Journal articles: 'Massey Twp'

1

Anderson, C. "Massey Leaving NSF for Top UC Job." Science 259, no. 5096 (February 5, 1993): 754. http://dx.doi.org/10.1126/science.259.5096.754.

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2

Langacker, Paul. "Neutrino Masses from the Top Down." Annual Review of Nuclear and Particle Science 62, no. 1 (November 23, 2012): 215–35. http://dx.doi.org/10.1146/annurev-nucl-102711-094925.

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3

Follett, Kenneth A. "Intrathecal Analgesia and Catheter-tip Inflammatory Masses." Anesthesiology 99, no. 1 (July 1, 2003): 5–6. http://dx.doi.org/10.1097/00000542-200307000-00004.

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4

Dobrescu, Bogdan A., and Patrick J. Fox. "Quark and lepton masses from top loops." Journal of High Energy Physics 2008, no. 08 (August 28, 2008): 100. http://dx.doi.org/10.1088/1126-6708/2008/08/100.

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5

Blöcker, T., F. Herwig, T. Driebe, H. Bramkamp, and D. Schönberner. "From Planetary Nebula nuclei to white dwarfs: The impact of evolutionary envelope masses." Symposium - International Astronomical Union 180 (1997): 389. http://dx.doi.org/10.1017/s0074180900131511.

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It is well known that the evolution of white dwarfs (WDs) depends sensitively on the question whether they have “thin” or “thick” envelopes of H and He (see Wood 1995). Standard evolutionary caluclations (e.g. Paczynksi 1971) show that at the tip of the Asymptotic Giant Branch the envelope masses are tightly correlated with the mass of the hydrogen exhausted core (≈ total mass). Accordingly, the masses of hydrogen, MH, and helium, MHe, on top of the degenerate C/O interiors decrease by orders of magnitudes with increasing stellar mass. In contrast, many applications of WD calculations consider only single values of qH,He = log(MH,He/M∗) asuming either “thick” or “thin” envelopes.

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6

Jhas, Sumit, and Sagun Tuli. "Intrathecal catheter-tip inflammatory masses: an intraparenchymal granuloma." Journal of Neurosurgery: Spine 9, no. 2 (August 2008): 196–99. http://dx.doi.org/10.3171/spi/2008/9/8/196.

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The authors report the case of a 54-year-old woman who presented with an intraparenchymal granuloma in her lower thoracic spinal cord. On imaging studies there was an intramedullary enhancement at the left dorsal aspect of the cord immediately adjacent to the tip of an intrathecal arachnoid catheter used for intraspinal drug therapy. At surgery, it was apparent that once this superficial component of the catheter and inflammatory mass was removed, there was a granulomatous component that extended into the spinal cord. A 5-mm caseating chalklike granuloma was carefully dissected away. To the authors' knowledge, this is the first reported case of an intrathecal catheter-tip granuloma growing inside the spinal cord parenchyma.

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7

MA, ERNEST. "FIXING THE TOP-QUARK AND HIGGS-BOSON MASSES." Modern Physics Letters A 07, no. 29 (September 21, 1992): 2741–46. http://dx.doi.org/10.1142/s0217732392002202.

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If the quadratic divergence of the standard electroweak model and its local variation with mass scale are both assumed to be zero, then a modified one-loop calculation yields mt ≃ 117 GeV and mH ≃ 183 GeV . Such a scenario may be the result of an underlying theory to be revealed at a much higher mass scale.

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8

Akano, M. "Masses and structures of bottom and top mesons." Il Nuovo Cimento A 108, no. 5 (May 1995): 541–54. http://dx.doi.org/10.1007/bf02816850.

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9

Fariborz, Amir H., Renata Jora, Salah Nasri, and Joseph Schechter. "A hierarchy of the quark masses in a top condensate model with multiple Higgses." Modern Physics Letters A 29, no. 06 (February 28, 2014): 1450030. http://dx.doi.org/10.1142/s0217732314500308.

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We discuss the quark masses in a top condensate model where not only two quark but also four quark composite states may exist. We show that the presence of the top color group SU (3)1× SU (3)2 with the correct quark representations can justify even in the absence of the additional technicolor interactions a hierarchy of the quark masses where the light quarks masses have the same size, the charm and bottom masses are higher and similar and the top is the heaviest.

