Quantum fluctuations in atomistic semiconductor devices

Atomistic Green function simulations of model 25 nm×25 nm Si MOSFETs predict strong fluctuation effects derived from mode fluctuations in the quantum transport through the inhomogeneous 2DEG channel caused by the spatial distribution of non-self-averaged discrete dopants.     

Quantum theory of dye lasers

A quantum model of dye laser is given. To account for triplet losses a six levels model for the molecular system is assumed. The solution of generalized von Neumann equation in thermodynamical limit leads to a system of kinetic equations. Stationary solutions of this system are discussed. There are two distinct types of dependence of photon number versus pumping parameter. Beside a usual one, a new dependence characteristic for dye lasers only is present. In this case the definition of threshold should be revised.     

Quantum effects in submillimetre hot hole semiconductor lasers

The hole dynamics and emission processes in degenerate band semiconductors in strong crossedE B fields were studied both theoretically and experimentally. The Luttinger effective mass Hamiltonian was used to study the Landau level energy spectrum in anisotropic valence bands of Ge. The dependence of the energy spectrum onE,H fields orientation is analysed. The role of quantum effects, such as interaction and mixing of light and heavy hole states in the scattering process and Landau level population is studied. The results of experimental studies of stimulated emission spectra for intersub-band and cyclotron transitions as well as their dependence onE,H field orientation are presented, the experimental data being in good agreement with the quantum model calculations.     

Synchronization between optically injected semiconductor lasers on undamped relaxation oscillations

Seeding light from a laser into the cavity of a second one is a simple experiment largely encountered in optical domain (Stover, H.L., Steier, W.H.: Appl. Phys. Lett. 8, 91–93 (1966); Lang, R.: IEEE J. Quant. Elect. 18(6), 976–983 (1982)). With an unidirectional coupling, optical injection is a basic tool to study synchronization process between oscillators. The dynamics induced in this experiment have been extensively described, theoretically and experimentally (Simpson, T.B. et al.: Quant. Semiclassical Opt. 9(5), 765–784 (1997); Wieczorek S.: Opt. Commun. 172, 279–295 (1999); Blin, S.: Comptes Rendus de la Phys. 4(6), 687–699 (2003)) but mainly when the seeded light is a continuous wave (CW). In this paper, we describe the synchronization on an undamped relaxation regime. In order to study the degree of correlation between the two synchronized lasers (TL and RL), we use a cascade of two optical injections (Guignard, C.: Conference on Lasers and Electro Optics—the Europeen Quant. Electronics Conference (CLEO-EQEC), Munich (Germany), EC1M (2003)) thus three lasers: Master-transmitter laser (TL)-receiver laser (RL). The seeding by a field showing undamped relaxations can be directly compared with the optical injection by a CW signal, especially when the injected power and the detuning between the TL and RL frequencies are varied. Synchronization on undamped relaxation are shown to occur at values of the optical injected power and detuning, for which the RL is in the locked or wave-mixing regime when it is seeded by a CW. However, additional tongues of synchronization also exist at detuning equal to the relaxation oscillation frequency (ROF).     

Quantum theory of fluctuations in a cold damped accelerometer

We present a quantum network approach to real high sensitivity measurements. Thermal and quantum fluctuations due to active as well as passive elements are taken into account. The method is applied to the analysis of the capacitive accelerometer using the cold damping technique, developed for fundamental physics in space by ONERA and the ultimate limits of this instrument are discussed. It is confirmed in this quantum analysis that the cold damping technique allows one to control efficiently the test mass motion without degrading the noise level. Received 20 April 1999 and Received in final form 2 July 1999     

复合双外腔半导体激光器的量子噪声

本文用半经典理论给出了复合双外腔半导体激光器的量子噪声谱.     

Quantum theory of the polariton of the bounded semiconductor

The quantization of the polariton field is carried out for the semiconductor bounded by the surface. The orthonormalized set of the normal mode of the vacuum-semiconductor system is explicitly given for the case of the excitonic polarization field with the standard form of the spatial dispersion and the additional boundary condition of the elastic type. The scheme is employed to interpret the several experiments: optical reflectance and transmission, resonant Raman and Brillouin scattering, and the induced absorption of the polariton. Particularly, a recent experiment on CuCl which shows the existence of correlation among the polaritons and reflected light is discussed in view of the quantum picture.     

Quantum mechanical tunneling phenomena in metal–semiconductor junctions

The impact of the quantum mechanical tunneling effect on the operation of MESFET device structure has been investigated. Due to the presence of a Schottky barrier in a highly doped semiconductor, the depletion region is so narrow that electrons can tunnel through the barrier and contribute to the gate leakage current. This, in turn, facilitates current gain of the Schottky junction transistor (SJT) in the subthreshold region. In a simulation of a SJT we have used 2D Monte Carlo particle-based simulations. Quantum mechanical tunneling effects have been accounted for by using the Airy function transfer matrix approach, valid for piecewise linear potential barriers.     

