Stimulated Emission of Radiation - stimulated emission is referring to the emission of radiation (a photon) from one quantum system at its transition frequency induced by the presence of other photons at that frequency - introduced by Einstein in 1917 to derive Planck's blackbody radiation law - is the basis for the operation of a LASER (Light Amplification by Stimulated Emission of Radiation) Consider an assembly of N atoms with energy levels E i and E j in thermal equilibrium with a thermal radiation field with energy density u(ν) at temperature T - the transition frequency ν ij in the individual atom is - the probability of an atom in state i to absorb a photon is proportional to u(ν ij ) (related to the number of photons at that frequency) and to the probability B ij (Einstein B coefficient) of the atom to absorb a photon at that frequency phys4.15 Page 1 - thus, the total number of atoms per second that absorb a photon is where N i is the number of atoms in state i - an atom in state j has a probability A ji (Einstein A coefficient) to spontaneously decay into state i by emitting a photon at frequency ν in a process called spontaneous emission - also, an atom in state j has a probability B ji to decay into state i by emitting a photon at frequency ν ij stimulated by the presence of other photons at that frequency the number of which is proportional to u(ν ij ) - this process is called stimulated emission - thus the total number N ji of atoms per second that make a transition into the lower state is given by - in thermal equilibrium the number of atoms that make a transition to lower energy must be identical to the number of atoms making a transition to higher energy phys4.15 Page 2
Transitions in a collection of atoms interacting with a radiation field - in thermal equilibrium - solve for the energy density of the radiation field u(ν) - with the number of atoms in the ground N i or excited state N j is given by classical M.-B. statistics - thus phys4.15 Page 3 - hence the energy density of a radiation field in thermal equilibrium is given by - this is Planck's formula for blackbody radiation for - for identical upwards and downwards transition rates - and with the ratio of spontaneous emission to induced emission rate given by note: - stimulated emission does occur and is consistent with the form of the blackbody spectrum - the probability for stimulated absorption is equal to the probability stimulated emission - the likelihood of spontaneous emission relative to stimulated emission increases rapidly with frequency - knowing one of the parameters A ji, B ji, B ij we can determine the other ones - spontaneous emission is 'stimulated' by vacuum fluctuations (QED) phys4.15 Page 4
Light Amplification by Stimulated Emission of Radiation (LASER) LASER Light Amplification by Stimulated Emission of Radiation properties: monochromatic coherent directed bright phys4.15 Page 5 Properties of LASER light monochromatic - relative line width coherence - temporal coherence - spatial coherence limited only by optics brightness - intensities - large photon flux in pulsed operation - short pulses phys4.15 Page 6
The LASER 1. active LASER medium (gas, dye, solid) 2. pumping (light, electrical energy) 3. 100% reflecting mirror 4. coupling mirror (< 1% transmission) 5. LASER beam phys4.15 Page 7 The LASER Principle - generation of a large number of excitations in a medium by (stimulated) absorption - a long lived metastable state to achieve population inversion - stimulated emission of radiation - storage of radiation field in a resonant cavity with partially transmitting mirror phys4.15 Page 8
Generation of Population Inversion - excitation by optical pumping in a three level system - transition (possibly non-radiative) to a metastable state - stimulated emission - at least a three level system is required to achieve population inversion as the symmetry between the probability for absorption (B ij ) and emission (B ji ) results at best in equal population of the two states such that emission cannot be the dominant process (i.e. there would be no amplification in number of photons) phys4.15 Page 9 Examples of Lasers Ruby Laser: Cr + ions in Al 2 O 3 crystal (sapphire) - optical pumping using flash light - Helium-Neon Laser: gas mixture (90 % He, 10 % Ne) where He is excited electrically in gas discharge and energy is transferred in collision to Ne phys4.15 Page 10
Nobel Prize in Physics 1964 for fundamental work in the field of quantum electronics, which has led to the construction of oscillators and amplifiers based on the maser-laser principle Charles H. Townes Nicolay G. Basov Aleksandr M. Prokhorov phys4.15 Page 11 Laser-Pointer housing electronics LASER and optics phys4.15 Page 12
CD Player compact disc the mechanism portable CD player (older modell) phys4.15 Page 13 Laser-Printer resolution up to 20 µm or 50 points per mm (= 1270 dpi) colors with multiple stages phys4.15 Page 14
Material Processing CO 2 gas LASER up to 20 kw power www.trumpf.com phys4.15 Page 15 Lasers in Medicine eye surgery dermatology etc. phys4.15 Page 16
Specific Heat of Solids - dependence of thermal energy stored in a solid on temperature - molar specific heat at constant volume c V : energy that needs to be added to 1 mol of a solid to increase its temperature by 1 Kelvin - thermal energy is stored in solids in the vibrations of its constituents (atoms, ions or molecules) - in a simple model the atoms can vibrate along 3 independent (x, y, z) directions that each can be considered as an independent harmonic oscillator - the equipartition theorem tells us the average energy stored in each degree of freedom, thus the total energy of a solid containing 1 mol = N 0 = 6.022 10 23 of atoms is given by - R = 8.31 J/mol is the ideal gas constant (pv = nrt) - specific heat (Dulong Petit law) phys4.15 Page 17 Dulong petit law fails for light elements (e.g. carbon) and at low temperatures, see plot - problem can be solved using the Bose-Einstein distribution function for the probability of an harmonic oscillator to have energy hν - average energy for a harmonic oscillator of frequency ν - total energy per mol - thus Einstein's specific heat formula is phys4.15 Page 18
- the high temperature limit of Einstein's formula - therefore - at high temperatures the thermal energy is much larger than the typical level separation of the harmonic oscillators in the solid and the specific heat is close to the classical prediction - at low temperatures the thermal energy is comparable to the level separation and quantum statistics start to play a role - for lighter elements with smaller masses the oscillator frequencies are higher and thus quantum effects are more important even at higher temperatures - the zero point motion does not play a role for the specific heat as it is only a constant offset in energy phys4.15 Page 19 Debeye theory - Debeye regarded a solid as a continuous elastic medium with elastic standing waves instead of considering the atoms as individual oscillators the way Einstein did - these standing waves can have frequencies ν up to a maximum value ν max - they are like transverse and longitudinal elastic waves that propagate at the speed of sound in the solid - their energies are quantized as in a harmonic oscillator - each quantum of the elastic wave is called a phonon - Debeye assumed that 3N different modes exist per mol in a solid - the resulting formula describes the specific heat of the solid better than Einstein's formula - to be discussed in detail in solid state physiscs phys4.15 Page 20