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10

Harris, B. A., and G. C. Joshi. "Top quark and Higgs boson masses from wormhole physics." Physical Review D 50, no. 9 (November 1, 1994): 5993–6002. http://dx.doi.org/10.1103/physrevd.50.5993.

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11

CVETIČ, G., and C. S. KIM. "FLAVOR GAUGE THEORY, AND MASSES OF TOP AND NEUTRINO." Modern Physics Letters A 09, no. 04 (February 10, 1994): 289–97. http://dx.doi.org/10.1142/s0217732394000307.

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We assume that the standard model (SM) breaks down around some energy Λ, and is replaced by a new (Higgsless) flavor gauge theory (FGT). We investigate this possibility by studying the renormalization group equations for the Yukawa couplings of SM with two Higgs doublets for various mt and υU/υD. With appropriate flavor democratic boundary conditions at Λ FGT , we derive the bounds on masses of top and tau-neutrino, which are compatible with experimental bounds.

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12

DECKER, ROGER, and JEAN PESTIEAU. "DETERMINATION OF THE TOP QUARK AND HIGGS BOSON MASSES." Modern Physics Letters A 07, no. 40 (December 28, 1992): 3773–75. http://dx.doi.org/10.1142/s0217732392003190.

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13

Deo, B. B., and L. Maharana. "Top quark and Higgs boson masses from vacuum energy." Physics Letters B 323, no. 3-4 (March 1994): 417–20. http://dx.doi.org/10.1016/0370-2693(94)91240-8.

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14

Maier, Andreas. "Heavy quark masses from production near threshold." Modern Physics Letters A 31, no. 29 (September 8, 2016): 1630029. http://dx.doi.org/10.1142/s0217732316300299.

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In this paper, we review the precision determination of the bottom and top quark masses from the total pair-production cross-section near threshold. The theory prediction of the cross-section includes QCD corrections up to third-order. We further discuss the combined impact of Higgs corrections, the QED Coulomb potential, non-resonant production, and P-wave production on the extraction of top quark properties.

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15

DECKER, ROGER, and JEAN PESTIEAU. "CANCELLATION OF ULTRAVIOLET DIVERGENCES IN THE SU(2)L×U(1) ELECTROWEAK MODEL." Modern Physics Letters A 04, no. 28 (December 30, 1989): 2733–38. http://dx.doi.org/10.1142/s0217732389003051.

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We assume that, in the SU(2)L×U(1) model, ultraviolet divergences of the charged lepton self-masses are zero. We predict the top and Higgs masses in the vicinity of the Z-boson mass. Our assumption holds only if there are no more than three generations of quarks and leptons and if quarks and leptons, except for the top quark, have negligible masses compared to the W-boson mass.

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16

Wang, Nabawy, Cioncolini, and Revell. "Solar Panels as Tip Masses in Low Frequency Vibration Harvesters." Energies 12, no. 20 (October 9, 2019): 3815. http://dx.doi.org/10.3390/en12203815.

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Tip masses are used in cantilevered piezoelectric energy harvesters to shift device resonance towards the required frequency for harvesting and to improve the electric power generation. Tip masses are typically in the form of concentrated passive weights. The aim of this study is to assess the inclusion of solar panels as active tip masses on the dynamics and power generation performance of cantilevered PVDF (polyvinylidene fluoride)-based vibration energy harvesters. Four different harvester geometries with and without solar panels are realized using off-the-shelf components. Our experimental results show that the flexible solar panels considered in this study are capable of reducing resonance frequency by up to 14% and increasing the PVDF power generated by up to 54%. Two analytical models are developed to investigate this concept; employing both an equivalent concentrated tip mass to represent the case of flexible solar panels and a distributed tip mass to represent rigid panels. Good prediction agreement with experimental results is achieved with an average error in peak power of less than 5% for the cases considered. The models are also used to identify optimum tip mass configurations. For the flexible solar panel model, it is found that the highest PVDF power output is produced when the length of solar panels is two thirds of the total length. On the other hand, results from the rigid solar panel model show that the optimum length of solar panels increases with the relative tip mass ratio, approaching an asymptotic value of half of the total length as the relative tip mass ratio increases significantly.

