Presentation on theme: "Interaction of Electromagnetic Radiation with Matter."— Presentation transcript:
Interaction of Electromagnetic Radiation with Matter
Dielectric Constant and Atomic Polarizability Under the action of the electric field, the positive and negative charges inside each atom are displaced from their equilibrium positions. The induced dipole moment is p = αE Where α is atomic polarizability.
Dielectric Constant and Atomic Polarizability The dielectric constant of a medium will depend on the manner in which the atoms are assembled. Let N be the number of atoms per unit volume. The polarization can be written approximately as P=Np=NαE=ε 0 ΧE Where Χ is susceptibility.
Dielectric Constant and Atomic Polarizability The dielectric constant ε of the medium is If the medium is nonmagnetic (i.e., μ=μ 0 ), the index of refraction is given by
Classical Electron Model In classical physics, we assume that the electrons are fastened elastically to the atoms and obey the following equation of motion The electric field of the optical wave in the atom can be written as
Classical Electron Model The equation has the following steady-state solution The induced dipole moment is The atomic polarizability is
Classical Electron Model If there are N atoms per unit volume, the index of refraction of such a medium is If the second term in this equation is small compared to 1, the index of refraction can be written as
Dispersion and Complex Refractive Index From the equation We can get that the index of refraction is higher for the waves with larger ω. The phenomenon that the refractive index depends on frequency is called the phenomenon of dispersion.
Dispersion and Complex Refractive Index The imaginary term iϒω in the equation accounts for the damping of electron motion and gives rise to the phenomenon of optical absorption.
Dispersion and Complex Refractive Index The complex refractive index can be written as
Dispersion and Complex Refractive Index For a wave written as In which Using the complex refractive index, the wave number K becomes
Dispersion and Complex Refractive Index The electric field of the wave becomes
Optical Pulse and Group Velocity In the pulsed mode, the pump energy can be concentrated into extremely short time durations, thereby increasing the peak power. The propagation of a pulse due to dispersion can be described by representing the pulse as a sum of many plane-wave solutions of Maxwell’s equations.
Optical Pulse and Group Velocity The scalar amplitude ψ(z,t) can be thought of as one of the components of electromagnetic field vectors. If A(k) denotes the amplitude of the plane-wave component with wave number k, the pulse ψ(z,t) can be written as
Optical Pulse and Group Velocity A laser pulse is usually characterized by its center frequency ω 0 or wave number k 0 and the frequency spread Δ ω or spread in wave number Δk. In other words, A(k) is sharply peaked around k 0. We expand ω(k) around the value k 0 in terms of a Taylor series:
Optical Pulse and Group Velocity The ψ(z,t) becomes The integral in above equation is a function of the composite variable [z – (dω/dk) 0 t] only and is called the envelope function
Optical Pulse and Group Velocity The amplitude of the pulse can be written as This shows that, apart from an overall phase, the laser pulse travels along undistorted in shape
Optical Pulse and Group Velocity The group velocity of the pulse is The group velocity represents the transport of energy.