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Size-Selective Hydrogenation of Olefins by Dendrimer
Size-Selective Hydrogenation of Olefins by Dendrimer

Physical Properties of Macromolecules Glass Transitions in Amorphous Polymers
Physical Properties of Macromolecules Glass Transitions in Amorphous Polymers

X-rays as a branch of optics A C Nobel Lecture, December 12, 1927
X-rays as a branch of optics A C Nobel Lecture, December 12, 1927

Sensitivity Analysis of a Position Device with Quadrant Photodiode
Sensitivity Analysis of a Position Device with Quadrant Photodiode

Novel Metrology Techniques Resolve Strong-Field
Novel Metrology Techniques Resolve Strong-Field

Abstract :soliton order N=1 and N=2 results are also obtained
Abstract :soliton order N=1 and N=2 results are also obtained

... order Soliton, optimum compression was done for input powers of several hundred watts. These results were at least in semi quantitative agreement with the nonlinear Schrödinger equation based prediction [8].C.R. Menyuk(et.al) (1987)was the first to derive the nonlinear pulse propagation equation und ...
Entanglement Spectrum in the Fractional Quantum Hall Effect
Entanglement Spectrum in the Fractional Quantum Hall Effect

... In particular the FQHE exhibits a new type of order different from the classical or quantum orders that can be described by the paradigm of Landau’s symmetry breaking theory. This new type of order is robust upon local perturbations and cannot be described by a symmetry or a broken symmetry. In part ...
Optical spectroscopy and electronic structure of the face-centered icosahedral quasicrystals Zn- R
Optical spectroscopy and electronic structure of the face-centered icosahedral quasicrystals Zn- R

blah
blah

... recorded in the thin InSe flakes, which supports the physical origin of each one of the P1–P6 components discussed in the main text. (ii) The -PL spectra obtained in terraces with similar thickness can be deconvoluted into P1–P6 components whose relative intensities appear to differ from flake to f ...
1/2
1/2

Separation of 2 (3), 9 (10), 16 (17), 23 (24)
Separation of 2 (3), 9 (10), 16 (17), 23 (24)

Ten Years of Spin Hall Effect
Ten Years of Spin Hall Effect

... The most striking feature of this result is its universality. Although the effect arises from random collisions of electrons with impurities (and possibly with other electrons), the average drift is controlled only by the average rate of momentum transfer, which in turn depends only on the applied e ...
Femtosecond Laser Pulses: Linear Properties
Femtosecond Laser Pulses: Linear Properties

Metal-to-ligand and ligand-to-metal charge transfer in thin films of
Metal-to-ligand and ligand-to-metal charge transfer in thin films of

... absorption spectra, experimental XAS spectra were modelled using the so-called ligand field multiplet (LFM) theory developed by Thole21 in the framework established by Cowan22 and Butler.23 This approach takes into account all the electronic Coulomb interactions as well as the spin–orbit coupling on ...
Coupling ultracold atoms to mechanical oscillators
Coupling ultracold atoms to mechanical oscillators

... Alternatively, one can increase the effective mass of the atoms by using a large number of them. Such collective enhancement is a promising route to achieve strong coupling mediated by an optical lattice (Sec. 5). For the perspective of creating a coupled quantum system where the mechanical oscillat ...
3D locations of the object directly from in
3D locations of the object directly from in

Dynamics and Excited States of Quantum Many
Dynamics and Excited States of Quantum Many

Sub-THz Electron Spin Resonance spectroscopy based on a Martin
Sub-THz Electron Spin Resonance spectroscopy based on a Martin

... to account for wavelength phase changes in very broad scans or to compensate unwanted standing wave modes. ESR detection and standing wave management. The signals returning from paramagnetic samples carry a rotated polarization which is the only component of the returning beam that is reflected by t ...
Frequency comb generation by CW laser injection
Frequency comb generation by CW laser injection

The 9th Asia Pacific
The 9th Asia Pacific

... Coupling efficiency between a SMF and a waveguide whose transverse intensity distributions are gaussian depends on the mismatch between their MFD. As the coupling efficiency is the overlap integral between the two field amplitudes, it is the higher when the two fields are the same and decreases with ...
LETTERS
LETTERS

... Fig. 4. The orbit of the wave packets agrees with the classical equations of motion in our harmonic trap with its incommensurate frequencies [24]. In summary, we have demonstrated coherent Bragg diffraction of Bose-Einstein condensed sodium atoms. This technique, demonstrated both with and without t ...
Frequency-resolved optical gating with the use of second
Frequency-resolved optical gating with the use of second

Single-photon multiple ionization processes studied by electron coincidence spectroscopy Per Linusson
Single-photon multiple ionization processes studied by electron coincidence spectroscopy Per Linusson



... As with 2x2 ray matrices, consider each element to correspond to a small deviation from its mean value (xin = x – x0 ). So we can think in terms of partial derivatives. the usual 2x2 ...
[pdf]
[pdf]

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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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