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17

Xue, She-Sheng. "Higgs boson and top-quark masses and parity-symmetry restoration." Physics Letters B 727, no. 1-3 (November 2013): 308–13. http://dx.doi.org/10.1016/j.physletb.2013.10.024.

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18

Braginsky, V. B., F. Ya Khalili, and P. S. Volikov. "The analysis of table-top quantum measurement with macroscopic masses." Physics Letters A 287, no. 1-2 (August 2001): 31–38. http://dx.doi.org/10.1016/s0375-9601(01)00469-8.

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19

Hassenbusch, Samuel, Kim Burchiel, Robert J. Coffey, Michael J. Cousins, Tim Deer, Marc B. Hahn, Stuart Du Pen, et al. "Management of Intrathecal Catheter-Tip Inflammatory Masses: A Consensus Statement." Pain Medicine 3, no. 4 (December 2002): 313–23. http://dx.doi.org/10.1046/j.1526-4637.2002.02055.x.

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20

Kahana, David E., and Sidney H. Kahana. "Top quark and Higgs boson masses in dynamical symmetry breaking." Physical Review D 52, no. 5 (September 1, 1995): 3065–71. http://dx.doi.org/10.1103/physrevd.52.3065.

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21

Köhler, R., T. Ratzka, M. G. Petr-Gotzens, and S. Correia. "Orbits and masses in the young triple system TWA 5." Astronomy & Astrophysics 558 (October 2013): A80. http://dx.doi.org/10.1051/0004-6361/201220560.

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22

Murphy, Paul M., and Michael J. Cousins. "Not All Intrathecal Catheter Tip MRI Findings Are Inflammatory Masses." Anesthesia & Analgesia 104, no. 6 (June 2007): 1602. http://dx.doi.org/10.1213/01.ane.0000260548.30158.c8.

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23

Coffey, Robert J., and Jeffrey W. Allen. "Not All Intrathecal Catheter Tip MRI Findings Are Inflammatory Masses." Anesthesia & Analgesia 104, no. 6 (June 2007): 1600–1602. http://dx.doi.org/10.1213/01.ane.0000260557.76884.72.

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24

ZHANG, GUO-CE, LI-QUN CHEN, and HU DING. "FORCED VIBRATION OF TIP-MASSED CANTILEVER WITH NONLINEAR MAGNETIC INTERACTIONS." International Journal of Applied Mechanics 06, no. 02 (March 17, 2014): 1450015. http://dx.doi.org/10.1142/s175882511450015x.

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This paper predicts the nonlinear relative motion of a cantilever with a tip mass and magnets based on a distributed-parameter model. The Kelvin viscoelastic model is used to account for the damping in the cantilever. Under the harmonic base excitation, the governing equation is deduced via a coordinate transformation linked to its static equilibrium. To qualitatively validate those results captured from the approximate methods, the finite difference method and the multi-scale method are respectively employed to determine the natural frequency and the steady-state response of forced vibration. It is analytically demonstrated that those modes uninvolved in a certain resonance actually have no effect on the response amplitude of the stable steady-state motion. The effects of forcing amplitude, viscoelastic damping, and tip mass on the steady-state response are detailed via the amplitude–frequency response curves. For the first time, the current works theoretically illustrated the conversion from the hardening-type behavior to the softening-type versus the augmenting magnetic force, as well as the opposing effect of different tip masses on the first mode and the higher modes.

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25

Ellwanger, U., and M. Lindner. "Constraints on new physics from the Higgs and top masses." Physics Letters B 301, no. 4 (March 1993): 365–71. http://dx.doi.org/10.1016/0370-2693(93)91164-i.

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26

Akano, M. "Masses and structures of quarks and composites of top quark." Il Nuovo Cimento A 86, no. 1 (March 1985): 11–22. http://dx.doi.org/10.1007/bf02905806.

