Odd Magne Ogreid
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Odd Magne Ogreid has a total of 23 co-authors. Here are the top co-authors by number of shared publications:
- Per Osland
University of Bergen
67 shared publications - Bohdan Grzadkowski
University of Warsaw
30 shared publications - Margarida Nesbitt Rebelo
Universidade de Lisboa
28 shared publications - Anton Kuncinas
Centro de Física Teórica de Partículas CFTP Departamento de Física Instituto Superior Técnico Universidade de Lisboa Avenida Rovisco Pais nr. 1 1049-001 Lisboa Portugal
10 shared publications - Pedro. M. Ferreira
Instituto Superior de Engenharia de Lisboa
8 shared publications - Howard E. Haber
Santa Cruz Institute for Particle Physics University of California 1156 High Street 95064 Santa Cruz CA USA
5 shared publications
Latest Publications
- Open Access
- 13 July 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (7) , 108
CP violation in H± → W±Z: a physical approach for the 2HDM
A bstract: We investigate CP violation in the process H ± → W ± Z within the framework of the two-Higgs-Doublet model (2HDM). Amplitudes are expressed transparently in terms of physical couplings. Our analysis qualitatively confirms recent results by Kanemura and Mura, for the interference between one-loop bosonic and fermionic amplitudes. Furthermore, we identify additional sources of CP violation arising from internal interference among the bosonic and also among the fermionic loop amplitudes. In the alignment limit, the asymmetry would vanish in the absence of fermionic loop contributions when the sum of the masses of the additional neutral scalars is higher than the mass of the Z . Our results allow for generic Yukawa couplings, and cover both explicit and spontaneous CP violation. For inclusive W ± and Z decays, the CP violation will only manifest itself as a charge asymmetry.
- 13 July 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (7) , 108
Open AccessCP violation in H± → W±Z: a physical approach for the 2HDM
A bstract: We investigate CP violation in the process H ± → W ± Z within the framework of the two-Higgs-Doublet model (2HDM). Amplitudes are expressed transparently in terms of physical couplings. Our analysis qualitatively confirms recent results by Kanemura and Mura, for the interference between one-loop bosonic and fermionic amplitudes. Furthermore, we identify additional sources of CP violation arising from internal interference among the bosonic and also among the fermionic loop amplitudes. In the alignment limit, the asymmetry would vanish in the absence of fermionic loop contributions when the sum of the masses of the additional neutral scalars is higher than the mass of the Z . Our results allow for generic Yukawa couplings, and cover both explicit and spontaneous CP violation. For inclusive W ± and Z decays, the CP violation will only manifest itself as a charge asymmetry.
- Open Access
- 2 July 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (7)
GOOFy — a systematic approach
A bstract: We investigate in detail a new class (GOOFy) of transformations for bosonic and fermionic fields that leave relevant parts of the Lagrangian density unchanged. The transformations act upon complex scalar fields Φ and Φ † employing generalized charge conjugation ( C ) transformation in a non-consistent manner , i.e. allowing for Φ † → (Φ † ) ′ ≠ (Φ ′ ) † . Requiring invariance of the kinetic terms under such transformations specifies the form of (Φ † ) ′ . An analogous strategy is also adopted for fermionic fields. This offers a systematic way to construct new GOOFy-invariant field-theoretical models. It turns out that theories which are invariant with respect to these GOOFy transformations satisfy relations among parameters that are found to be RGE-stable up to two and three loop orders, thus constituting fixed-points under running of the RGE. This has been verified for various theories containing different numbers of bosonic and fermionic fields. In particular it has been shown that the Standard Model (SM) can not be a viable electroweak theory if demanding invariance under GOOFy transformations. However, the two-Higgs-Doublet Model (2HDM) may be invariant under GOOFy transformations (Yukawa couplings included), providing an interesting phenomenological example of physics beyond the SM. The most striking aspect of this study is the RGE stability of new relations between model parameters in a wide class of field theories. We also present a set of new relations between 2HDM potential parameters that constitute a fixed point under the running of the RGE up to at least three loop order.
