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Page 358
... meson of lifetime 70 at rest in the system K ' * For example , negative mu mesons can become bound in hydrogen - like orbits around nuclei with binding energies that are not negligible compared to the energy liberated in their decay ...
... meson of lifetime 70 at rest in the system K ' * For example , negative mu mesons can become bound in hydrogen - like orbits around nuclei with binding energies that are not negligible compared to the energy liberated in their decay ...
Page 359
... meson is created at the origin of K ' at time t ' = t = 0. As seen from the system K the position of the meson is given by z = vt . If it lives a time 70 in K ' , then at its instant of decay , we find t ' = - 2 = t ( 11.23 ) - The time ...
... meson is created at the origin of K ' at time t ' = t = 0. As seen from the system K the position of the meson is given by z = vt . If it lives a time 70 in K ' , then at its instant of decay , we find t ' = - 2 = t ( 11.23 ) - The time ...
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... meson , K meson , proton , etc. ) , the collisions with electrons and with nuclei have different consequences . The light electrons can take up appreciable amounts of energy from the incident particle without causing significant ...
... meson , K meson , proton , etc. ) , the collisions with electrons and with nuclei have different consequences . The light electrons can take up appreciable amounts of energy from the incident particle without causing significant ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