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27

Binétruy, P., and C. A. Savoy. "Higgs and top masses in a non-minimal supersymmetric theory." Physics Letters B 277, no. 4 (March 1992): 453–58. http://dx.doi.org/10.1016/0370-2693(92)91809-n.

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28

Stamps, Robert H., and Michael R. Evans. "Growth of Dracaena marginata and Spathiphyllum `Petite' in Spaghnum Peat and Coconut Coir Dust-based Growing Media." HortScience 33, no. 3 (June 1998): 522e—522. http://dx.doi.org/10.21273/hortsci.33.3.522e.

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Dracaena marginata Lam. and Spathiphyllum `Petite' were grown in three greenhouse growing media made with Philippine coconut (Cocos nucifera L.) coir dust (CD) or Canadian sphagnum peat (SP). Three soilless media [Cornell, Hybrid, Univ. of Florida #2 (UF-2)] were prepared using CD or SP and pine bark (PB), vermiculite (V), and/or perlite (P) in the following ratios (percent by volume): Cornell = 50 CD or SP:25 V:25 P; Hybrid = 40 CD or SP:30 V:30 PB; UF-2 = 50 CD or SP:50 PB. When most of the plants of each genus were of marketable size, plant root and top masses and grades were determined as well as plant top growth indices. For dracaena, there were interactions between medium component (CD/SP) and medium type for everything except mass and grades of roots. For Cornell mix, plant top growth index and grades were higher for SP- (SPM) than the CD-containing medium (CDM). However, masses were not different due to component. For Hybrid mix, only top mass was affected (CDM 12%> SPM). For UF-2, top plant index and top and total plant masses were higher for CDM than SPM by 10, 19 and 15%, respectively. Overall, plant masses were the same for all three mixes containing CD; however, top plant index and grades were higher for the Hybrid and UF-2 mixes than for Cornell. Using SP, plants in Cornell and Hybrid mixes generally outperformed those in UF-2. For spathiphyllum, there were no interactions and medium component only affected root ratings (CDM > SPM). Plant top, root and total masses and root ratings were higher for Cornell and Hybrid than for UF-2.

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29

Maas, Dustin, Mohammad H. Firooz, Junxing Zhang, Neal Patwari, and Sneha K. Kasera. "Channel Sounding for the Masses: Low Complexity GNU 802.11b Channel Impulse Response Estimation." IEEE Transactions on Wireless Communications 11, no. 1 (January 2012): 1–8. http://dx.doi.org/10.1109/twc.2011.111611.091774.

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30

Just, K., and L. S. The. "Top and Higgs Mass from Cancellation Conditions." Zeitschrift für Naturforschung A 42, no. 3 (March 1, 1987): 241–45. http://dx.doi.org/10.1515/zna-1987-0305.

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We propose a way of connecting the masses of all those particles which couple to the “electroweak” Higgs scalar. Up to radiative corrections to be given later, we expect mt = 81 GeV and mH = 66 GeV. Our realistic (but flexible) cutoff is explained as far as needed.

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31

Kooi, Bob W., and Max Kuipers. "The Dynamics of Springboards." Journal of Applied Biomechanics 10, no. 4 (November 1994): 335–51. http://dx.doi.org/10.1123/jab.10.4.335.

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The maneuvers of a competition diver on a springboard before takeoff may serve to maximize the height of the flight phase. To simplify analysis, it is often assumed that the diver performs motions at the top of a single degree-of-freedom (DOF) system, usually consisting of one mass and one linear spring. This system is expected to simulate the behavior of the board sufficiently. In this paper we propose a new single DOF system approximating the effects of a board with passable accuracy. This model is applied to three types of springboards to obtain numerical values for their virtual masses at the tip.

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32

GLADYSHEV, A. V., and D. I. KAZAKOV. "RENORMALIZATION GROUP IMPROVED RADIATIVE CORRECTIONS TO THE SUPERSYMMETRIC HIGGS BOSON MASSES." Modern Physics Letters A 10, no. 40 (December 28, 1995): 3129–37. http://dx.doi.org/10.1142/s0217732395003288.

