meson theory is an early quantum field theory that models the strong nuclear force as being mediated by massive mesons, introducing the concept of a short-range Yukawa potential between nucleons.
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E.
Sakata model of hadrons
The Sakata model of hadrons is an early composite model in particle physics that treated hadrons as bound states of a few fundamental baryons, serving as a precursor to the quark model.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
NED2
Entity disambiguation (via description)
gpt-5-mini-2025-08-07
Target entity: Migdal–Watson approach to final-state interactions Target entity description: The Migdal–Watson approach to final-state interactions is a theoretical method in nuclear and particle physics that factors strong interaction effects into scattering amplitudes to describe how particles interact after the primary reaction has occurred.
-
A.
Born approximation in scattering theory
The Born approximation in scattering theory is a perturbative method used in quantum mechanics to approximate scattering amplitudes by treating the interaction potential as a small perturbation to a free-particle wave.
-
B.
Lippmann–Schwinger equation
The Lippmann–Schwinger equation is an integral equation in quantum scattering theory that reformulates the Schrödinger equation to describe how incoming waves are transformed into scattered waves by a potential.
-
C.
The Photoproduction of Positive and Negative Pions in Hydrogen and Deuterium
"The Photoproduction of Positive and Negative Pions in Hydrogen and Deuterium" is Martin Perl’s doctoral thesis, an experimental particle physics study of how high-energy photons produce charged pions when interacting with hydrogen and deuterium targets.
-
D.
Yukawa meson theory
Yukawa meson theory is an early quantum field theory that models the strong nuclear force as being mediated by massive mesons, introducing the concept of a short-range Yukawa potential between nucleons.
-
E.
Sakata model of hadrons
The Sakata model of hadrons is an early composite model in particle physics that treated hadrons as bound states of a few fundamental baryons, serving as a precursor to the quark model.
- F. None of above. chosen
Referenced by (1)
Full triples — surface form annotated when it differs from this entity's canonical label.