Effect of changes in pH of the medium on electrical activity of the Ranvier node

Belyaev, V. I.

doi:10.1007/bf01062754

Cited by 14 publications

(15 citation statements)

References 12 publications

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“…Using the replacements given in Eq. (15), one can easily obtain the expressions for the invariant functions Π B i for the p Ã , n Ã , Σ þÃ , Σ −Ã , Ξ 0Ã , and Σ −Ã baryons: …”

Section: Appendix A: Photon Distribution Amplitudesmentioning

confidence: 99%

Magnetic moments ofJP=32−baryons in QCD

Aliev

Savcı

2014

Phys. Rev. D

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The magnetic moments of the low lying, negative parity, spin-3=2 baryons, including the Λ Ã baryon, are calculated within the light cone QCD sum rules method. The contributions coming from the positive parity, spin-3=2 baryons, as well as from the positive and negative parity spin-1=2 baryons are eliminated by constructing combinations of various invariant amplitudes corresponding to the coefficients of the different Lorentz structures. We also present the results for the magnetic moments of the positive parity, spin-3=2 baryons.

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Section: Appendix A: Photon Distribution Amplitudesmentioning

confidence: 99%

Magnetic moments ofJP=32−baryons in QCD

Aliev

Savcı

2014

Phys. Rev. D

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“…We generate signal events for each operator using Comphep [17,18] and shower them with Pythia [19] with the help of the Comphep-Pythia interface [20]. Detector effects are simulated using PGS [21] with the CDF detector model.…”

Section: Collider Constraintsmentioning

confidence: 99%

Constraints on light Majorana dark matter from colliders

Goodman¹,

Ibe²,

Rajaraman³

et al. 2011

Physics Letters B

363

380

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We explore model-independent collider constraints on light Majorana dark matter particles. We find that colliders provide a complementary probe of WIMPs to direct detection, and give the strongest current constraints on light DM particles. Collider experiments can access interactions not probed by direct detection searches, and outperform direct detection experiments by about an order of magnitude for certain operators in a large part of parameter space. For operators which are suppresssed at low momentum transfer, collider searches have already placed constraints on such operators limiting their use as an explanation for DAMA. * *

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“…The difficulty in observing the extra singlet states, s or a, is a consequence of their tiny couplings to SM particles unless their mixing with the doublet states are substantial. The LHC potential for probing the Higgs sector of singlet extensions of the MSSM, including the NMSSM, was explored in [17][18][19][46][47][48][49][50][51] with emphasis on the light Higgs doublet/singlet. The production of the heavy states was not considered.…”

Section: Introductionmentioning

confidence: 99%

Precision measurements, dark matter direct detection and LHC Higgs searches in a constrained NMSSM

Bélanger¹,

Hugonie²,

Pukhov³

2009

J. Cosmol. Astropart. Phys.

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We reexamine the constrained version of the Next-to-Minimal Supersymmetric Standard Model with semi universal parameters at the GUT scale (CNMSSM). We include constraints from collider searches for Higgs and susy particles, upper bound on the relic density of dark matter, measurements of the muon anomalous magnetic moment and of B-physics observables as well as direct searches for dark matter. We then study the prospects for direct detection of dark matter in large scale detectors and comment on the prospects for discovery of heavy Higgs states at the LHC.

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Effect of changes in pH of the medium on electrical activity of the Ranvier node

Cited by 14 publications

References 12 publications

Magnetic moments ofJP=32−baryons in QCD

Magnetic moments ofJP=32−baryons in QCD

Constraints on light Majorana dark matter from colliders

Precision measurements, dark matter direct detection and LHC Higgs searches in a constrained NMSSM

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