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The one-loop radiative corrections to the Higgs boson potential in the MSSM, originating from the top quark and squark loops, are summed in the leading log approximation using the renormalization group (RG). The RG improved effective potential is minimized and the corrections to the CP-odd and CP-even Higgs boson masses are calculated. The resulting masses exhibit smoother top mass dependence than those calculated without RG summation. We have also found that for preferable values of the top mass the light Higgs mass does not exceed 100 GeV.

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33

TERAZAWA, HIDEZUMI. "A SIMPLE RELATION AMONG THE QUARK MASSES." Modern Physics Letters A 10, no. 03 (January 30, 1995): 199–205. http://dx.doi.org/10.1142/s0217732395000235.

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Based on our recent suggestion that the first and second generations of quarks and leptons can be taken as almost and quasi Nambu–Goldstone fermions, respectively, we can derive a simple relation among the quark masses, [Formula: see text], from which the top quark mass is predicted to be mt ≅ (180±100) − (200±110) GeV .

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34

Vayonakis, C. E. "On the Unitarity Limits of Top-Quark and Higgs-Boson Masses." Europhysics Letters (EPL) 12, no. 1 (May 1, 1990): 29–33. http://dx.doi.org/10.1209/0295-5075/12/1/006.

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35

Anderson, Greg W. "New cosmological constraints on the Higgs boson and top quark masses." Physics Letters B 243, no. 3 (June 1990): 265–70. http://dx.doi.org/10.1016/0370-2693(90)90849-2.

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36

Halzen, Francis, and Duncan A. Morris. "The top quark mass from weak boson masses without neutral currents." Physics Letters B 237, no. 1 (March 1990): 107–12. http://dx.doi.org/10.1016/0370-2693(90)90471-h.

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37

Achiman, Yoav, and André Lukas. "Heavy top in an E6 model for fermionic masses and mixing." Nuclear Physics B 384, no. 1-2 (October 1992): 78–100. http://dx.doi.org/10.1016/0550-3213(92)90462-k.

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38

Blumhofer, Andreas, and Berthold Stech. "Top and Higgs masses from vacuum leaks of the standard model." Physics Letters B 293, no. 1-2 (October 1992): 137–41. http://dx.doi.org/10.1016/0370-2693(92)91492-r.

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39

Garside, William, and Nina Hillman. "The extended survival of tw5/tw5 mouse embryo cells in vitro." Genetical Research 55, no. 1 (February 1990): 21–25. http://dx.doi.org/10.1017/s0016672300025155.

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SummaryThe tw5 haplotype is a recessive mutation which is lethal when homozygous in mouse embryos following implantation. This series of studies was undertaken to determine the effect of the tw5/tw5 genotype on embryos developing in vitro. Blastocyst embryos from + / tw5inter se matings were compared with control blastocysts obtained from matings between T/ + and + / + females and + / tw5 males for their abilities to continue development in vitro in two culture media. The data show that there are no significant differences between the percentages of experimental and control blastocyst embryos which attach and outgrow or which contain inner cell masses on any day of culture up to equivalent gestation day 21 in either media. These findings show that the life span of cells from tw5 / tw5 embryos can be extended significantly by in vitro culture.

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40

Vogel, Bärbel, Rolf Müller, Gebhard Günther, Reinhold Spang, Sreeharsha Hanumanthu, Dan Li, Martin Riese, and Gabriele P. Stiller. "Lagrangian simulations of the transport of young air masses to the top of the Asian monsoon anticyclone and into the tropical pipe." Atmospheric Chemistry and Physics 19, no. 9 (May 8, 2019): 6007–34. http://dx.doi.org/10.5194/acp-19-6007-2019.

