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Related papers: Landscapes at Colliders

200 papers

We consider a scalar field with a bottom-less potential, such as $g^3 \phi$, finding that cosmologies unavoidably end up with a crunch, late enough to be compatible with observations if $g \lesssim 1.2 H_0^{2/3} M_{\rm Pl}^{1/3}$. If…

General Relativity and Quantum Cosmology · Physics 2019-09-09 Alessandro Strumia , Daniele Teresi

In the eternally inflationary background driven by the metastable vacua of the landscape, it is possible that some local quantum fluctuations with the null energy condition violation can be large enough to stride over the barriers among…

General Relativity and Quantum Cosmology · Physics 2008-11-26 Yun-Song Piao

We rediscuss the main Cosmological Problems as illusions originated from our ignorance of the hidden information holographically stored in {\it vacuo}. The Cosmological vacuum state is full of a large number of dynamical quantum hairs,…

General Relativity and Quantum Cosmology · Physics 2020-05-26 Andrea Addazi

The currently accepted mathematical description of the fundamental constituents and interactions of matter is the Standard Model of particle physics. Its last missing particle, the famous Higgs boson, was observed at the Large Hadron…

High Energy Physics - Phenomenology · Physics 2024-03-22 Andreas Crivellin , Bruce Mellado

Despite the many outstanding cosmological observations leading to a strong evidence for a nonvanishing cosmological constant (CC) term in the gravitational field equations, the theoretical status of this quantity seems to be lagging well…

High Energy Physics - Theory · Physics 2010-02-11 Ilya L. Shapiro , Joan Sola

Constants of Nature that have nongeneric values pose a riddle often referred to as the finetuning problem. The conspicuous values assumed by many physical constants (e.g., the vanishing effective cosmological constant, the smallness of the…

High Energy Physics - Phenomenology · Physics 2008-02-03 D. L. Bennett , C. D. Froggatt , H. B. Nielsen

Even if nothing but a light Higgs is observed at the LHC, suggesting that the Standard Model is unmodified up to scales far above the weak scale, Higgs physics can yield surprises of fundamental significance for cosmology. As has long been…

High Energy Physics - Phenomenology · Physics 2009-05-22 Nima Arkani-Hamed , Sergei Dubovsky , Leonardo Senatore , Giovanni Villadoro

Quantum scale invariance in the UV has been recently advocated as an attractive way of solving the gauge hierarchy problem arising in the Standard Model. We explore the cosmological signatures at the electroweak scale when the breaking of…

High Energy Physics - Phenomenology · Physics 2014-09-24 Glauber C. Dorsch , Stephan J. Huber , Jose Miguel No

We point out that $\Lambda$CDM cosmology has an ignored assumption. That is, the $\Lambda$ component of the universe moves synchronously with ordinary matters on Hubble scales. If cosmological constant is vacuum energy, this assumption may…

General Relativity and Quantum Cosmology · Physics 2007-05-23 Ding-fang Zeng , Yi-hong Gao

Within present constraints on the observed smooth energy and its equation of state parameter, it is important to find out whether the smooth energy is static (cosmological constant) or dynamic (quintessence). The most dynamical quintessence…

Astrophysics · Physics 2009-04-13 S. A. Bludman , M. Roos

Although the Higgs potential in the Standard Model (SM) contains only a simple electroweak symmetry breaking vacuum in the small field region, additional metastable or global vacua could exist in models beyond the SM. In this paper, we…

High Energy Physics - Phenomenology · Physics 2021-10-01 Yang Bai , Seung J. Lee , Minho Son , Fang Ye

In models with a non-minimal Higgs sector, the lightest scalar state may be a neutral CP-even Higgs boson, whose properties are nearly identical to those of the minimal Higgs boson of the Standard Model. In such a scenario, the other Higgs…

High Energy Physics - Phenomenology · Physics 2007-05-23 Howard E. Haber

We consider the impact of colored scalars that can couple directly to matter fields on the recently measured h to gamma gamma excess. Among all possible candidates only scalar states transforming as (8, 2,1/2) and (6,3,1/3) under the…

High Energy Physics - Phenomenology · Physics 2012-12-11 Ilja Dorsner , Svjetlana Fajfer , Admir Greljo , Jernej F. Kamenik

In the landscape, if there is to be any prospect of scientific prediction, it is crucial that there be states which are distinguished in some way. The obvious candidates are states which exhibit symmetries. Here we focus on states which…

High Energy Physics - Theory · Physics 2009-12-08 M. Dine , G. Festuccia , A. Morisse

The long awaited discovery of a new light scalar at the LHC opens up a new era of studies of the Higgs sector in the SM and its extensions. In this paper we discuss the consequences of the observation of a light Higgs boson with the mass…

High Energy Physics - Phenomenology · Physics 2012-10-02 Alexandre Arbey , Marco Battaglia , Abdelhak Djouadi , Farvah Mahmoudi

