Electric dipole Transition moment

Electric dipole Transition moment

Elastic and Inelastic Scattering Raman Powerpoint Templates

Rayleigh Scattering vs Raman Scattering

Interaction between electric field of incident photon and molecule Electric field oscillating with incident frequency vi: Induces molecular electric dipole (p): Proportional to molecular polarizability,  Polarization results in nuclear displacement Classical Raman Physics

For small distortions, polarizability is linearly proportional to the displacement • Resultant dipole: Rayleigh Scattering Stokes Raman Anti-Stokes Raman

Roto-Vibrational Raman ΔJ = 0 ± 2 LineSpacing 4B

Ressonance Raman Scattering effect enhanced by a factor 106

Instrumentation

Lasers Ar+ ion 488.0 nm & 514.5 nm • Kr+ ion 530.9 nm & 647.1 nm • He:Ne 632.8 nm • Nd:YAG 1064 nm • Diode 630 nm & 980 nm • Resolution < 6 cm-1 → • Laser Linewidth < 1 cm-1 • Wavelength Stabilization is a must have • (most common 785 nm NIR 300mW

Holographic notch filter

Electric dipole Transition moment

Electric dipole Transition moment

Presentation Transcript

Electric Dipole Moment of Neutron and Neutrinos

Dipole Moment of Solitons

Electric dipole moment searches

Measurement of the electron’s electric dipole moment

DIPOLE MOMENT

Electric Dipole

Search for the electron electric dipole moment

Neutron Electric Dipole Moment Experiment

Neutron Electric Dipole Moment

Electric Dipole Moment Searches in Nuclei, Atoms, and Molecules

Magnetic dipole moment

Muon electric dipole moment induced by unparticles

Search for the Electron Electric Dipole Moment

Last lecture The electric dipole Electric field due to a dipole Electric dipole moment

Magnetic Dipole Moment

Deuteron Polarimeter for Electric Dipole Moment Search

ELECTRIC DIPOLE MOMENT IN DEFORMED NUCLEI

Magnetic Dipole Moment

Last lecture The electric dipole Electric field due to a dipole Electric dipole moment

Electric Dipole Moment Experiments