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Abstract. We have performed backward trajectory calculations and simulations with the three-dimensional Chemical Lagrangian Model of the Stratosphere (CLaMS) for two succeeding monsoon seasons using artificial tracers of air mass origin. With these tracers we trace back the origin of young air masses (age <6 months) at the top of the Asian monsoon anticyclone and of air masses within the tropical pipe (6 months < age <18 months) during summer 2008. The occurrence of young air masses (<6 months) at the top of the Asian monsoon anticyclone up to ∼460 K is in agreement with satellite measurements of chlorodifluoromethane (HCFC-22) by the Michelson Interferometer for Passive Atmospheric Sounding (MIPAS) instrument. HCFC-22 can be considered as a regional tracer for continental eastern Asia and the Middle East as it is mainly emitted in this region. Our findings show that the transport of air masses from boundary layer sources in the region of the Asian monsoon into the tropical pipe occurs in three distinct steps. First, very fast uplift in “a convective range” transports air masses up to 360 K potential temperature within a few days. Second, air masses are uplifted from about 360 K up to 460 K within “an upward spiralling range” within a few months. The large-scale upward spiral extends from northern Africa to the western Pacific. The air masses are transported upwards by diabatic heating with a rate of up to 1–1.5 K per day, implying strong vertical transport above the Asian monsoon anticyclone. Third, transport of air masses occurs within the tropical pipe up to 550 K associated with the large-scale Brewer–Dobson circulation within ∼1 year. In the upward spiralling range, air masses are uplifted by diabatic heating across the (lapse rate) tropopause, which does not act as a transport barrier, in contrast to the extratropical tropopause. Further, in the upward spiralling range air masses from inside the Asian monsoon anticyclone are mixed with air masses convectively uplifted outside the core of the Asian monsoon anticyclone in the tropical adjacent regions. Moreover, the vertical transport of air masses from the Asian monsoon anticyclone into the tropical pipe is weak in terms of transported air masses compared to the transport from the monsoon anticyclone into the northern extratropical lower stratosphere. Air masses from the Asian monsoon anticyclone (India/China) contribute a minor fraction to the composition of air within the tropical pipe at 550 K (6 %), and the major fractions are from Southeast Asia (16 %) and the tropical Pacific (15 %).

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41

Brodzik, A. K. "Phase-only filtering for the masses (of DNA Data): a new approach to sequence alignment." IEEE Transactions on Signal Processing 54, no. 6 (June 2006): 2456–66. http://dx.doi.org/10.1109/tsp.2006.873717.

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42

NAYAK, SRIPATI KUMAR, and LAMBODAR P. SINGH. "MODIFIED BAG MODEL AND t-FLAVORED HADRON SPECTROSCOPY." International Journal of Modern Physics A 06, no. 24 (October 10, 1991): 4331–40. http://dx.doi.org/10.1142/s0217751x91002082.

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Masses of t-flavored hadrons have been computed using a modified bag model well suited for considering heavy quarks inside the bag. Results have been obtained for mt=50 GeV and 150 GeV as representative masses of the light and heavy top scenarios.

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43

Zhuang, Duanyang, Ke Ma, Chunan Tang, Zhengzhao Liang, and Zhenwei Wang. "Microseismic Monitoring of Energy Changes in Deep Tunnels during the TBM Tunneling of the Jinping II Hydropower Station." Advances in Civil Engineering 2018 (July 18, 2018): 1–15. http://dx.doi.org/10.1155/2018/5364628.

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The TBM tunneling at the Jinping II hydropower station in Southwest China has received extensive concerns around the world because of its large engineering scale and the high rockburst risks faced in the tunnel advancement. The associated energy changes of rockbursts and control method for safe TBM tunneling are to be further investigated. A movable microseismic (MS) monitoring system was established to capture the MS events and rockbursts when the TBM excavated the headrace tunnel #1 at the Jinping II hydropower station. The spatial and temporal patterns of the energy changes in the tunnel rock masses were studied. Meanwhile, the evolution of a rockburst encountered in front of the TBM excavation face was revealed, and the performance of the top pilot tunnel method on the reduction of the rockburst risks in the headrace tunnel #1 was evaluated based on the energy changes of the surrounding rock masses. It can be concluded that energy accumulation and energy release firstly occurred in the surrounding rock masses at the southern end of the top pilot tunnel section of the headrace tunnel #1. Then, energy transference of the rock masses took place from the southern end to northwest of the top pilot tunnel giving rise to the occurrence of a moderate rockburst about 30 m in front of the tunnel. However, no rockbursts appeared when the TBM excavated through the top pilot tunnel section of the headrace tunnel #1. Therefore, the top pilot tunnel method really works in reducing the risks of rockbursts during the TBM tunneling in deep tunnels.