Is the weak scale natural? This ever pending question makes the search for new particle production a highly motivated primary goal of the next LHC phase. These searches may or may not be successful. While waiting for a needed higher energy…

High Energy Physics - Phenomenology · Physics 2014-03-25 Riccardo Barbieri , Andrea Tesi

The small and negative value of the Standard Model Higgs quartic coupling at high scales can be understood in terms of anthropic selection on a landscape where large and negative values are favored: most universes have a very short-lived…

High Energy Physics - Phenomenology · Physics 2015-06-26 Francesco D'Eramo , Lawrence J. Hall , Duccio Pappadopulo

There are many possibilities for new physics beyond the Standard Model that feature non-standard Higgs sectors. These may introduce new sources of CP violation, and there may be mixing between multiple Higgs bosons or other new scalar…

High Energy Physics - Phenomenology · Physics 2022-10-26 S. Kraml , E. Accomando , A. G. Akeroyd , E. Akhmetzyanova , J. Albert , A. Alves , N. Amapane , M. Aoki , G. Azuelos , S. Baffioni , A. Ballestrero , V. Barger , A. Bartl , P. Bechtle , G. Belanger , A. Belhouari , R. Bellan , A. Belyaev , P. Benes , K. Benslama , W. Bernreuther , M. Besancon , G. Bevilacqua , M. Beyer , M. Bluj , S. Bolognesi , M. Boonekamp , F. Borzumati , F. Boudjema , A. Brandenburg , T. Brauner , C. P. Buszello , J. M. Butterworth , M. Carena , D. Cavalli , G. Cerminara , S. Y. Choi , B. Clerbaux , C. Collard , J. A. Conley , A. Deandrea , S. De Curtis , R. Dermisek , A. De Roeck , G. Dewhirst , M. A. Diaz , J. L. Diaz-Cruz , D. D. Dietrich , M. Dolgopolov , D. Dominici , M. Dubinin , O. Eboli , J. Ellis , N. Evans , L. Fano , J. Ferland , S. Ferrag , S. P. Fitzgerald , H. Fraas , F. Franke , S. Gennai , I. F. Ginzburg , R. M. Godbole , T. Gregoire , G. Grenier , C. Grojean , S. B. Gudnason , J. F. Gunion , H. E. Haber , T. Hahn , T. Han , V. Hankele , C. Hays , S. Heinemeyer , S. Hesselbach , J. L. Hewett , K. Hidaka , M. Hirsch , W. Hollik , D. Hooper , J. Hosek , J. Hubisz , C. Hugonie , J. Kalinowski , S. Kanemura , V. Kashkan , T. Kernreiter , W. Khater , V. A. Khoze , W. Kilian , S. F. King , O. Kittel , G. Klamke , J. L. Kneur , C. Kouvaris , M. Krawczyk , P. Krstonosic , A. Kyriakis , P. Langacker , M. P. Le , H. -S. Lee , J. S. Lee , M. C. Lemaire , Y. Liao , B. Lillie , V. Litvin , H. E. Logan , B. McElrath , T. Mahmoud , E. Maina , C. Mariotti , P. Marquard , A. D. Martin , K. Mazumdar , D. J. Miller , P. Mine , K. Moenig , G. Moortgat-Pick , S. Moretti , M. M. Muhlleitner , S. Munir , R. Nevzorov , H. Newman , P. Niezurawski , A. Nikitenko , R. Noriega-Papaqui , Y. Okada , P. Osland , A. Pilaftsis , W. Porod , H. Przysiezniak , A. Pukhov , D. Rainwater , A. Raspereza , J. Reuter , S. Riemann , S. Rindani , T. G. Rizzo , E. Ros , A. Rosado , D. Rousseau , D. P. Roy , M. G. Ryskin , H. Rzehak , F. Sannino , E. Schmidt , H. Schroder , M. Schumacher , A. Semenov , E. Senaha , G. Shaughnessy , R. K. Singh , J. Terning , L. Vacavant , M. Velasco , A. Villanova del Moral , F. von der Pahlen , G. Weiglein , J. Williams , K. Williams , A. F. Zarnecki , D. Zeppenfeld , D. Zerwas , P. M. Zerwas , A. R. Zerwekh , J. Ziethe

The possibility that the Fermi scale is the only fundamental energy scale of Nature is under serious consideration at present, yet cosmic rays may already have provided direct evidence of new physics at a much higher scale. The recent…

High Energy Physics - Phenomenology · Physics 2016-11-03 Subir Sarkar

The Bousso-Polchinski (BP) Landscape is a proposal for solving the Cosmological Constant Problem. The solution requires counting the states in a very thin shell in flux space. We find an exact formula for this counting problem which has two…

High Energy Physics - Theory · Physics 2015-05-20 Cesar Asensio , Antonio Segui
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