MonographU.S. Government Printing Office, 1975 |
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Page 14
... correction for effects of scattering can be accomplished by extrapolating the observed ratio quadratic- ally to infinite distance . 6 . NUMERICAL RESULTS AND CONCLUSIONS The equations that have been presented in the earlier sections ...
... correction for effects of scattering can be accomplished by extrapolating the observed ratio quadratic- ally to infinite distance . 6 . NUMERICAL RESULTS AND CONCLUSIONS The equations that have been presented in the earlier sections ...
Page 26
... correcting errors in portions of the manuscript . This work was supported in part by the Department of Defense , Calibration Coordination Group 74-92 , U. S. Army Missile Command , Redstone Arsenal , Alabama 35809 . 8. REFERENCES 1. Yu ...
... correcting errors in portions of the manuscript . This work was supported in part by the Department of Defense , Calibration Coordination Group 74-92 , U. S. Army Missile Command , Redstone Arsenal , Alabama 35809 . 8. REFERENCES 1. Yu ...
Page 131
... corrections will have to be applied . In the procedure outlined in this monograph , the wave func- tions Y n of the system are obtained as configuration mixtures in a discretized basis ( cf. Eq . 1.29 , or 1.30 , together with 1.32 and ...
... corrections will have to be applied . In the procedure outlined in this monograph , the wave func- tions Y n of the system are obtained as configuration mixtures in a discretized basis ( cf. Eq . 1.29 , or 1.30 , together with 1.32 and ...
Page 137
... case . Finally , of course , the scattering states are correct as far as the CM motion is concerned . No recoil or relativistic corrections have to be made . D. THE PHYSICAL VACUUM The lowest eigenstate , say | -137- C.4.
... case . Finally , of course , the scattering states are correct as far as the CM motion is concerned . No recoil or relativistic corrections have to be made . D. THE PHYSICAL VACUUM The lowest eigenstate , say | -137- C.4.
Page 11
... corrections ... - Chapter III QUADRUPOLE AND MAGNETIC STATIC MOMENTS ... III.1 - Quadrupole moments .... III.2 - III.1.1 - Spin O field ..... III.1.2 - Spin 1/2 field .... III.1.3 Spin 1 field .... Magnetic moments . III.2.1 - Spin 0 ...
... corrections ... - Chapter III QUADRUPOLE AND MAGNETIC STATIC MOMENTS ... III.1 - Quadrupole moments .... III.2 - III.1.1 - Spin O field ..... III.1.2 - Spin 1/2 field .... III.1.3 Spin 1 field .... Magnetic moments . III.2.1 - Spin 0 ...
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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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