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Multiscalar production amplitudes beyond threshold

We present exact tree-order amplitudes for $H^* \to n~H$, for final states containing one or two particles with non-zero three-momentum, for various interaction potentials. We show that there are potentials leading to tree amplitudes that satisfy unitarity, not only at threshold but also in the abov...

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Autores principales: Argyres, E.N., Papadopoulos, Costas G., Kleiss, Ronald H.P.
Lenguaje:eng
Publicado: 1992
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0550-3213(93)90205-4
http://cds.cern.ch/record/559491
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author Argyres, E.N.
Papadopoulos, Costas G.
Kleiss, Ronald H.P.
author_facet Argyres, E.N.
Papadopoulos, Costas G.
Kleiss, Ronald H.P.
author_sort Argyres, E.N.
collection CERN
description We present exact tree-order amplitudes for $H^* \to n~H$, for final states containing one or two particles with non-zero three-momentum, for various interaction potentials. We show that there are potentials leading to tree amplitudes that satisfy unitarity, not only at threshold but also in the above kinematical configurations and probably beyond. As a by-product, we also calculate $2\to n$ tree amplitudes at threshold and show that for the unbroken $\phi^4$ theory they vanish for $n>4~$, for the Standard Model Higgs they vanish for $n\ge 3~$ and for a model potential, respecting tree-order unitarity, for $n$ even and $n>4~$. Finally, we calculate the imaginary part of the one-loop $1\to n$ amplitude in both symmetric and spontaneously broken $\phi^4$ theory.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1992
record_format invenio
spelling cern-5594912021-07-15T22:58:33Zdoi:10.1016/0550-3213(93)90205-4http://cds.cern.ch/record/559491engArgyres, E.N.Papadopoulos, Costas G.Kleiss, Ronald H.P.Multiscalar production amplitudes beyond thresholdParticle Physics - PhenomenologyWe present exact tree-order amplitudes for $H^* \to n~H$, for final states containing one or two particles with non-zero three-momentum, for various interaction potentials. We show that there are potentials leading to tree amplitudes that satisfy unitarity, not only at threshold but also in the above kinematical configurations and probably beyond. As a by-product, we also calculate $2\to n$ tree amplitudes at threshold and show that for the unbroken $\phi^4$ theory they vanish for $n>4~$, for the Standard Model Higgs they vanish for $n\ge 3~$ and for a model potential, respecting tree-order unitarity, for $n$ even and $n>4~$. Finally, we calculate the imaginary part of the one-loop $1\to n$ amplitude in both symmetric and spontaneously broken $\phi^4$ theory.We present exact tree-order amplitudes for $H~* \to nH$, for final states containing one or two particles with non-zero three-momentum, for various interaction potentials. We show that there are potentials leading to tree amplitudes that satisfy unitarity, not only at threshold but also in the above kinematical configurations and probably beyond. As a by-product, we also calculate $2\to n$ tree amplitudes at threshold and show that for the unbroken $\phi~4$ theory they vanish for $n>4$, for the Standard Model Higgs they vanish for $n\ge 3$ and for a model potential, respecting tree-order unitarity, for $n$ even and $n>4$. Finally, we calculate the imaginary part of the one-loop $1\to n$ amplitude in both symmetric and spontaneously broken $\phi~4$ theory.We present exact tree-order amplitudes for $H~* \to nH$, for final states containing one or two particles with non-zero three-momentum, for various interaction potentials. We show that there are potentials leading to tree amplitudes that satisfy unitarity, not only at threshold but also in the above kinematical configurations and probably beyond. As a by-product, we also calculate $2\to n$ tree amplitudes at threshold and show that for the unbroken $\phi~4$ theory they vanish for $n>4$, for the Standard Model Higgs they vanish for $n\ge 3$ and for a model potential, respecting tree-order unitarity, for $n$ even and $n>4$. Finally, we calculate the imaginary part of the one-loop $1\to n$ amplitude in both symmetric and spontaneously broken $\phi~4$ theory.We present exact tree-order amplitudes for H ∗ → n H , for final states containing one or two particles with non-zero three-momentum, for various interaction potentials. We show that there are potentials leading to tree amplitudes that satisfy unitary, not only at threshold but also in the above kinematical configurations and probably beyond. As a by-product, we also calculated 2 → n tree amplitudes at threshold and show that for the unbroken ifφ 4 theory they vanish for n ⩾ 4, for the standard Model Higgs they vanish for n ⪖ 3 and for a model potential, respecting tree-order unitarity, for n even and n ⩾ 4. Finally, we calculate the imaginary part of the one-loop 1 → n amplitude in both symmetric and spontaneously broken φ 4 theory.hep-ph/9211237CERN-TH-6714-92CERN-TH-6714-92oai:cds.cern.ch:5594911992-11-11
spellingShingle Particle Physics - Phenomenology
Argyres, E.N.
Papadopoulos, Costas G.
Kleiss, Ronald H.P.
Multiscalar production amplitudes beyond threshold
title Multiscalar production amplitudes beyond threshold
title_full Multiscalar production amplitudes beyond threshold
title_fullStr Multiscalar production amplitudes beyond threshold
title_full_unstemmed Multiscalar production amplitudes beyond threshold
title_short Multiscalar production amplitudes beyond threshold
title_sort multiscalar production amplitudes beyond threshold
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0550-3213(93)90205-4
http://cds.cern.ch/record/559491
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AT papadopouloscostasg multiscalarproductionamplitudesbeyondthreshold
AT kleissronaldhp multiscalarproductionamplitudesbeyondthreshold