- 2 July 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (7)
Open AccessGOOFy — a systematic approach
A bstract: We investigate in detail a new class (GOOFy) of transformations for bosonic and fermionic fields that leave relevant parts of the Lagrangian density unchanged. The transformations act upon complex scalar fields Φ and Φ † employing generalized charge conjugation ( C ) transformation in a non-consistent manner , i.e. allowing for Φ † → (Φ † ) ′ ≠ (Φ ′ ) † . Requiring invariance of the kinetic terms under such transformations specifies the form of (Φ † ) ′ . An analogous strategy is also adopted for fermionic fields. This offers a systematic way to construct new GOOFy-invariant field-theoretical models. It turns out that theories which are invariant with respect to these GOOFy transformations satisfy relations among parameters that are found to be RGE-stable up to two and three loop orders, thus constituting fixed-points under running of the RGE. This has been verified for various theories containing different numbers of bosonic and fermionic fields. In particular it has been shown that the Standard Model (SM) can not be a viable electroweak theory if demanding invariance under GOOFy transformations. However, the two-Higgs-Doublet Model (2HDM) may be invariant under GOOFy transformations (Yukawa couplings included), providing an interesting phenomenological example of physics beyond the SM. The most striking aspect of this study is the RGE stability of new relations between model parameters in a wide class of field theories. We also present a set of new relations between 2HDM potential parameters that constitute a fixed point under the running of the RGE up to at least three loop order.
- Open Access
- 27 April 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 113 (7)
Imaginary scaling invariance of the one-loop effective potential
Recently, a hitherto unknown class of renormalization group stable relations between parameters of bosonic field theories has been identified and dubbed as the r 0 or “GOOFy” symmetries. Here, one-loop properties of the r 0 invariant two-Higgs doublet model and a minimal symmetric model are discussed. It is concluded that the symmetry is present at the one-loop provided the UV cutoff squared transforms nontrivially under r 0 . The minimal model requires the presence of two real fields.
- 27 April 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 113 (7)
Open AccessImaginary scaling invariance of the one-loop effective potential
Recently, a hitherto unknown class of renormalization group stable relations between parameters of bosonic field theories has been identified and dubbed as the r 0 or “GOOFy” symmetries. Here, one-loop properties of the r 0 invariant two-Higgs doublet model and a minimal symmetric model are discussed. It is concluded that the symmetry is present at the one-loop provided the UV cutoff squared transforms nontrivially under r 0 . The minimal model requires the presence of two real fields.
- Open Access
GOOFy -- a systematic approach
We investigate in detail a new class (GOOFy) of transformations for bosonic and fermionic fields that leave the Lagrangian density unchanged. The transformations act upon complex scalar fields Φand Φ^\dagger employing generalized charge conjugation (C) transformation in a non-consistent manner, i.e. allowing for Φ\dagger \to (Φ\dagger)^\prime \neq (Φ^\prime)^\dagger. Requiring invariance of the kinetic terms under such transformations specifies the form of (Φ\dagger)^\prime. An analogous strategy is also adopted for fermionic fields. This offers a systematic way to construct new GOOFy-invariant field-theoretical models. It turns out that theories which are invariant with respect these GOOFy transformations satisfy relations among parameters that are found to be RGE-stable up to two and three loop orders, thus constituting fixed-points under running of the RGE. This has been verified for various theories containing different numbers of bosonic and fermionic fields. In particular it has been shown that the Standard Model (SM) can not be a viable electroweak theory if demanding invariance under GOOFy transformations. However, the two-Higgs-Doublet Model (2HDM) may be invariant under GOOFy transformations (Yukawa couplings included), providing an interesting phenomenological example of physics beyond the SM. The most striking aspect of this study is the RGE stability of new relations between model parameters in a wide class of field theories. We also present a set of new relations between 2HDM potential parameters that constitute a fixed point under the running of the RGE up to at least three loop order.
