### Patents Record file:///C:/WIMR/remote_copy/faculty/documents/patents/NMR_sca...

"... An NMR zeugmatographic scanner is modified to produce flow images. A motion sensitizing gradient field is applied to the gyromagnetic nuclei after transverse excitation and prior to emission measurement. The motion sensitized free induction signal which results is processed using an inverse Fourier ..."

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by applying a

*transverse*excitation signal to a gyromagnetic material and to thereby impart a*transverse**magnetic**moment**thereto*, and which produces a FID signal responsive to emissions by the*transversely**magnetized*gyromagnetic material, the improvement comprising: means for locating the position###
Two-dimensional method of *moments* modelling of lossless overmoded *transverse* *magnetic* cavities

, 2004

"... ..."

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The tau weak-*magnetic* dipole *moment*

, 1994

"... We calculate the prediction for the anomalous weak-magnetic form factor within the Standard Model. With all par-of the tau lepton at q2 = M2 Z ticles on-shell, this is a electroweak gauge invariant quantity. Its value is aw τ (M2 Z) = − (2.10 + 0.61 i) × 10−6. We show that the transverse and norm ..."

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We calculate the prediction for the anomalous weak-

*magnetic*form factor within the Standard Model. With all par-of the tau lepton at q2 = M2 Z ticles on-shell, this is a electroweak gauge invariant quantity. Its value is aw τ (M2 Z) = − (2.10 + 0.61 i) × 10−6. We show that the*transverse*###
Anomalous Chromomagnetic *Moments* of Quarks and Large *Transverse* Energy Jets

, 2008

"... We consider the jet cross sections for gluons coupling to quarks with an anomalous chromomagnetic moment. We then apply this to the deviation and bounds from QCD found in the CDF and D0 Fermilab data, respectively, to find a range of possible values for the anomalous moments. The quadratic and quart ..."

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and quartic terms in the anomalous

*moments*can fit to the rise of a deviation with*transverse*energy. Since previous analyses have been done on the top quark total cross section, here we assume the same*moment*on all quarks except the top and find the range |κ ′ | ≡ |κ/(2mq) | = 1.0 ± 0.3 TeV −1###
1 Markov-Yukawa *Transversality* On Covariant Null-Plane: Baryon Form Factor And *Magnetic* *Moments*

, 2008

"... The baryon-qqq vertex function governed by the Markov-Yukawa Transversality Principle (MY TP), is formulated via the Covariant Null-Plane Ansatz (CNPA) as a 3-body generalization of the corresponding q¯q problem, and employed to calculate the proton e.m. form factor and baryon octet magnetic moments ..."

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The baryon-qqq vertex function governed by the Markov-Yukawa

*Transversality*Principle (MY TP), is formulated via the Covariant Null-Plane Ansatz (CNPA) as a 3-body generalization of the corresponding q¯q problem, and employed to calculate the proton e.m. form factor and baryon octet*magnetic*###
The Neutrino *Magnetic* *Moment* at a Nuclear Reactor

, 1997

"... experiments MUNU will have a low electron energy threshold (of a few 100 keV) and will measure both the angle and the energy of 17 the recoil electron, thus providing a rough measurement of the incident neutrino energy [3, 4]. We will also measure the Weinberg angle at a very low Q 2 with a preci ..."

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(TPC), filled with CF 4 gas at 5 bar. The coordinate z along the field direction is determined by the drift time. The

*transverse*coordinates x and y are measured by (2\Theta256) cathode strips with a pitch of 3.5 mm. The TPC is shielded by liquid scintillator to suppress<F12.6###
SOME ASPECTS OF *TRANSVERSITY* ∗

, 1995

"... The specificities of transverse polarization with respect to helicity of ultrarelativistic fermions are pointed out. For massless fermions, a covariant transversity four-vector is defined, up to a kind of gauge transformation. The tranversity distribution of quarks in a nucleon is defined. Its possi ..."

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possible connection to the

*magnetic*or electric dipole*moment*of the baryon is conjectured. Consequences of the approximate chiral invariance on*transverse*spin asymmetries in hard processes are enumerated. The ”sheared jet effect ” introduced by Collins for measuring the*transverse*polarization of a final###
Derivation of the Proton’s *Magnetic* *Moment* beyond QED and QCD Theories

, 2008

"... Abstract. The first precise derivation of the proton’s magnetic moment based on the Dynamic Model of Elementary Particles (DM), beyond quantum electro- and chromodynamics, is presented in this paper. Longitudinal and transversal exchange interactions and corresponding to them longitudinal and transv ..."

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Abstract. The first precise derivation of the proton’s

*magnetic**moment*based on the Dynamic Model of Elementary Particles (DM), beyond quantum electro- and chromodynamics, is presented in this paper. Longitudinal and*transversal*exchange interactions and corresponding to them longitudinal###
The Ising-Kondo lattice with *transverse* field: an f-*moment* Hamiltonian for URu2Si2?

, 1996

"... We study the phase diagram of the Ising-Kondo lattice with transverse magnetic field as a possible model for the weak-moment heavy-fermion compound URu2Si2, in terms of two low-lying f singlets in which the uranium moment is coupled by on-site exchange to the conduction electron spins. In the mean-f ..."

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We study the phase diagram of the Ising-Kondo lattice with

*transverse**magnetic*field as a possible model for the weak-*moment*heavy-fermion compound URu2Si2, in terms of two low-lying f singlets in which the uranium*moment*is coupled by on-site exchange to the conduction electron spins. In the mean###
USM-TH-198 Connection between the Sivers function and the anomalous *magnetic* *moment*

, 2006

"... The same light-front wave functions of the proton are involved in both the anomalous magnetic moment of the nucleon and the Sivers function. Using the diquark model, we derive a simple relation between the anomalous magnetic moment and the Sivers function, which should hold in general with good appr ..."

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momentum, anomalous

*magnetic**moment*, Sivers function,*transverse*spin The quark orbital angular momentum [1] (or quark*transverse*motion) plays an important role for understanding the spin and quark structure of the nucleon, since as shown by many studies [2,3,4,5,6,7], it is the missing block of the total