A Maxwell–Schrödinger solver for quantum optical few-level systems

详细信息    查看全文

• 作者：Robert Fleischhaker^a ; ^{robert.fleischhaker@mpi-hd.mpg.de} ; J&#xf6 ; rg Evers ; ^a ; ^{joerg.evers@mpi-hd.mpg.de}
• 关键词：Maxwell– ; Schr&#xf6 ; dinger equation ; Quantum optical few-level system ; Cross-coupling ; Magnetic field component ; Second order Lax– ; Wendroff algorithm ; Adams predictor
• 刊名：Computer Physics Communications
• 出版年：2011
• 出版时间：March 2011
• 年：2011
• 卷：182
• 期：3
• 页码：739-747
• 全文大小：545 K

文摘

The msprop program presented in this work is capable of solving the Maxwell–Schrödinger equations for one or several laser fields propagating through a medium of quantum optical few-level systems in one spatial dimension and in time. In particular, it allows to numerically treat systems in which a laser field interacts with the medium with both its electric and magnetic component at the same time. The internal dynamics of the few-level system is modeled by a quantum optical master equation which includes coherent processes due to optical transitions driven by the laser fields as well as incoherent processes due to decay and dephasing. The propagation dynamics of the laser fields is treated in slowly varying envelope approximation resulting in a first order wave equation for each laser field envelope function. The program employs an Adams predictor formula second order in time to integrate the quantum optical master equation and a Lax–Wendroff scheme second order in space and time to evolve the wave equations for the fields. The source function in the Lax–Wendroff scheme is specifically adapted to allow taking into account the simultaneous coupling of a laser field to the polarization and the magnetization of the medium. To reduce execution time, a customized data structure is implemented and explained. In three examples the features of the program are demonstrated and the treatment of a system with a phase-dependent cross coupling of the electric and magnetic field component of a laser field is shown.

Program summary

Program title: msprop

Catalogue identifier: AEHR_v1_0

Program summary URL: http://cpc.cs.qub.ac.uk/summaries/AEHR_v1_0.html

Program obtainable from: CPC Program Library, Queen's University, Belfast, N. Ireland

Licensing provisions: Standard CPC licence, http://cpc.cs.qub.ac.uk/licence/licence.html

No. of lines in distributed program, including test data, etc.: 507 625

No. of bytes in distributed program, including test data, etc.: 10 698 552

Distribution format: tar.gz

Programming language: C (C99 standard), Mathematica, bash script, gnuplot script

Computer: Tested on x86 architecture

Operating system: Unix/Linux environment

RAM: Less than 30 MB

Classification: 2.5

External routines: Standard C math library, accompanying bash script uses gnuplot, bc (basic calculator), and convert (ImageMagick)

Nature of problem: We consider a system of quantum optical few-level atoms exposed to several near-resonant continuous-wave or pulsed laser fields. The complexity of the problem arises from the combination of the coherent and incoherent time evolution of the atoms and its dependence on the spatially varying fields. In systems with a coupling to the electric and magnetic field component the simultaneous treatment of both field components poses an additional challenge. Studying the system dynamics requires solving the quantum optical master equation coupled to the wave equations governing the spatio-temporal dynamics of the fields [1,2].

Solution method: We numerically integrate the equations of motion using a second order Adams predictor method for the time evolution of the atomic density matrix and a second order Lax–Wendroff scheme for iterating the fields in space [3]. For the Lax–Wendroff scheme, the source function is adapted such that a simultaneous coupling to the polarization and the magnetization of the medium can be taken into account.

Restrictions: The evolution of the fields is treated in slowly varying envelope approximation [2] such that variations of the fields in space and time must be on a scale larger than the wavelength and the optical cycle. Propagation is restricted to the forward direction and to one dimension. Concerning the description of the atomic system, only a finite number of basis states can be treated and the laser-driven transitions have to be near-resonant such that the rotating-wave approximation can be applied [2].

Unusual features: The program allows the dipole interaction of both the electric and the magnetic component of a laser field to be taken into account at the same time. Thus, a system with a phase-dependent cross coupling of electric and magnetic field component can be treated (see Section 4.2 and [4]). Concerning the implementation of the data structure, it has been optimized for faster memory access. Compared to using standard memory allocation methods, shorter run times are achieved (see Section 3.2).

Additional comments: Three examples are given. They each include a readme file, a Mathematica notebook to generate the C-code form of the quantum optical master equation, a parameter file, a bash script which runs the program and converts the numerical data into a movie, two gnuplot scripts, and all files that are produced by running the bash script.

Running time: For the first two examples the running time is less than a minute, the third example takes about 12 minutes. On a Pentium 4 (3 GHz) system, a rough estimate can be made with a value of 1 second per million grid points and per field variable.

References:

[1] Z. Ficek, S. Swain, Quantum Interference and Coherence: Theory and Experiments, Springer, Berlin, 2005.

[2] M.O. Scully, M.S. Zubairy, Quantum Optics, Cambridge University Press, Cambridge, 1997.

[3] W.H. Press, B.P. Flannery, S.A. Teukolsky, W.T. Vetterling, Numerical Recipes, Cambridge University Press, Cambridge, 1992.

[4] R. Fleischhaker, J. Evers, Phys. Rev. A 80 (2009) 063816.