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Journal articles on the topic 'Non universal gaugino masses'

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Author: Grafiati

Published: 14 March 2023

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1

Chamoun, Nidal, Chao-Shang Huang, Chun Liu, and Xiao-Hong Wu. "Non-universal gaugino masses in supersymmetric SO(10)." Nuclear Physics B 624, no. 1-2 (March 2002): 81–94. http://dx.doi.org/10.1016/s0550-3213(01)00652-6.

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2

Birkedal-Hansen, Andreas. "SUSY dark matter with non-universal gaugino masses." Nuclear Physics B - Proceedings Supplements 124 (July 2003): 155–58. http://dx.doi.org/10.1016/s0920-5632(03)02096-6.

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3

Horton, D., and G. G. Ross. "Naturalness and focus points with non-universal gaugino masses." Nuclear Physics B 830, no. 1-2 (May 2010): 221–47. http://dx.doi.org/10.1016/j.nuclphysb.2009.12.031.

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4

Profumo, Stefano, and Carlos E. Yaguna. "Non-universal gaugino masses and the fate of μ→eγ." Nuclear Physics B 681, no. 1-2 (March 2004): 247–60. http://dx.doi.org/10.1016/j.nuclphysb.2003.11.027.

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5

Chamoun, Nidal, Chao-Shang Huang, Chun Liu, and Xiao-Hong Wu. "Intermediate scale dependence of non-universal gaugino masses in supersymmetricSO(10)." Journal of Physics G: Nuclear and Particle Physics 37, no. 10 (September 7, 2010): 105016. http://dx.doi.org/10.1088/0954-3899/37/10/105016.

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6

King, Stephen F., Jonathan P. Roberts, and Durga Prasad Roy. "Natural dark matter in SUSY GUTs with non-universal gaugino masses." Journal of High Energy Physics 2007, no. 10 (November 1, 2007): 106. http://dx.doi.org/10.1088/1126-6708/2007/10/106.

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7

Chakrabarti, Subhendu, Amitava Datta, and N. K. Mondal. "Contributed report: Probing non-universal gaugino masses — Prospects at the Tevatron." Pramana 63, no. 6 (December 2004): 1355–57. http://dx.doi.org/10.1007/bf02704900.

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8

Chamoun, Nidal. "Group theory and unification of forces: Application to ‘non-universal’ gaugino masses." Journal of the Egyptian Mathematical Society 19, no. 1-2 (April 2011): 33–38. http://dx.doi.org/10.1016/j.joems.2011.09.012.

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9

Cerdeno, D. G., and C. Munoz. "Neutralino dark matter in supergravity theories with non-universal scalar and gaugino masses." Journal of High Energy Physics 2004, no. 10 (October 7, 2004): 015. http://dx.doi.org/10.1088/1126-6708/2004/10/015.

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10

Bhattacharya, Subhaditya, AseshKrishna Datta, and Biswarup Mukhopadhyaya. "Non-universal gaugino masses: a signal-based analysis for the Large Hadron Collider." Journal of High Energy Physics 2007, no. 10 (October 24, 2007): 080. http://dx.doi.org/10.1088/1126-6708/2007/10/080.

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11

Huitu, K., J. Laamanen, P. N. Pandita, and Sourov Roy. "Phenomenology of non-universal gaugino masses and implications for the Higgs boson decay." Pramana 69, no. 5 (November 2007): 823–27. http://dx.doi.org/10.1007/s12043-007-0189-z.

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12

GOGOLADZE, ILIA, RIZWAN KHALID, SHABBAR RAZA, and QAISAR SHAFI. "NEUTRALINO DARK MATTER IN FLIPPED SU(5)." Modern Physics Letters A 25, no. 40 (December 28, 2010): 3371–79. http://dx.doi.org/10.1142/s0217732310034602.

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We investigate neutralino dark matter in supersymmetric flipped SU(5), focusing on candidates with masses of order 30–150 GeV and spin-independent cross-sections that are consistent with the most recent CDMS II results. We assume gravity mediated supersymmetry breaking and restrict the magnitude of the soft supersymmetry breaking mass parameters to 1 TeV or less. With non-universal soft gaugino and Higgs masses, and taking flipped SU(5) into account, we identify allowed regions of the parameter space and highlight some benchmark solutions including Higgs and sparticle spectroscopy.

