Please note that the content of this book primarily consists of articles available from Wikipedia or other free sources online. If two fermions interact through a Yukawa interaction with Yukawa particle mass μ, the potential between the two particles, known as the Yukawa potential, will be: V(r) = -frac{g^2}{4pi} frac{1}{r} e^{-mu r} which is the same as a Coulomb potential except for the sign and the exponential factor. The sign will make the interaction attractive between all particles (the electromagnetic interaction is repulsive for identical particles). This is explained by the fact that the Yukawa particle has spin zero and even spin always results in an attractive potential. The exponential will give the interaction a finite range, so that particles at great distances will hardly interact any longer.
"synopsis" may belong to another edition of this title.
Please note that the content of this book primarily consists of articles available from Wikipedia or other free sources online. If two fermions interact through a Yukawa interaction with Yukawa particle mass μ, the potential between the two particles, known as the Yukawa potential, will be: V(r) = -frac{g^2}{4pi} frac{1}{r} e^{-mu r} which is the same as a Coulomb potential except for the sign and the exponential factor. The sign will make the interaction attractive between all particles (the electromagnetic interaction is repulsive for identical particles). This is explained by the fact that the Yukawa particle has spin zero and even spin always results in an attractive potential. The exponential will give the interaction a finite range, so that particles at great distances will hardly interact any longer.
"About this title" may belong to another edition of this title.
Seller: BuchWeltWeit Ludwig Meier e.K., Bergisch Gladbach, Germany
Taschenbuch. Condition: Neu. This item is printed on demand - it takes 3-4 days longer - Neuware -High Quality Content by WIKIPEDIA articles! If two fermions interact through a Yukawa interaction with Yukawa particle mass , the potential between the two particles, known as the Yukawa potential, will be: V(r) = -frac{g^2}{4pi} frac{1}{r} e^{-mu r} which is the same as a Coulomb potential except for the sign and the exponential factor. The sign will make the interaction attractive between all particles (the electromagnetic interaction is repulsive for identical particles). This is explained by the fact that the Yukawa particle has spin zero and even spin always results in an attractive potential. The exponential will give the interaction a finite range, so that particles at great distances will hardly interact any longer. 60 pp. Englisch. Seller Inventory # 9786131109010
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Taschenbuch. Condition: Neu. nach der Bestellung gedruckt Neuware - Printed after ordering - High Quality Content by WIKIPEDIA articles! If two fermions interact through a Yukawa interaction with Yukawa particle mass , the potential between the two particles, known as the Yukawa potential, will be: V(r) = -frac{g^2}{4pi} frac{1}{r} e^{-mu r} which is the same as a Coulomb potential except for the sign and the exponential factor. The sign will make the interaction attractive between all particles (the electromagnetic interaction is repulsive for identical particles). This is explained by the fact that the Yukawa particle has spin zero and even spin always results in an attractive potential. The exponential will give the interaction a finite range, so that particles at great distances will hardly interact any longer. Seller Inventory # 9786131109010
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Taschenbuch. Condition: Neu. Yukawa Interaction | Particle Physics, Hideki Yukawa, Scalar Field (Quantum Field Theory), Nucleon, Strong Nuclear Force, Standard Model | Lambert M. Surhone (u. a.) | Taschenbuch | Englisch | 2026 | OmniScriptum | EAN 9786131109010 | Verantwortliche Person für die EU: preigu GmbH & Co. KG, Lengericher Landstr. 19, 49078 Osnabrück, mail[at]preigu[dot]de | Anbieter: preigu Print on Demand. Seller Inventory # 113273828
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Taschenbuch. Condition: Neu. This item is printed on demand - Print on Demand Titel. Neuware -Please note that the content of this book primarily consists of articlesavailable from Wikipedia or other free sources online. If two fermionsinteract through a Yukawa interaction with Yukawa particle mass ¿, thepotential between the two particles, known as the Yukawa potential, willbe: V(r) = -frac{g^2}{4pi} frac{1}{r} e^{-mu r} which is the same as aCoulomb potential except for the sign and the exponential factor. Thesign will make the interaction attractive between all particles (theelectromagnetic interaction is repulsive for identical particles). Thisis explained by the fact that the Yukawa particle has spin zero and evenspin always results in an attractive potential. The exponential willgive the interaction a finite range, so that particles at greatdistances will hardly interact any longer.VDM Verlag, Dudweiler Landstraße 99, 66123 Saarbrücken 60 pp. Englisch. Seller Inventory # 9786131109010
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