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Overview Density functional calculations of NMR chemical shifts and
Overview Density functional calculations of NMR chemical shifts and

In Situ Raman Spectroscopic Study of Gypsum (CaSO4·2H2O) and
In Situ Raman Spectroscopic Study of Gypsum (CaSO4·2H2O) and

A high-field solid-state Cl NMR and quantum chemical
A high-field solid-state Cl NMR and quantum chemical

Schroedinger`s cat states generated by the environment
Schroedinger`s cat states generated by the environment

... photons [7, 8]. Alternatively, large spin characterizes macroscopic atomic ensembles that are entangled via interaction with a common light source [9]. The weakness of their interactions with the environment renders large-spin ensembles robust against decoherence and thus makes them good candidates ...
I. Results from Prior NSF Support
I. Results from Prior NSF Support

... echo point where a weak laser beam records the time variation of the matter wave interference pattern by reflection. is time measured from the echo point. In our interferometer (Fig 1), an expanded sodium BEC is split into three momentum states. by a short 1s Kapitza-Dirac diffraction light pulse ...
SHS_OH_flame_ApplOpt_revision_RJB
SHS_OH_flame_ApplOpt_revision_RJB

Producing Squeezed Input States for an Atomic Clock Using an Optical Cavity.
Producing Squeezed Input States for an Atomic Clock Using an Optical Cavity.

Microscopic quantum coherence in a photosynthetic-light
Microscopic quantum coherence in a photosynthetic-light

Amorphous to Tetragonal Zirconia
Amorphous to Tetragonal Zirconia

... spectral positions of these peaks, however, cannot be attributed to any specific ionic state, due to the finite uncertainty involved in deconvolution in the background of complex envelop of density of states. Hence, these peaks are referred to Zr+ζ, 0 ≤ |ζ| < 4, with varying (2.8−3.2 eV) spin orbit sp ...
Synchronized ti scattering microscopy
Synchronized ti scattering microscopy

Analytical Chemistry
Analytical Chemistry

Nonlinear effects in Silicon Waveguides
Nonlinear effects in Silicon Waveguides

... • Experimental data in agreement with numerical predictions. ...
Ligand Conformation Enforces Trigonal
Ligand Conformation Enforces Trigonal

Crystal structure and spectroscopic properties of [Zn(2-qmpe)Cl ] containing diethyl (quinolin-2-ylmethyl)phosphonate ligand (2-qmpe)
Crystal structure and spectroscopic properties of [Zn(2-qmpe)Cl ] containing diethyl (quinolin-2-ylmethyl)phosphonate ligand (2-qmpe)

Detection Sensitivity of Single-Molecule Optical Absorption at Room
Detection Sensitivity of Single-Molecule Optical Absorption at Room

On the Annihilation Cross Section of the Antinucleon and the Nucleon
On the Annihilation Cross Section of the Antinucleon and the Nucleon

Atom “Pinhole Camera” with Nanometer Resolution
Atom “Pinhole Camera” with Nanometer Resolution

Short-pulse limits in optical instrumentation design for the S
Short-pulse limits in optical instrumentation design for the S

Hyperfine Structure in the Rotational Spectrum of GaF: A
Hyperfine Structure in the Rotational Spectrum of GaF: A

Acta Chim. Slov. 2000, 47, 179−185. 179 Co(II), Ni(II) and Cu(II
Acta Chim. Slov. 2000, 47, 179−185. 179 Co(II), Ni(II) and Cu(II

Paper
Paper

Pulsed-laser ablation of Mg in liquids: surfactant
Pulsed-laser ablation of Mg in liquids: surfactant

... plasma and liquid will lead to the formation of magnesium hydroxides (Mg + 2H2 O!Mg(OH)2 + 2H ). The increase in the amount of Mg(OH)2 also caused the free hydroxyl ions in the liquid to increase gradually through relatively slow dissolution of Mg(OH)2 (Mg(OH)2 () Mg2þ + 2OH ), leading to an incre ...
Generation of arbitrary Dicke states in spinor Bose±Einstein
Generation of arbitrary Dicke states in spinor Bose±Einstein

... this need not be the case. In order to create squeezed states with arbitrary prescribed value of hJ^z i ˆ m0 and arbitrary Dicke states, we propose to use instead the following method: ®rst, a coupling pulse of appropriate strength is applied to the ground state jj; ji, creating an initial CSS with ...
Generation of relativistic intensity pulses at a kilohertz
Generation of relativistic intensity pulses at a kilohertz

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

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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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