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13

Bélanger, G., F. Boudjema, A. Cottrant, A. Pukhov, and A. Semenov. "WMAP constraints on SUGRA models with non-universal gaugino masses and prospects for direct detection." Nuclear Physics B 706, no. 1-2 (January 2005): 411–54. http://dx.doi.org/10.1016/j.nuclphysb.2004.11.036.

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14

Huitu, Katri, Ritva Kinnunen, Jari Laamanen, Sami Lehti, Sourov Roy, and Tapio Salminen. "Search for Higgs bosons in SUSY cascades in CMS and dark matter with non-universal gaugino masses." European Physical Journal C 58, no. 4 (November 7, 2008): 591–608. http://dx.doi.org/10.1140/epjc/s10052-008-0786-0.

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15

Bandyopadhyay, Priyotosh. "Probing non-universal gaugino masses via Higgs boson production under SUSY cascades at the LHC: a detailed study." Journal of High Energy Physics 2009, no. 07 (July 30, 2009): 102. http://dx.doi.org/10.1088/1126-6708/2009/07/102.

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16

Spies, A., and G. Anton. "Confronting recent results from selected direct and indirect dark matter searches and the Higgs boson with supersymmetric models with non-universal gaugino masses." Journal of Cosmology and Astroparticle Physics 2013, no. 06 (June 18, 2013): 022. http://dx.doi.org/10.1088/1475-7516/2013/06/022.

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17

ZHENG, SIBO, and JIA-HUI HUANG. "FROM SUPERCURRENTS TO SOFT TERMS." Modern Physics Letters A 26, no. 31 (October 10, 2011): 2345–56. http://dx.doi.org/10.1142/s0217732311036632.

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In this paper conformal hidden sectors of Ferrara–Zumino multiplets are investigated in framework of gravity mediation. The two-point correlator of Ferrara–Zumino multiplets can be parametrized, which implies the wave function renormalizations of components fields in gravity supermultiplet can be evaluated in relatively simple form. Soft terms are calculated via supercurrent approach. We find gaugino masses are independent of sfermion masses on general grounds. The unification of gaugino masses is not universal. In comparison with general gauge mediation, there are no sum rules for sfermion masses of each generation.

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18

Dermíšek, Radovan, and Navin McGinnis. "Little hierarchy in the minimally specified MSSM." International Journal of Modern Physics A 33, no. 25 (September 10, 2018): 1850145. http://dx.doi.org/10.1142/s0217751x18501452.

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We study constrained versions of the minimal supersymmetric model and investigate the hierarchy between the electroweak scale and the scale of superpartners that can be achieved without relying on specifying model parameters by more than one digit (or with better than 10% precision). This approach automatically avoids scenarios in which a large hierarchy is obtained by special choices of parameters and yet keeps scenarios that would otherwise be disfavored by various sensitivity measures. We consider models with universal gaugino and scalar masses, models with nonuniversal Higgs masses or nonuniversal gaugino masses and focus on scenarios in which all the model parameters are either of the same order or zero at the grand unification scale. We find that the maximal hierarchy between the electroweak scale and stop masses, requiring that model parameters are not specified beyond one digit, ranges from a factor of [Formula: see text][Formula: see text]10–30 for the CMSSM up to [Formula: see text][Formula: see text]300 for models with nonuniversal Higgs or gaugino masses.

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19

Baer, Howard, Csaba Balázs, Alexander Belyaev, Radovan Dermísek, Arash Mafi, and Azar Mustafayev. "Viable models with non-universal gaugino mediated supersymmetry breaking." Journal of High Energy Physics 2002, no. 05 (May 31, 2002): 061. http://dx.doi.org/10.1088/1126-6708/2002/05/061.

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20

Fornengo, Nicolao. "Light neutralino dark matter in gaugino non-universal models." Journal of Physics: Conference Series 39 (May 1, 2006): 163–65. http://dx.doi.org/10.1088/1742-6596/39/1/039.

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21

Khalil, Shaaban. "Non-universal gaugino phases and the LSP relic density." Physics Letters B 484, no. 1-2 (June 2000): 98–102. http://dx.doi.org/10.1016/s0370-2693(00)00598-0.

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22

Arkani-Hamed, Nima, Hsin-Chia Cheng, and Takeo Moroi. "Non-unified gaugino masses in supersymmetric missing partner models with hypercolor." Physics Letters B 387, no. 3 (October 1996): 529–34. http://dx.doi.org/10.1016/0370-2693(96)01089-1.

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23

Bélanger, G., F. Boudjema, A. Pukhov, and R. K. Singh. "Constraining the MSSM with universal gaugino masses and implication for searches at the LHC." Journal of High Energy Physics 2009, no. 11 (November 6, 2009): 026. http://dx.doi.org/10.1088/1126-6708/2009/11/026.

