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Page 400
... mass , the mass difference is AM = m „ 0 135.0 Mev , while the target mass is m2 = m , 938.5 Mev . Then the = threshold energy is Tth = 135.01 + 135.0 2 ( 938.5 ) = 135.0 ( 1.072 ) = 144.7 Mev As another example consider the production ...
... mass , the mass difference is AM = m „ 0 135.0 Mev , while the target mass is m2 = m , 938.5 Mev . Then the = threshold energy is Tth = 135.01 + 135.0 2 ( 938.5 ) = 135.0 ( 1.072 ) = 144.7 Mev As another example consider the production ...
Page 590
... mass merely appears as an added coefficient of the acceleration in ( 17.33 ) . 17.5 Lorentz Transformation ... mass being 2 x 137 times the electron mass , is another of these numerological coincidences which may ultimately have some ...
... mass merely appears as an added coefficient of the acceleration in ( 17.33 ) . 17.5 Lorentz Transformation ... mass being 2 x 137 times the electron mass , is another of these numerological coincidences which may ultimately have some ...
Page 623
... Mass . ( 1951 ) . Electrodynamics of Continuous Media , Addison - Wesley , Reading , Mass . ( 1960 ) . Lighthill , M. J. , Introduction to Fourier Analysis and Generalized Functions , Cambridge University Press ( 1958 ) . Linhart ...
... Mass . ( 1951 ) . Electrodynamics of Continuous Media , Addison - Wesley , Reading , Mass . ( 1960 ) . Lighthill , M. J. , Introduction to Fourier Analysis and Generalized Functions , Cambridge University Press ( 1958 ) . Linhart ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