Basic Principles of Spectroscopy |
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Page 21
Raymond Chang. is present , the hamiltonian 3 ' representing the electric - field - electric- dipole - moment interaction is given by JC ' = ε • น When the field is just turned on , we still have ch ( t ) Substituting Eq . ( 1-67 ) into ...
Raymond Chang. is present , the hamiltonian 3 ' representing the electric - field - electric- dipole - moment interaction is given by JC ' = ε • น When the field is just turned on , we still have ch ( t ) Substituting Eq . ( 1-67 ) into ...
Page 81
... field . In an inhomogeneous electric field , the interaction is between the nuclear quadrupole moment and the electric field gradient ( EFG ) q at the nucleus . In the cartesian coordinates we define the EFGs along the x , y , and z ...
... field . In an inhomogeneous electric field , the interaction is between the nuclear quadrupole moment and the electric field gradient ( EFG ) q at the nucleus . In the cartesian coordinates we define the EFGs along the x , y , and z ...
Page 141
Raymond Chang. electric field . The proper treatment of the Stark effect is beyond the scope of this book . Here we shall merely quote some of the important results . The energy in the presence of the field EJ , M is given by5 EJ.M = Es ...
Raymond Chang. electric field . The proper treatment of the Stark effect is beyond the scope of this book . Here we shall merely quote some of the important results . The energy in the presence of the field EJ , M is given by5 EJ.M = Es ...
Contents
PREFACE | 1 |
NUCLEAR QUADRUPOLE RESONANCE SPECTROSCOPY | 29 |
NUCLEAR MAGNETIC RESONANCE SPECTROSCOPY | 52 |
Copyright | |
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