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24

Suematsu, D. "Phenomenological features in a model with non-universal gaugino CP phases." European Physical Journal C 52, no. 1 (July 25, 2007): 211–21. http://dx.doi.org/10.1140/epjc/s10052-007-0362-z.

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25

Balázs, Csaba, and Radovan Dermísek. "Yukawa coupling unification and non-universal gaugino mediation of supersymmetry breaking." Journal of High Energy Physics 2003, no. 06 (June 13, 2003): 024. http://dx.doi.org/10.1088/1126-6708/2003/06/024.

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26

PÉREZ MERCADER, J. "1-LOOP EFFECTS IN 4-d SUPERGRAVITY GENERATED BY HETEROTIC STRINGS ON ASYMMETRIC ORBIFOLDS." Modern Physics Letters A 04, no. 01 (January 1989): 83–90. http://dx.doi.org/10.1142/s0217732389000113.

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We consider the class of N = 1, d = 4 supergravity theories generated in the compactification of heterotic superstrings on asymmetric orbifolds. We study the dominant quadratic contribution to the 1-loop effective potential and find it to be negative. We also examine the mass term for the chiral fields and find that they are massless at the compactification scale. We show that it is possible to have models where, at the compactification scale, the cosmological constant, the gaugino masses and the masses for the chiral non-gauge singlet fields are all zero.

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27

Baer, H. "Study of viable models with non-universal gaugino mediation with CompHEP and ISAJET." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 502, no. 2-3 (April 21, 2003): 560–63. http://dx.doi.org/10.1016/s0168-9002(03)00502-3.

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28

Lleyda, A., and C. Muñoz. "Non-universal soft scalar masses in supersymmetric theories." Physics Letters B 317, no. 1-2 (November 1993): 82–91. http://dx.doi.org/10.1016/0370-2693(93)91574-7.

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29

Kobayashi, Tatsuo, Daijiro Suematsu, Kiyonori Yamada, and Yoshio Yamagishi. "Non-universal soft scalar masses in superstring theories." Physics Letters B 348, no. 3-4 (April 1995): 402–10. http://dx.doi.org/10.1016/0370-2693(95)00194-p.

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30

Autermann, Christian. "Search for R-Parity violating SUSY with the DØ Experiment." International Journal of Modern Physics A 20, no. 15 (June 20, 2005): 3322–24. http://dx.doi.org/10.1142/s0217751x05026455.

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We have searched for R-parity violating supersymmetry in final states with electrons and muons, assuming a single non-zero LLĒ or [Formula: see text] coupling, in particular λ121, λ122 or λ′211. In the absence of an excess in the data, upper cross-section limits are set as a function of gaugino and slepton masses. The searches are performed on data collected with the DØ detector in Run II, at a center of mass energy of 1.96 TeV and an integrated luminosity of up to 240 pb-1. All limits are improving significantly compared to the DØ Run I results.

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31

Ellis, John, Toby Falk, Keith A. Olive, and Yudi Santoso. "Exploration of the MSSM with non-universal Higgs masses." Nuclear Physics B 652 (March 2003): 259–347. http://dx.doi.org/10.1016/s0550-3213(02)01144-6.

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32

Ellis, John, Keith A. Olive, and Yudi Santoso. "The MSSM parameter space with non-universal Higgs masses." Physics Letters B 539, no. 1-2 (July 2002): 107–18. http://dx.doi.org/10.1016/s0370-2693(02)02071-3.

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33

Cannoni, M., J. Ellis, M. E. Gómez, S. Lola, and R. Ruiz de Austri. "Supersymmetry searches in GUT models with non-universal scalar masses." Journal of Cosmology and Astroparticle Physics 2016, no. 03 (March 22, 2016): 041. http://dx.doi.org/10.1088/1475-7516/2016/03/041.

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34

Kim, Sung-Gi, Nobuhiro Maekawa, Keiko I. Nagao, Mihoko M. Nojiri, and Kazuki Sakurai. "LHC signature of supersymmetric models with non-universal sfermion masses." Journal of High Energy Physics 2009, no. 10 (October 2, 2009): 005. http://dx.doi.org/10.1088/1126-6708/2009/10/005.

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35

Flacke, Thomas, Kyoungchul Kong, and Seong Chan Park. "A review on non-minimal universal extra dimensions." Modern Physics Letters A 30, no. 05 (February 3, 2015): 1530003. http://dx.doi.org/10.1142/s0217732315300037.

