By Günter Figal

Connecting aesthetic event with our event of nature or with different cultural artifacts, Aesthetics as Phenomenology makes a speciality of what paintings capacity for cognition, popularity, and affect—how artwork alterations our daily disposition or habit. Günter Figal engages in a penetrating research of the instant at which, in our contemplation of a piece of artwork, response and concept confront one another. For these educated within the visible arts and for extra informal audience, Figal unmasks artwork as a decentering event that opens additional probabilities for realizing our lives and our international.

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Connecting aesthetic event with our event of nature or with different cultural artifacts, Aesthetics as Phenomenology makes a speciality of what paintings skill for cognition, acceptance, and affect—how artwork alterations our daily disposition or habit. Günter Figal engages in a penetrating research of the instant at which, in our contemplation of a piece of artwork, response and idea confront one another.

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Phys. Commun. 180, 431–454 (2009) 28. A. Belyaev, P. Hamers, and M. Thomas, Triple Higgs production at a 100 TeV collider as a measurement of anomolous Higgs couplings to weak bosons, Upcoming 29. -J. , LHC signatures of new Gauge bosons in minimal Higgsless model. Phys. Rev. 1 Motivation The discovery of the Higgs boson at the LHC [1, 2] has ushered in a new era in the study of the electroweak symmetry breaking (EWSB) sector. Since the longitudinal polarisations of the electroweak gauge bosons (VL ’s, V = W ± , Z) have their origin in EWSB, determining their interactions is of fundamental importance to unravel the mechanism of EWSB.

3 Cross section for triple Higgs production pp → jjhhh with VBF cuts as a function of the anomalous coupling a for LHC14 (dark lines) and LHC33 (light lines). Solid lines are for other parameters fixed to SM values and dashed lines are for parameters given by MCHM4 relations (Eq. 5 for pp → jjW + W − , leading to an small increase in cross section for anomalous coupling instead of a reduction in the more inclusive case. For pp → jjW + W − h this does not occur, presumably as the overall increase in the longitudinal scattering was too small.

The different channels are: (π 0 π 0 , π + π − ) → π + π − π + π − (dashed line), (π 0 π 0 , π + π − ) → π + π − h (thick solid line), (π 0 π 0 , π + π − ) → hhh (dotted line), and (π 0 π 0 , π + π − ) → π + π − (thin solid line) for comparison. The notation (π 0 π 0 , π + π − ) indicates that both π 0 π 0 and π + π − initial states were taken into account model effects in the √ MCHM4 by altering the other parameters according to Eq. 13 along with d3 = 1 − ξ [17]. 9. The largest increases are observed for triple Higgs production.

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