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Athermal laser design
Athermal laser design

Phase Sensitive Amplification in Single and Double Pumped Non
Phase Sensitive Amplification in Single and Double Pumped Non

... …) through Field Conjugation and Phase Multiplication and to sum them (via Field Addition) and eventually set their amplitudes (via Magnitude scaling). This represents Fourier synthesis which in principle allows any transfer characteristics to be obtained – we generate the signal harmonics first and ...
Poster 1
Poster 1

... pairs interfere at PBS, so lower curve is below the red line Thus we have observed some polarization entanglement 1000s of data per curve, taken while sweeping the cavity ...
Low atmospheric density measurement based on Rayleigh
Low atmospheric density measurement based on Rayleigh

... instantaneous measurements of atmospheric density with the seeded species I2 in the range of (0.1–6.5)×1017 cm–3 [9]. As the seeded material may introduce unacceptable corrosion or undesirable influence on the flow field, the applications of molecular tagging techniques such as coherent anti-Stokes ...
Measured limits to contamination of optical
Measured limits to contamination of optical

Full Paper
Full Paper

Core Scattering of Stark Wave Packets
Core Scattering of Stark Wave Packets

OCT
OCT

...  Equation 8 establishes that the envelope of  equals the Fourier transform of the spectrum. Since we assumed a symmetric spectrum, the envelope is a real function. Further, the phase (modulation) of  is linear with  , where the shape is given by the mean frequency,     0 . ...
Fundamentals of Spectroscopy for Optical Remote Sensing
Fundamentals of Spectroscopy for Optical Remote Sensing

... quantum) transitions. Of course, all of such spectroscopy starts with the basics of quantum physics, quantum mechanics, electromagnetism, lasers, optics, etc. The thoughts outlined above help form the teaching philosophy and course structure for the spectroscopy class. For this graduate-level class ...
Doppler-Free Spectroscopy of Iodine at 739nm
Doppler-Free Spectroscopy of Iodine at 739nm

Optical Fibres
Optical Fibres

Stimulated Raman Transitions Between Hyperfine Ground States of
Stimulated Raman Transitions Between Hyperfine Ground States of

Five ways to the nonresonant dynamic Stark effect
Five ways to the nonresonant dynamic Stark effect

... A similar effect occurs in the oscillating electric fields produced by lasers. If the field oscillates with a very low frequency, the level shifts adiabatically follow the static Stark shift formula. As the frequency is increased, and under appropriate conditions, the eigenstates do not follow the i ...
AN2 ATOMS
AN2 ATOMS

... Molecular energy levels A molecule consists of several atoms bound together. A proper treatment of molecular energies regards all atoms and all their electrons as one system. A typical molecule has many more possible energy states than a single atom. Consequently, since every electron in a molecule ...
Total view of the AFM
Total view of the AFM

... • There are different types – Ion Microprobe, TOF-SIMS, and Quadrupole SIMS. The first two are more important: the first is also called dynamic SIMS where a complete depth profile can be done and uses q/m ratio to separate ions, and the 2nd used for static SIMS as only a few monolayers are removed, ...
Macroscopic effects in noncollinear high-order
Macroscopic effects in noncollinear high-order

6.1 Characteristics Because VCSELs emit from the top surface of the
6.1 Characteristics Because VCSELs emit from the top surface of the

... slope efficiency decreases. For DWDM applications, which require very precise operating wavelengths, most of the current laser diode designs need to be cooled to within ± 0.3 °C. As previously explained, the direct modulation of a laser diode has several limitations, including limited propagation di ...
L Generation of squeezed states and twin beams system
L Generation of squeezed states and twin beams system

... pursuit. However, recently it has become clear that in practical situations squeezed states are not expected to play a significant role in ultra-precision interferometry, for two reasons. First, the degree of squeezing observed has remained limited, owing to imperfect quantum efficiency of detectors ...
Trionic optical potential for electrons in semiconductors ARTICLES *
Trionic optical potential for electrons in semiconductors ARTICLES *

... 3.6 meV in CdTe semiconductor quantum wells. For red detuning, the continuum and the bound trion level give contributions of opposite sign to the shift of the electron ground-state energy (see Fig. 2). As a consequence, the potential depth saturates at a maximum of εEb . For intermediate blue detuni ...
M. Tech in Optoelectronics and Laser Technology
M. Tech in Optoelectronics and Laser Technology

... Classification of optical processes, optical coefficients, complex refractive index and dielectric constant, Optical materials : Crystalline insulators and semiconductor, glasses, metal, molecular materials, doped glass and insulator characteristics, Optical Physics in the Solid state, crystal symme ...
Introduction
Introduction

... • The purpose of a rise-time budget is to ensure that the complete system is able to operate at the intended bit-rate • The rise-time characteristics of the transmitter and receiver are usually known. The allocated rise time will depend on the format used by the system, i.e.Return to Zero (RZ) or No ...
Quantum computation with trapped polar molecules
Quantum computation with trapped polar molecules

PDF
PDF

IJFTR 12(2) 100-102
IJFTR 12(2) 100-102

... measures the refractive index at the fibre surtace. Interferometric measurements of the refractive index across the fibre have shown that Becke-line refractive indices are not confined to the fibre surface but may occur at any point on the fibre radius 11• Clearly, any method or any formula used for ...
Three-dimensional superresolution technology applied to
Three-dimensional superresolution technology applied to

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Ultrafast laser spectroscopy

Ultrafast laser spectroscopy is a spectroscopic technique that uses ultrashort pulse lasers for the study of dynamics on extremely short time scales (attoseconds to nanoseconds). Different methods are used to examine dynamics of charge carriers, atoms and molecules. Many different procedures have been developed spanning different time scales and photon energy ranges; some common methods are listed below.
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