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We report on the current status of non-minimal universal extra dimension (NMUED) models. Our emphasis is on the possible extension of the minimal UED (MUED) model by allowing bulk masses and boundary localized terms. We take into account the data from the Large Hadron Collider (LHC) as well as direct and indirect searches of dark matter (DM) and electroweak (EW) precision measurements.

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36

Datta, Amitava, Aseshkrishna Datta, and M. K. Parida,. "Signatures of non-universal soft breaking sfermion masses at hadron colliders." Physics Letters B 431, no. 3-4 (July 1998): 347–53. http://dx.doi.org/10.1016/s0370-2693(98)00507-3.

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37

Allanach, Ben C., Christopher Gorham Lester, M. Andy Parker, and Bryan R. Webber. "Measuring sparticle masses in non-universal string inspired models at the LHC." Journal of High Energy Physics 2000, no. 09 (September 5, 2000): 004. http://dx.doi.org/10.1088/1126-6708/2000/09/004.

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38

Lester, Christopher G., Michael Andy Parker, and Martin J. White. "Three body kinematic endpoints in SUSY models with non-universal Higgs masses." Journal of High Energy Physics 2007, no. 10 (October 12, 2007): 051. http://dx.doi.org/10.1088/1126-6708/2007/10/051.

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39

Kraml, Sabine, and Dao Thi Nhung. "Three-body decays of sleptons in models with non-universal Higgs masses." Journal of High Energy Physics 2008, no. 02 (February 18, 2008): 061. http://dx.doi.org/10.1088/1126-6708/2008/02/061.

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40

Sen, Parongama, and Amnon Aharony. "Universal Mass Ratios of Non-Unique Spanning Clusters in Percolation." International Journal of Modern Physics C 08, no. 05 (October 1997): 1169–73. http://dx.doi.org/10.1142/s012918319700103x.

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We find that when two or more spanning clusters exist at the percolation threshold, the mass of each scales with the same fractal dimension D=1.89 in two dimensions and D=2.53 in three dimensions. We also determine the ratios of the masses of the spanning clusters. In two dimensions, this is done for different lattices of different shapes. In the case of two spanning clusters, the ratio of the larger spanning cluster to the smaller lies around 1.4 for two dimensions, almost independent of lattice structure and shape.

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41

ANANTHANARAYAN, B., and P. N. PANDITA. "SQUARK AND SLEPTON MASSES AS PROBES OF SUPERSYMMETRIC SO(10) UNIFICATION." Modern Physics Letters A 19, no. 06 (February 28, 2004): 467–79. http://dx.doi.org/10.1142/s0217732304013210.

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We carry out an analysis of the non-universal supersymmetry breaking scalar masses arising in SO(10) supersymmetric unification. By considering patterns of squark and slepton masses, we derive a set of sum rules for the sfermion masses which are independent of the manner in which SO(10) breaks to the Standard Model gauge group via its SU(5) subgroups. The phenomenology arising from such non-universality is unaffected by the symmetry breaking pattern, so long as the breaking occurs via any of the SU(5) subgroups of the SO(10) group.

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42

Causse, M. B., and J. Orloff. "Supersymmetric penguin contributions to the decay b → sγ with non-universal squarks masses." European Physical Journal C 23, no. 4 (April 2002): 749–55. http://dx.doi.org/10.1007/s100520100882.

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43

Jin, Changhyun. "Reinterpretation of Thermodynamics Consisting of Mass-Based Energy and Non-Mass-Based Energy." Science of Advanced Materials 14, no. 11 (November 1, 2022): 1750–55. http://dx.doi.org/10.1166/sam.2022.4378.

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Energy can be broadly classified into mass-based and non-mass-based. Therefore, thermodynamics is too broad and universal to interpret the complex phenomena within only matter. Here, we suggest that (1) the current mixed concept of energy and work can actually be expressed as the actions of non-masses and the actions of masses, respectively, and (2) the definition of total energy must be revised based on the product of temperature and entropy. These findings, i.e., that space contains energy and the current concept of temperature actually corresponds to space density, are validated by a reinterpretation of thermodynamics.

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44

Chen, Mu-Chun, and Jinrui Huang. "Lifting slepton masses with a non-universal, non-anomalous U(1)NAF′ in Anomaly Mediated SUSY Breaking." Physics Letters B 706, no. 1 (November 2011): 53–62. http://dx.doi.org/10.1016/j.physletb.2011.10.065.

