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556
Coil sensitivity encoding for fast MRI. In:
 Proceedings of the ISMRM 6th Annual Meeting,
, 1998
"... New theoretical and practical concepts are presented for considerably enhancing the performance of magnetic resonance imaging (MRI) by means of arrays of multiple receiver coils. Sensitivity encoding (SENSE) is based on the fact that receiver sensitivity generally has an encoding effect complementa ..."
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Cited by 193 (3 self)
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configurations and kspace sampling patterns. Special attention is given to the currently most practical case, namely, sampling a common Cartesian grid with reduced density. For this case the feasibility of the proposed methods was verified both in vitro and in vivo. Scan time was reduced to onehalf using a two
Mechanistic Study of Halftitanocenebased Reductive Pinacol Coupling Reaction
, 2011
"... The reductive pinacol coupling reaction of aldehydes or ketones creating a new CC bond has been a major tool to produce 1,2diol compounds. The reaction mechanism is known to be composed of sequential three steps (activation, coupling, and dissociation). In this work, we studied the dissociation st ..."
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The reductive pinacol coupling reaction of aldehydes or ketones creating a new CC bond has been a major tool to produce 1,2diol compounds. The reaction mechanism is known to be composed of sequential three steps (activation, coupling, and dissociation). In this work, we studied the dissociation
Fivehour halflife of mouse liver gapjunction protein
 J. Cell
, 1981
"... ABSTRACT The halflife of a gapjunction polypeptide band migrating at 21,000 Mr on SDS polyacrylamide gels isolated from mouse liver is measured to be 5 h. Two lowmolecular weight bands, probably related to the 21,000 Mr material by proteolysis, have measured halflives of 4.6 and 5.2 h. Gap juncti ..."
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Cited by 25 (6 self)
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ABSTRACT The halflife of a gapjunction polypeptide band migrating at 21,000 Mr on SDS polyacrylamide gels isolated from mouse liver is measured to be 5 h. Two lowmolecular weight bands, probably related to the 21,000 Mr material by proteolysis, have measured halflives of 4.6 and 5.2 h. Gap
I Renormalization of the 2point function of the Hubbard model at halffilling
, 2008
"... We prove that the Hubbard model at finite temperature T and halffilling is analytic in its coupling constant λ for λ  ≤ c/log T  2, where c is some numerical constant. We also bound the selfenergy and prove that the Hubbard model at halffilling is not a Fermi liquid (in the mathematically pr ..."
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Cited by 5 (3 self)
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We prove that the Hubbard model at finite temperature T and halffilling is analytic in its coupling constant λ for λ  ≤ c/log T  2, where c is some numerical constant. We also bound the selfenergy and prove that the Hubbard model at halffilling is not a Fermi liquid (in the mathematically
A Theoretical Study of the Mechanism for the Reductive HalfReaction of Pea Seedling
, 2000
"... On the basis of a large amount of experimental information, the reductive halfreaction of PSAO has been studied quantum mechanically using hybrid density functional theory (B3LYP). The suggested mechanism agrees very well with the one suggested experimentally and incorporates the observation of two ..."
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Cited by 2 (1 self)
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On the basis of a large amount of experimental information, the reductive halfreaction of PSAO has been studied quantum mechanically using hybrid density functional theory (B3LYP). The suggested mechanism agrees very well with the one suggested experimentally and incorporates the observation
Inverse Problem of Velocity Reconstruction in Weakly Lateral Heterogeneous Halfspace
"... Abstract A wave propagation generated by a boundary source into a weakly lateral heterogeneous medium (WLHM) occupying a halfspace is considered in the acoustic approximation. WLHM means that the velocity of the wave propagation depends weakly on the horizontal coordinates in comparison with the s ..."
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solution of a coupled linear system of Volterratype integral equations. We demostrate the effectiveness of the approach in numerical applications in the 2D case. 1.
The two dimensional Hubbard Model at halffilling: I. Convergent Contributions, Journ. Stat. Phys. Vol 106
 Ann. Henri Poincaré
, 2002
"... We prove analyticity theorems in the coupling constant for the Hubbard model at halffilling. The model in a single renormalization group slice of index i is proved to be analytic in λ for λ  ≤ c/i for some constant c, and the skeleton part of the model at temperature T (the sum of all graphs wit ..."
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Cited by 10 (7 self)
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We prove analyticity theorems in the coupling constant for the Hubbard model at halffilling. The model in a single renormalization group slice of index i is proved to be analytic in λ for λ  ≤ c/i for some constant c, and the skeleton part of the model at temperature T (the sum of all graphs
SpinWave Excitations of HalfFilled Kondo Lattice Model
, 1998
"... The spin excitations in the antiferromagnetic phase of halffilled Kondo lattice model are studied by means of the decoupling approximation for spin Green’s function. The spinwave spectrum is calculated as a function of Kondo coupling, and this is used to calculate the thermodynamic quantities at l ..."
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The spin excitations in the antiferromagnetic phase of halffilled Kondo lattice model are studied by means of the decoupling approximation for spin Green’s function. The spinwave spectrum is calculated as a function of Kondo coupling, and this is used to calculate the thermodynamic quantities
The Superconducting Instabilities of the non halffilled Hubbard Model in Two Dimensions
, 1995
"... The problem of weakly correlated electrons on a square lattice is formulated in terms of oneloop renormalization group. Starting from the action for the entire Brillouin zone (and not with a lowenergy effective action) we reduce successively the cutoff Λ about the Fermi surface and follow the reno ..."
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corresponds to the B2 representation (dxy symmetry), while near half filling the strongest attraction occurs in the B1 representation (dx2−y2 symmetry). In the direction of the van Hove singularities, the order parameter shows peaks with increasing strength as one approaches half filling. Using the form
epl draft Metallicity in the halffilled HolsteinHubbard model
, 808
"... PACS 71.30.+h – Metal insulator transitions and other electronic transitions PACS 71.10.HF – NonFermiliquid ground states, electron phase diagrams and phase transitions in model systems PACS 71.38.k – Polarons and electronphonon interactions Abstract. We reexamine the Peierls insulator to Mott ..."
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(HHM) is particularly rewarding to study. [5–14] It accounts for a tightbinding electron band, an intrasite Coulomb repulsion between electrons of opposite spin, a local coupling of the charge carriers to optical phonons, and the energy of the phonon subsystem in harmonic approximation: H = −t ∑ c †
Results 1  10
of
556