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Monte-Carlo Simulation of Stellar Intensity Interferometry by Janvida Rou
Monte-Carlo Simulation of Stellar Intensity Interferometry by Janvida Rou

PDF Link
PDF Link

Early-time dynamics of the photoexcited hydrated electron
Early-time dynamics of the photoexcited hydrated electron

Rotation and phase-shift operations for a charge qubit in a double
Rotation and phase-shift operations for a charge qubit in a double

Electron Induced Fluorescence Spectra of Methane
Electron Induced Fluorescence Spectra of Methane

Three key regimes of single pulse generation per round trip of all
Three key regimes of single pulse generation per round trip of all

Chemical Bond Activation Observed with an X
Chemical Bond Activation Observed with an X

Raman spectroscopy
Raman spectroscopy

Geometric manipulation of the quantum states of two
Geometric manipulation of the quantum states of two

Multiphoton population transfer between rovibrational states of HF: adiabatic
Multiphoton population transfer between rovibrational states of HF: adiabatic

... forbidden and the transition occurs through tunnelling. We show that for larger peak intensities, the transfer can be looked upon as a classical transition in phase space, similar to that observed in the atomic case. We extend our simulations to fully three-dimensional quantum calculations and inves ...
Orientation of perylene derivatives on semiconductor surfaces
Orientation of perylene derivatives on semiconductor surfaces

Proton Resonance Frequencies in Several Organophosphorus Acids
Proton Resonance Frequencies in Several Organophosphorus Acids

Finite-momentum condensation in a pumped microcavity R. T. Brierley
Finite-momentum condensation in a pumped microcavity R. T. Brierley

Slowing Down the Speed of Light - The Institute of Optics
Slowing Down the Speed of Light - The Institute of Optics

Role of dispersion in pulse emission from a sliding
Role of dispersion in pulse emission from a sliding

... the amplitude A of the solitary-wave solution [Eqs. (3) and (4)] on the dispersion coefficient D. In Figs. 3 – 5 the linear excess gain d . 0, whereas in Figs. 6 – 8 d , 0. In Figs. 3 – 5 we set b ­ 3d ­ 0.15 and we varied the nonlinear gain (or saturable loss) coefficient from g ­ 0 (dashed curves) ...
Supplementary Information
Supplementary Information

Ultrafast Laser-induced Damage and the Influence of Spectral Effects
Ultrafast Laser-induced Damage and the Influence of Spectral Effects

New approach to pulse propagation in nonlinear
New approach to pulse propagation in nonlinear

... Propagation of optical pulses through nonlinear dispersive media is studied in many contexts ranging from optical communications [1] to ultrafast optics [2]. The usual starting point is the nonlinear Schrödinger (NLS) equation, obtained from Maxwell’s equations under the slowly varying envelope appr ...
The Ultrasound Machine
The Ultrasound Machine

PDF
PDF

... theoretical fit obtained from the model described above. The fitting is achieved by letting vary α , ρ and t . The ultimate goal of the fit is to estimate the propagation loss α . The three spectra depicted in insets (a), (b) and (c) respectively are such that back reflections ρ changes from 0.008 t ...
Application of the Sampling and Replication Operators to Describe
Application of the Sampling and Replication Operators to Describe

... duration for the pulse, which is acceptable for amplification in the active medium that has a gain curve of bandwidth . Thus, for amplification of extremely short laser pulses, the gain curve of the active medium must have the widest possible bandwidth . ...
Rotational Spectroscopy of Diatomic Molecules - Assets
Rotational Spectroscopy of Diatomic Molecules - Assets

... Molecular spectroscopy involves the study of the absorption or emission of electromagnetic radiation by matter; the radiation may be detected directly, or indirectly through its effects on other molecular properties. The primary purpose of spectroscopic studies is to understand the nature of the nuc ...
Nonlinear optical spectroscopy of single, few, and many molecules
Nonlinear optical spectroscopy of single, few, and many molecules

5150119
5150119

... Recently, photonic generation of RF, microwave and millimeterwave signals has been widely studied. This technique uses the optical fiber as the transmission medium for considerably stable carriers that are generated in a wide range of RF and microwave frequencies, with applications on mobile communi ...
Superconducting phase qubit coupled to a nanomechanical resonator:
Superconducting phase qubit coupled to a nanomechanical resonator:

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Two-dimensional nuclear magnetic resonance spectroscopy

Two-dimensional nuclear magnetic resonance spectroscopy (2D NMR) is a set of nuclear magnetic resonance spectroscopy (NMR) methods which give data plotted in a space defined by two frequency axes rather than one. Types of 2D NMR include correlation spectroscopy (COSY), J-spectroscopy, exchange spectroscopy (EXSY), and nuclear Overhauser effect spectroscopy (NOESY). Two-dimensional NMR spectra provide more information about a molecule than one-dimensional NMR spectra and are especially useful in determining the structure of a molecule, particularly for molecules that are too complicated to work with using one-dimensional NMR.The first two-dimensional experiment, COSY, was proposed by Jean Jeener, a professor at the Université Libre de Bruxelles, in 1971. This experiment was later implemented by Walter P. Aue, Enrico Bartholdi and Richard R. Ernst, who published their work in 1976.
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