Quantum Correlations in NMR systems

In conventional NMR experiments, the Zeeman energy gaps of the nuclear spin ensembles are much lower than their thermal energies, and accordingly exhibit tiny polarizations. Generally such low-purity quantum states are devoid of quantum entanglement. However, there exist certain nonclassical correlations which can be observed even in such systems. In this chapter, we discuss three such quantum correlations, namely, quantum contextuality, Leggett-Garg temporal correlations, and quantum discord. In each case, we provide a brief theoretical background and then describe some results from NMR experiments.Comment: 21 pages, 7 figure

Denial of long-term issues with agriculture on tropical peatlands will have devastating consequences

Lette

Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector

A measurement of the mass of the W boson is presented based on proton–proton collision data recorded in 2011 at a centre-of-mass energy of 7 TeV with the ATLAS detector at the LHC, and corresponding to 4.6 fb−1 of integrated luminosity. The selected data sample consists of 7.8 × 106 candidates in the W → μν channel and 5.9 × 106 candidates in the W → eν channel. The W-boson mass is obtained from template fits to the reconstructed distributions of the charged lepton transverse momentum and of the W boson transverse mass in the electron and muon decay channels, yielding mW = 80370 ± 7 (stat.) ± 11(exp. syst.) ± 14 (mod. syst.) MeV = 80370 ± 19 MeV, where the first uncertainty is statistical, the second corresponds to the experimental systematic uncertainty, and the third to the physics-modelling systematic uncertainty. A measurement of the mass difference between the W+ and W− bosons yields mW+ − mW− = − 29 ± 28 MeV

Measurement of the W-boson mass in pp collisions at s√=7TeV with the ATLAS detector

A measurement of the mass of the W boson is presented based on proton–proton collision data recorded in 2011 at a centre-of-mass energy of 7 TeV with the ATLAS detector at the LHC, and corresponding to 4.6 fb−1 of integrated luminosity. The selected data sample consists of 7.8×106 candidates in the W→μν channel and 5.9×106 candidates in the W→eν channel. The W-boson mass is obtained from template fits to the reconstructed distributions of the charged lepton transverse momentum and of the W boson transverse mass in the electron and muon decay channels, yielding mW=80370=80370±7 (stat.)±11(exp. syst.)±14 (mod. syst.) MeV±19MeV, where the first uncertainty is statistical, the second corresponds to the experimental systematic uncertainty, and the third to the physics-modelling systematic uncertainty. A measurement of the mass difference between the W+ and W− bosons yields mW+−mW−=−29±28 MeV

Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector

A measurement of the mass of the W boson is presented based on proton–proton collision data recorded in 2011 at a centre-of-mass energy of 7 TeV with the ATLAS detector at the LHC, and corresponding to 4.6 fb−14.6 fb−1 of integrated luminosity. The selected data sample consists of 7.8×1067.8×106 candidates in the W→μνW→μν channel and 5.9×1065.9×106 candidates in the W→eνW→eν channel. The W-boson mass is obtained from template fits to the reconstructed distributions of the charged lepton transverse momentum and of the W boson transverse mass in the electron and muon decay channels, yielding mW=80370=80370±7 (stat.)±11(exp. syst.)±14 (mod. syst.) MeV±19MeV, mW=80370±7 (stat.)±11(exp. syst.)±14 (mod. syst.) MeV=80370±19MeV, where the first uncertainty is statistical, the second corresponds to the experimental systematic uncertainty, and the third to the physics-modelling systematic uncertainty. A measurement of the mass difference between the W+W+ and W−W− bosons yields mW+−mW−=−29±28mW+−mW−=−29±28 MeV

Comparative Efficacy of Four Different Solid Phase Extraction Cartridges Used to Determine Tetracycline in Foods of Animal Origin

Four different types of Solid Phase Extraction (SPE) cartridges namely R-Biopharm (RB), Chromabond (CB), Isolute (IS) and Megabond (MB) were used in this study. Control and spiked samples of beef, chicken and shrimp were also used. Optical Density (OD) values of control and spiked samples were measured with the help of Enzyme Linked Immunosorbent Assay (ELISA) reader. Percent binding values for each SPE cartridges were calculated using OD values of respective control and spiked samples. Based on % binding values a comparative study of 4 different Solid Phase Extraction (SPE) cartridges was carried out. Analysis of variance indicated no significant differences among the % binding values considering different samples irrespective of SPE cartridges (P=0.821266, F = 0.201279) or different SPE cartridges irrespective of samples (P = 0.168119, F = 2.180932). From this study, it can be recommended that any of the four SPE cartridges available in the working area can be used for the analysis of tetracycline from foods of animal origin.DOI: http://dx.doi.org/10.3329/bjvm.v13i1.23727Bangl. J. Vet. Med. (2015). 13 (1): 89-91</jats:p