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44

ter Veldhuis, W. T. A. "Two-loop renormalization-group-improved top-quark and Higgs-boson masses in the top-quark condensate model." Physical Review D 45, no. 9 (May 1, 1992): 3201–5. http://dx.doi.org/10.1103/physrevd.45.3201.

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45

LEMKE, E. H. "DERIVATION OF A NOVEL RELATION BETWEEN THE MASSES OF THE TOP-QUARK AND AN ELECTROWEAK SCALAR." International Journal of Modern Physics A 15, no. 11 (April 30, 2000): 1597–612. http://dx.doi.org/10.1142/s0217751x00000719.

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We start with generating the masses of the charged leptons by gap equations. Then we present analogous radiative masses of the electroweak vector-bosons. We derive them from the global SU (2)L× U (1) symmetry without making recourse to any scalar fields or spontaneous breaking of gauge symmetry. Nevertheless, we find the mixing angle relation [Formula: see text]. Moreover, we find that the radiatively generated masses of Z and W require the existence of a cutoff energy of the order of 1014 GeV, which is just the grand-unification energy scale. We then eliminate the cutoff by renormalizing the two coupling constants and arrive at a function between mW and m top if mZ, [Formula: see text] and sin 2θ eff are given. Comparison with the electroweak precision data shows that the predicted value of mW does reproduce the experimental data though the vacuum loops of the leptons, of the light quarks as well as of possible scalar particles have been ignored. Then, we introduce a doublet of scalar bosons to investigate its effect on the mW prediction. We fix its couplings to the photon, to W as well as Z by localizing SU (2)L× U (1). The radiative mZ and mW results interdict a spontaneous breaking of the gauge symmetry. So there are an elementary charged and neutral scalar field. Their masses are identical. We show that there is no radiative effect of these scalars on the masses of W and Z. However, the scalar fields affect the coupling constants and, by this, the relationship between mW and m top alters. We calculate the modifications and find a relatively small effect. It seems to be comparable in magnitude with the QCD-corrections of the loops of vacuum polarization. Substituting the experimental mW value, we get a relation between m top and m scalar . The mass of the top-quark is increasing with increasing m scalar . In the standard model, m top also increases with increasing m Higgs . The effect of the elementary scalar is however much weaker.

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46

Han, Tao, German Valencia, and Yili Wang. "New Signatures For Top In Hadron Collider." International Journal of Modern Physics A 20, no. 14 (June 10, 2005): 3214–17. http://dx.doi.org/10.1142/s0217751x05026182.

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We study the signatures for new TeV resonances that couple to top or bottom quarks both at the Tevatron Run II and at the LHC. We find that it is possible to study these resonances when they are produced in association with a pair of heavy quarks or in association with a single top at the LHC. In particular, with an integrated luminosity of 300 fb-1 at the LHC, it is possible to probe resonance masses up to around 2 TeV.

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47

Londoño, Diana. "Accuracy and Implications of Percutaneous Renal Biopsy in the Management of Renal Masses." Permanente Journal 17, no. 3 (August 1, 2013): 4–7. http://dx.doi.org/10.7812/tpp/12-110.

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Hau, N. H., A. C. Ravel, A. Duclos, F. Giammarile, and P. J. Souquet. "TEP-TDM-FDG et diagnostic de malignité des nodules et masses pulmonaires." Revue des Maladies Respiratoires 25, no. 1 (January 2008): 33–41. http://dx.doi.org/10.1016/s0761-8425(08)70464-9.

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Ananthanarayan, B., Q. Shafi, and X. M. Wang. "Improved predictions for top quark, lightest supersymmetric particle, and Higgs scalar masses." Physical Review D 50, no. 9 (November 1, 1994): 5980–84. http://dx.doi.org/10.1103/physrevd.50.5980.

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Barger, V., J. Hewett, and T. Rizzo. "Top-quark mass predictions from W,Z masses and Z partial widths." Physical Review Letters 65, no. 11 (September 1990): 1313–16. http://dx.doi.org/10.1103/physrevlett.65.1313.

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Journal articles on the topic 'Massey Twp'

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