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Micro-machining with ultrashort laser pulses: From
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the atomic nucleus - NPAC
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... Linear and Nonlinear Absorption In case the incident wave with spectral energy density  ( )  I ( ) c And spectral width  L Which is large compared to the halfwidth of the Absorption profile  L The total intensity becomes I   I ( )d  I ( 0 ) L ...
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Low-coherence heterodyne photon correlation spectroscopy
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... To test for contributions from solvation, Raman scattering and others, we made a series of experiments in which the up-converted ¯uorescence was varied from 310 to 350 nm. As shown for TMP, for all wavelengths, the same single exponential decay to the baseline was observed with only a small di€erenc ...
Dissipative Preparation of Spin Squeezed Atomic Ensembles in a Steady States
Dissipative Preparation of Spin Squeezed Atomic Ensembles in a Steady States

... fields do not couple directly to the clock states jF ¼ 1; mF ¼ 0i and jF ¼ 2; mF ¼ 0i and therefore act as a repumping field for the proposed four-state scheme. The repump processes can be easily incorporated in our formalism in the form of additional single-atom scattering channels [29]. These proc ...
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Cofacial Dicobalt Complex of a Binucleating Hexacarboxamide Cryptand Ligand DOI: 10.1021/ic100395a
Cofacial Dicobalt Complex of a Binucleating Hexacarboxamide Cryptand Ligand DOI: 10.1021/ic100395a

... centers, ruling out the presence of a second axial ligand. The distance between the metal centers is 6.4078 Å (avg). The structure of 3 reveals that Kþ ions bridge the dicobalt cryptate units, resulting in an extended three-dimensional structure. This is in analogy to protonated cryptands, which ma ...
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... Classical and quantum computers both represent information in the form of binary digits (bit). When we use spins for representing information, we arbitrarily assign “0” to a spin up and “1” to a spin down. As shown in Figure 1, we need a sufficiently large number of spins to store the information th ...
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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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