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45

Briceño, César, Kevin L. Luhman, Lee Hartmann, John R. Stauffer, and J. Davy Kirkpatrick. "The Brown Dwarf Deficit in Taurus: Evidence for a Non-Universal IMF." Symposium - International Astronomical Union 211 (2003): 81–82. http://dx.doi.org/10.1017/s0074180900210322.

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We present the results of a deep, optical/IR wide field imaging survey of selected fields in the nearby (d~ 140 pc) Taurus star-forming region. We report the discovery of 9 new members with spectral types M5.75–M9.5. We derive an Initial Mass Function encompassing 54% of the known members in Taurus. Comparison with dense regions like the Trapezium Cluster in Orion shows that Taurus has produced x2 less brown dwarfs. We suggest that the lower frequency of brown dwarfs in Taurus may result from the low-density star-forming environment, leading to larger minimum Jeans masses.

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46

Ellis, John, S. F. King, and J. P. Roberts. "The fine-tuning price of neutralino dark matter in models with non-universal Higgs masses." Journal of High Energy Physics 2008, no. 04 (April 29, 2008): 099. http://dx.doi.org/10.1088/1126-6708/2008/04/099.

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47

Sheykin, Anton, and Sergey Manida. "Universal Constants and Natural Systems of Units in a Spacetime of Arbitrary Dimension." Universe 6, no. 10 (October 1, 2020): 166. http://dx.doi.org/10.3390/universe6100166.

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We study the properties of fundamental physical constants using the threefold classification of dimensional constants proposed by J.-M. Lévy-Leblond: constants of objects (masses, etc.), constants of phenomena (coupling constants), and “universal constants” (such as c and ℏ). We show that all of the known “natural” systems of units contain at least one non-universal constant. We discuss the possible consequences of such non-universality, e.g., the dependence of some of these systems on the number of spatial dimensions. In the search for a “fully universal” system of units, we propose a set of constants that consists of c, ℏ, and a length parameter and discuss its origins and the connection to the possible kinematic groups discovered by Lévy-Leblond and Bacry. Finally, we give some comments about the interpretation of these constants.

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48

Ellis, John, Keith A. Olive, Yudi Santoso, and Vassilis C. Spanos. "OnBs→μ+μ−and cold dark matter scattering in the MSSM with non-universal Higgs masses." Journal of High Energy Physics 2006, no. 05 (May 25, 2006): 063. http://dx.doi.org/10.1088/1126-6708/2006/05/063.

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49

Ellis, John, Keith A. Olive, and Pearl Sandick. "Update on the direct detection of dark matter in MSSM models with non-universal Higgs masses." New Journal of Physics 11, no. 10 (October 16, 2009): 105015. http://dx.doi.org/10.1088/1367-2630/11/10/105015.

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50

Eckert, D., V. Ghirardini, S. Ettori, E. Rasia, V. Biffi, E. Pointecouteau, M. Rossetti, et al. "Non-thermal pressure support in X-COP galaxy clusters." Astronomy & Astrophysics 621 (January 2019): A40. http://dx.doi.org/10.1051/0004-6361/201833324.

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Galaxy clusters are the endpoints of structure formation and are continuously growing through the merging and accretion of smaller structures. Numerical simulations predict that a fraction of their energy content is not yet thermalized, mainly in the form of kinetic motions (turbulence, bulk motions). Measuring the level of non-thermal pressure support is necessary to understand the processes leading to the virialization of the gas within the potential well of the main halo and to calibrate the biases in hydrostatic mass estimates. We present high-quality measurements of hydrostatic masses and intracluster gas fraction out to the virial radius for a sample of 13 nearby clusters with available XMM-Newton and Planck data. We compare our hydrostatic gas fractions with the expected universal gas fraction to constrain the level of non-thermal pressure support. We find that hydrostatic masses require little correction and infer a median non-thermal pressure fraction of ∼6% and ∼10% at R500 and R200, respectively. Our values are lower than the expectations of hydrodynamical simulations, possibly implying a faster thermalization of the gas. If instead we use the mass calibration adopted by the Planck team, we find that the gas fraction of massive local systems implies a mass bias 1 − b = 0.85 ± 0.05 for Sunyaev–Zeldovich-derived masses, with some evidence for a mass-dependent bias. Conversely, the high bias required to match Planck cosmic microwave background and cluster count cosmology is excluded by the data at high significance, unless the most massive halos are missing a substantial fraction of their baryons.

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