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Oxford University Press eBooks

Coherent Interactions of Fields and Atoms

Stephen Colby Rand

Published May 26, 2010• 0 citations
Publisher

Abstract

Chapter 5 begins the systematic application of the density matrix to describe optical interactions. First, stationary two‐ and three‐level atoms interacting with a traveling wave are compared to show that the presence of additional levels changes the saturation behavior of atoms. Then motion of the atoms is introduced and the phenomena of spatial and frequency‐domain hole‐burning are analyzed. Special effects due to standing waves, such as the light shift are covered in this section. Next, tri‐level coherence is considered, to extend the concept of coherences to two‐photon transitions or Zeeman interactions in folded Λ‐ or V‐systems. Higher (third‐)order interactions are also analyzed. This includes four‐wave mixing and pump‐probe spectroscopy which form the basis of common nonlinear laser spectrocopies. The chapter closes by pointing out that higher order coherent interactions, which can sometimes be important if they are deliberately phase‐matched, are best treated using a diagrammatic calculational technique based on Feynman diagrams.

DOI
10.1093/acprof:oso/9780199574872.003.0005

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Chapter 5 begins the systematic application of the density matrix to describe optical interactions. First, stationary two‐ and three‐level atoms interacting with a traveling wave are compared to show that the presence of additional levels changes the saturation behavior of atoms. Then motion of the atoms is introduced and the phenomena of spatial and frequency‐domain hole‐burning are analyzed. Special effects due to standing waves, such as the light shift are covered in this section. Next, tri‐level coherence is considered, to extend the concept of coherences to two‐photon transitions or Zeeman interactions in folded Λ‐ or V‐systems. Higher (third‐)order interactions are also analyzed. This includes four‐wave mixing and pump‐probe spectroscopy which form the basis of common nonlinear laser spectrocopies. The chapter closes by pointing out that higher order coherent interactions, which can sometimes be important if they are deliberately phase‐matched, are best treated using a diagrammatic calculational technique based on Feynman diagrams.
Chapter 5 begins the systematic application of the density matrix to describe optical interactions. Stationary two-and three-level atoms interacting with a traveling wave are compared to show that the presence of additional levels changes the saturation behavior of atoms. Then motion of the atoms is introduced and the phenomena of spatial and frequency-domain hole-burning are analyzed. Special effects due to standing waves, such as the light shift, are covered in this section. Next, tri-level coherence is considered, to extend the concept of coherences to two-photon transitions or Zeeman interactions in folded 3- or Λ-systems. Higher order interactions are also analyzed. This includes four-wave mixing and pump–probe techniques which form the basis of common nonlinear laser spectroscopies. Quantum interference is covered as a prelude to the topic of electromagnetically induced transparency. Higher order coherent interactions are also treated using a diagrammatic calculation technique based on Feynman diagrams.
In this paper we report on the study of two and multi-level atoms interacting with multiple laser beams. The semi-classical approach is used to describe the system in which the atoms are treated quantum mechanically via the density matrix operator, while the laser beams are treated classically using Maxwells equations. We present results of a two level atom interacting with single and multiple laser beams and demonstrate Rabi oscillations between the levels. The effects of laser modulation on the dynamics of the atom (atomic populations and coherences) are examined by solving the optical Bloch equations. Plots of the density matrix elements as a function of time are presented for various parameters such as laser intensity, detuning, modulation etc. In addition, phase-space plots and Fourier analysis of the density matrix elements are provided. The atomic polarization, estimated from the coherence terms of the density matrix elements, is used in the numerical solution of Maxwells equations to determine the behaviour of the laser beams as they propagate through the atomic ensemble. The effects of saturation and hole-burning are demonstrated in the case of two counter propagating beams with one being a strong beam and the other being very weak. The above work is extended to include four-wave mixing in four level atoms in a diamond configuration. Two co-propagating beams of different wavelengths drive the atoms from a ground state |1〉 to an excited state |3〉 via an intermediate state |2〉. The atoms then move back to the ground state via another intermediate state |4〉, resulting in the generation of two additional correlated photon beams. The characteristics of these additional photons are studied.
