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ICTP Lectures - IAEA-NDS
ICTP Lectures - IAEA-NDS

PHY303 1 TURN OVER PHY303 Data Provided: A formula sheet
PHY303 1 TURN OVER PHY303 Data Provided: A formula sheet

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Many-body interactions in the quantum well under strong optical
Many-body interactions in the quantum well under strong optical

Full-text PDF - Verlag der Zeitschrift für Naturforschung
Full-text PDF - Verlag der Zeitschrift für Naturforschung

Principles of Technology
Principles of Technology

... a. The stability of a nucleus is tied to the existence of two nuclear forces. b. These forces, called the strong and weak interactions, are much more powerful at the very small distances present within the nucleus than are gravitational or electromagnetic forces. c. At larger distances, however, the ...
A >200 meV Uphill Thermodynamic Landscape for Radical
A >200 meV Uphill Thermodynamic Landscape for Radical

Modulation instability for a relaxational Kerr medium Xue Liu , S.M. Shahriar
Modulation instability for a relaxational Kerr medium Xue Liu , S.M. Shahriar

Liquid State NMR Quantum Computing
Liquid State NMR Quantum Computing

... rotations in the proper way.8 – 10 In summary, spin-1/2 nuclei in a molecule can serve as bits in a computer, while pulses and delay times provide universal logic gates. ...
An Optical Pulse Generator from a Sinusoidal Optical Signal Using
An Optical Pulse Generator from a Sinusoidal Optical Signal Using

... varied around the fRES = 103 MHz. The latter is calculated from (1) using L1 = 401.0 cm, L2 = 597.5 cm and neff = 1.46. An integer number of analogue cycles should match with L1 and L2 simultaneously. A simple calculation leads to fRES1 = 103 MHz, fRES2 = 1.03 GHz and so on, remembering that an inte ...
Effective Charge Transfer Distances in Cyanide
Effective Charge Transfer Distances in Cyanide

PPT - jick.net
PPT - jick.net

Direct observation of light focusing by single photoreceptor cell nuclei
Direct observation of light focusing by single photoreceptor cell nuclei

QM Chemical Shift Calculations to Infer on the Long
QM Chemical Shift Calculations to Infer on the Long

Electromagnetically induced transparency
Electromagnetically induced transparency

Plasmonic waveguide filters with nanodisk resonators
Plasmonic waveguide filters with nanodisk resonators

Hyperbolic Secant Squared Pulse Shape
Hyperbolic Secant Squared Pulse Shape

... The dependence of the refractive index on wavelength has two effects on a pulse, one in space and the other in time. Dispersion disperses a pulse in space (angle): “Angular dispersion” ...
Chemistry Olympiad Support Booklet
Chemistry Olympiad Support Booklet

Matter-Wave Metrology as a Complementary Tool for Mass
Matter-Wave Metrology as a Complementary Tool for Mass

... employed as a complementary tool for mass spectroscopy where fragmentation might occur in either the source or the ionization process. Our method is based on the fact that the molecular polarizability is often a good indicator of the number of constituents in the molecule. The interference fringe co ...
Title Goes Here
Title Goes Here

... spectra. We should notice that the inhomogeneous broadening is small (0.9 meV) and the temperature is low (5-8 K), which are favorable conditions for strong FES effects. Even under these conditions, the FES effect was found to be weak. This indicates that the strength of FES effects are governed by ...
440400 - IDEALS @ Illinois
440400 - IDEALS @ Illinois

... “....Electrostatics is dominant in strong hydrogen bonds, where it contributes 60-70 per cent of the attractive terms. In weak hydrogen bonds, the relative contribution of electrostatics is smaller, and in the weakest C-H..O bonds,....., the electrostatic term can be of the same magnitude or even sm ...
Strong critical coupling and polaritonic coherent perfect
Strong critical coupling and polaritonic coherent perfect

J. Am. Chem. SOC. 1993,115, 7685-7695
J. Am. Chem. SOC. 1993,115, 7685-7695

Probing vibrational ladder-excitation in CO2 microwave plasma with a free electron laser to develop a route to efficient solar fuels
Probing vibrational ladder-excitation in CO2 microwave plasma with a free electron laser to develop a route to efficient solar fuels

Analysis of Fundamental and Higher Order
Analysis of Fundamental and Higher Order

< 1 ... 34 35 36 37 38 39 40 41 42 ... 70 >

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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