Quantum theory of wave propagation and linear amplification in free electron lasers

A quantum field theory of free electron lasers is formulated and evaluated for the case of linear propagation and amplification of thermal noise and radiation emitted spontaneously and from shot noise.     

Instabilities in semiconductor lasers

One of the most relevant problems connected with optical fiber communication is that related to the presence of instabilities in the output of semiconductor lasers. These instabilities appear as nonlinearities in the optical power-current characteristic (kinks) or as dynamics instabilities (self-pulsing). These phenomena more frequently occur in devices without a refractive index profile introduced ad hoc in the junction plane (gain-guided lasers); self-pulsing, in particular, is present in aged lasers. Both of them, however, can appear also in nonaged lasers with lateral confinement of the e.m. field (index-guided lasers). In this paper the principal experimental results obtained studying instability phenomena and the physical mechanisms proposed for their explanation are reported and discussed.     

Frequency dynamics of semiconductor lasers with atomic absorbers: theory and experiments

In this paper we discuss the spectral behavior of monomode semiconductor laser systems whose output amplitude is constant, but whose frequency may be bistable, multistable, locked or present instabilities. The explored configurations are: (i) a laser diode (Fabry-Pérot) under orthogonal filtered optical feedback; and (ii) an extended-cavity diode laser with an intracavity strongly-saturated resonant vapor. Starting from rate equations for the carrier density and for the radiation field oscillating in the cavity of these systems we describe spectral features which are in very good quantitative agreement with experimental observations.     

Quantum Cascade Lasers: the quantum technology for semiconductor lasers in the mid-far-infrared

The quantum cascade laser is a new light source based on resonant tunnelling and optical transitions between quantised conduction band states. In these semiconductor devices the principles of operation arise from the quantum engineering of electronic energy levels and tailoring of their wavefunctions. In recent years the performance of these devices has improved markedly and this semiconductor technology is now an attractive choice for the fabrication of mid-far infrared lasers in a very wide spectral range (3–80 μm). At present, quantum cascade lasers are capable of continuous-wave room temperature operation and can deliver 200–300 mW of average power (at λ∼9 μm) operating on a Peltier cooler. To cite this article: C. Sirtori, J. Nagle, C. R. Physique 4 (2003).     

Gain and saturation in semiconductor lasers

Several approaches have been developed for modelling the gain and saturation behaviour of semiconductor lasers, and this study includes a historical review of these various approaches. Special attention is given to rate equation models and to the possibility of so-called gain nonlinearities that might affect the CW and modulation performance of semiconductor lasers. Discussions are mainly limited to the GaAs/GaAIAs and InGaAsP/InP systems, for which the gain and gain nonlinearities have been most extensively studied.     

Frequency stabilization in semiconductor lasers

Three promising methods of improving temporal coherence in semiconductor lasers are reviewed. They are the development of novel laser devices, a technique of optical feedback and a technique of electrical feedback. The main discussion in this paper is focused on the technique of electrical feedback. The theoretical limit of frequency stability and recent experimental results are presented with respect to the following five subjects which are indispensable in the realization of highly coherent lasers: (a) frequency stabilization; (b) improvements in frequency reproducibility; (c) linewidth reduction; (d) frequency tracking; and (e) stable, accurate and wideband frequency sweep.     

Optical bistability in semiconductor lasers

Optical and Quantum Electronics -     

Influence of radiation fluctuations on the magnitude of optoelectronic signal in semiconductor lasers with external optical feedback

Numerical modeling of dynamical processes in semiconductor lasers with external delayed optical feedback has been performed on the basis of the rate equations taking into account the quantum fluctuations of radiative transition rates. It has been shown that the nature of the optoelectronic signal as a function of pump current is determined by the magnitude of the optoelectronic coupling and corresponds to the behavior of the autocorrelation function of the radiation. It has been found that the radiation coherence decreases substantially with strong optical feedback. Experimental measurements confirming the theoretical results have been performed. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 75, No. 6, pp. 809–813, November–December, 2008.     

Quantum fluctuations and inertia

One of the three key assumptions involved in the stochastic formulation of quantum mechanics, the inverse proportionality of the quantum diffusion constant to the inertial mass, is shown to be amenable to experimental test. By relaxing this assumption, a non-linear generalization of the Schrödinger equation is found. The present experimental uncertainty in the measurement of the Lamb shift is then used to bound the deviation from the aforementioned inverse proportionality to be less than 4 × 10⁻¹³.