MonographU.S. Government Printing Office, 1975 |
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Page 11
... means that the solution of the problem of interacting fields is represented by an expansion in terms of free fields . As is well known this procedure , strictly speaking , may not be legitimate in relativistic field theory in contrast ...
... means that the solution of the problem of interacting fields is represented by an expansion in terms of free fields . As is well known this procedure , strictly speaking , may not be legitimate in relativistic field theory in contrast ...
Page 12
... means of the inverse transformations a ε + Ε = = f [ £ x ( c ) A + Σ K [ K K K f ( ɛ ) B K K etc ... , we shall obtain discretized basis configurational states r ) . The corresponding x ( r ) for the solution amplitudes n discretized ...
... means of the inverse transformations a ε + Ε = = f [ £ x ( c ) A + Σ K [ K K K f ( ɛ ) B K K etc ... , we shall obtain discretized basis configurational states r ) . The corresponding x ( r ) for the solution amplitudes n discretized ...
Page 40
... mean values of complicated products of creation and annihilation operators according to well known technique . A few simple examples will be worked out in the following chapters . III.1 - CHAPTER III FREE FIELD DISCRETIZED EXPANSIONS ...
... mean values of complicated products of creation and annihilation operators according to well known technique . A few simple examples will be worked out in the following chapters . III.1 - CHAPTER III FREE FIELD DISCRETIZED EXPANSIONS ...
Page 134
... means of ( 1.56 ) , ( 1.58 ) the intrinsic energy of the system . Using the previously obtained rest mases of the nucleon and the pion one can derive the discrete relative momentum of the scattering state , and one can verify that Y ...
... means of ( 1.56 ) , ( 1.58 ) the intrinsic energy of the system . Using the previously obtained rest mases of the nucleon and the pion one can derive the discrete relative momentum of the scattering state , and one can verify that Y ...
Page 136
... means of ( A.3 ) , ( A.32 ) , ( B. 3 ) by the parton laboratory coordinates , equation ( C.7 ) is already almost in the form ( B.2 ) . To achieve that form one must rewrite the multipoles making up the nucleon system and the pion system ...
... means of ( A.3 ) , ( A.32 ) , ( B. 3 ) by the parton laboratory coordinates , equation ( C.7 ) is already almost in the form ( B.2 ) . To achieve that form one must rewrite the multipoles making up the nucleon system and the pion system ...
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accuracy analysis ANGLE OF INCIDENCE ASTM attenuation factor bath beam beam splitter Boson bulb Bureau of Standards Celsius Center Certificate chemical chemistry clinical coefficient comparison component computed configurations correction cuvettes defined degrees determined difference emergent stem energy estimate Fermion field fringe functions gage block given glass graduated Hamiltonian interaction interferometric interval invariant matrix elements isospin laboratory length limits liquid measurement process measurement system ment mercury meson momentum mometer multipoles National Bureau NBS Spec nominal nucleon obtained operators parameters particle percent physical pion precision predicted value procedures properties provides Publ quantum numbers rate of change reference method relativistic Report of Calibration Schrödinger picture shown in figure solutions Spectrophotometry spin SRM's standard deviation Standard Reference Materials subscription surface systematic error technical Technology tion uncertainty variability vector wavelength WEDGE ANGLE
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