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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 ' : = c2 = t ( 11.23 ) - The ...
... 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 ' : = c2 = t ( 11.23 ) - The ...
Page 394
... meson decay . 2. Charged K meson sometimes decays into two pi mesons with a lifetime T = 1.2 x 10-8 sec : K + = 135.0 Mev . Thus the The charged K meson has a rest energy M = 494 Mev , while the two pi mesons have rest energies , m ...
... meson decay . 2. Charged K meson sometimes decays into two pi mesons with a lifetime T = 1.2 x 10-8 sec : K + = 135.0 Mev . Thus the The charged K meson has a rest energy M = 494 Mev , while the two pi mesons have rest energies , m ...
Page 425
... meson production in pi meson - nucleon collisions , ( c ) pi - meson pair production in nucleon - nucleon collisions , ( d ) nucleon - pair production in electron - electron collisions . 12.2 If a system of mass M decays or transforms ...
... meson production in pi meson - nucleon collisions , ( c ) pi - meson pair production in nucleon - nucleon collisions , ( d ) nucleon - pair production in electron - electron collisions . 12.2 If a system of mass M decays or transforms ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