This chapter begins with a heuristic derivation of atomic population rate equations which include changes to level populations due to stimulated transitions as well as level relaxations and pump. These equations are used to study the saturation of population inversion with increasing light intensity and its dependence on the type of gain medium (three-level gain media vs. four-level gain media), lineshape and nature of line broadening (homogeneous vs inhomogeneous broadening). How saturation affects lineshape and thus gain and absorption giving rise to phenomena like power broadening and spectral hole burning is also discussed. The chapter summarizes the equations of motion for atomic polarization, inversion and the cavity field describing their nonlinear dynamical coupling. These equations, known as the Maxwell-Bloch equations, provide a complete description of atom-field interaction in a laser. Approximations of these equations, including the rate equation approximation, to deal with different laser classes are briefly described. These will be used in the next few chapters to explore and understand the rich and varied behavior of lasers. The chapter ends with a summary of select gain media for different types of commonly used lasers.
Chapter 6 begins by transforming the optical wave itself into a quantized form, and the full implications of the wave‐particle duality of Chapter 2 become clear. The electric field may be pictured as an infinite ladder of discrete states and this structure allows optical interactions to be described photon by photon. The origin of spontaneous emission emerges from this treatment as a transition process that is stimulated by electric field fluctuations of the vacuum, and Weisskopf–Wigner theory explains why it is irreversible. The subject of coherent states is introduced and intriguing possibilities outlined regarding the noise properties of components of these states that form different quadratures in terms of the optical phase. Next, statistical analysis of light fields is considered to serve as a basis for more quantitative comparisons of fields and their noise properties. Methods of calculating the first and second degrees of coherence are presented, and the ranges of values corresponding to “classical” versus “quantum” light sources are discussed. The reduced density matrix is developed to justify analysis that focuses on only certain aspects of optical dynamics while ignoring others, as an important tool for simplifying complex problems. Finally, in view of its historical importance, the problem of calculating the fluorescence spectrum of resonantly excited two‐level atoms is considered using both a method of moments and dressed atom theory.
Mechanical effects of light are considered in the first section of Chapter 7, together with their application to “optical tweezers.” This leads naturally to a discussion of laser cooling by a variety of techniques. Doppler cooling, magneto‐optic traps, sub‐Doppler cooling, and velocity‐selective coherent population trapping (VSCPT) are all covered. Then coherent population transfer is analyzed as a counterintuitive way of altering the occupation of energy levels in an exceptionally efficient manner. Coherent transverse optical magnetism, covered next, is the only example in the book of an optical effect mediated by the magnetic field of light. This phenomenon is characterized by intense emission of magnetic rather than electric dipole radiation at only moderate intensities and theoretically enables negative indices of refraction and spin control in unstructured, natural (nonmagnetic) materials. Electromagnetically induced transparency (EIT) is also described. This phenomenon is based on tri‐level coherence and can turn opaque media transparent over a limited bandwidth. Additionally, it can intensify high‐order nonlinear optical processes via intermediate step enhancement that is fully resonant. It has been applied to slow or store light as well. In this final chapter, squeezed light is given as an example of a coherent state with altered noise properties. Because the noise in squeezed quadratures of such a state can be reduced below the shot noise limit, it has applications to precision measurements and secure communication. The final section is on cavity quantum electrodynamics (QED). This topic treats the interaction of atoms with weak fields that are enhanced through the use of external cavities. In cavity QED, single photons can interact strongly enough with atoms to exhibit Rabi‐splitting behavior, and the strong coupling limit is considered to be a viable approach to quantum computation.
This chapter shows that several non-linear features can be demonstrated and the line shape of sub-natural line width can be obtained by manipulation of the powers of the two interacting laser radiations. The interaction of the laser radiation can produce a coherent superposition of the atomic states such that atoms are trapped in one state so that the atomic system may be transparent even in the presence of radiation frequency that is on resonance. Saturation spectroscopy is more conveniently performed in three level atomic systems interacting with two laser radiations. One of the radiations, called pump beam, has higher intensity and frequency on resonance or close to resonance with the transition frequency across two levels of the atom. The second laser radiation, called probe beam, is weaker and interacts with two other energy levels, one of which is common to the pump transition. A few hyperfine transitions are within the envelope of one Doppler profile.