Open AccessGOOFy -- a systematic approach
We investigate in detail a new class (GOOFy) of transformations for bosonic and fermionic fields that leave the Lagrangian density unchanged. The transformations act upon complex scalar fields Φand Φ^\dagger employing generalized charge conjugation (C) transformation in a non-consistent manner, i.e. allowing for Φ\dagger \to (Φ\dagger)^\prime \neq (Φ^\prime)^\dagger. Requiring invariance of the kinetic terms under such transformations specifies the form of (Φ\dagger)^\prime. An analogous strategy is also adopted for fermionic fields. This offers a systematic way to construct new GOOFy-invariant field-theoretical models. It turns out that theories which are invariant with respect these GOOFy transformations satisfy relations among parameters that are found to be RGE-stable up to two and three loop orders, thus constituting fixed-points under running of the RGE. This has been verified for various theories containing different numbers of bosonic and fermionic fields. In particular it has been shown that the Standard Model (SM) can not be a viable electroweak theory if demanding invariance under GOOFy transformations. However, the two-Higgs-Doublet Model (2HDM) may be invariant under GOOFy transformations (Yukawa couplings included), providing an interesting phenomenological example of physics beyond the SM. The most striking aspect of this study is the RGE stability of new relations between model parameters in a wide class of field theories. We also present a set of new relations between 2HDM potential parameters that constitute a fixed point under the running of the RGE up to at least three loop order.
- Open Access
CP violation in H^\pm \to W^\pm Z: A physical approach for the 2HDM
We investigate CP violation in the process H^\pm \to W^\pm Z within the framework of the two-Higgs-Doublet model (2HDM). Amplitudes are expressed transparently in terms of physical couplings. Our analysis qualitatively confirms recent results by Kanemura and Mura, for the interference between one-loop bosonic and fermionic amplitudes. Furthermore, we identify additional sources of CP violation arising from internal interference among the bosonic and also among the fermionic loop amplitudes. In the alignment limit, the asymmetry would vanish in the absence of fermionic loop contributions when the sum of the masses of the additional neutral scalars is higher than the mass of the Z. Our results allow for generic Yukawa couplings, and cover both explicit and spontaneous CP violation. For inclusive W^\pm and Z decays, the CP violation will only manifest itself as a charge asymmetry.
Open AccessCP violation in H^\pm \to W^\pm Z: A physical approach for the 2HDM
We investigate CP violation in the process H^\pm \to W^\pm Z within the framework of the two-Higgs-Doublet model (2HDM). Amplitudes are expressed transparently in terms of physical couplings. Our analysis qualitatively confirms recent results by Kanemura and Mura, for the interference between one-loop bosonic and fermionic amplitudes. Furthermore, we identify additional sources of CP violation arising from internal interference among the bosonic and also among the fermionic loop amplitudes. In the alignment limit, the asymmetry would vanish in the absence of fermionic loop contributions when the sum of the masses of the additional neutral scalars is higher than the mass of the Z. Our results allow for generic Yukawa couplings, and cover both explicit and spontaneous CP violation. For inclusive W^\pm and Z decays, the CP violation will only manifest itself as a charge asymmetry.
- Open Access
- 12 September 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (9) , 1-45
CP-violation in the Weinberg 3HDM potential
We explore the phenomenology of Weinberg’s ℤ 2 × ℤ 2 symmetric three-Higgs-doublet potential, allowing for spontaneous violation of CP due to complex vacuum expectation values. An overview of all possible ways of satisfying the stationary-point conditions is given, with one, two or three non-vanishing vacuum expectation values, together with conditions for CP conservation in terms of basis invariants. All possible ways of satisfying the conditions for CP conservation are given. Scans of allowed parameter regions are given, together with measures of CP violation, in terms of the invariants. The light states identified in an earlier paper are further explored in terms of their CP-violating couplings. Loop-induced CP violation in WWZ couplings, as well as charge-asymmetric scattering are also commented on.
- 12 September 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (9) , 1-45
Open AccessCP-violation in the Weinberg 3HDM potential
We explore the phenomenology of Weinberg’s ℤ 2 × ℤ 2 symmetric three-Higgs-doublet potential, allowing for spontaneous violation of CP due to complex vacuum expectation values. An overview of all possible ways of satisfying the stationary-point conditions is given, with one, two or three non-vanishing vacuum expectation values, together with conditions for CP conservation in terms of basis invariants. All possible ways of satisfying the conditions for CP conservation are given. Scans of allowed parameter regions are given, together with measures of CP violation, in terms of the invariants. The light states identified in an earlier paper are further explored in terms of their CP-violating couplings. Loop-induced CP violation in WWZ couplings, as well as charge-asymmetric scattering are also commented on.
- Open Access
Imaginary scaling
Recently, a hitherto unknown class of RG-stable relations between parameters of bosonic field theories have been identified and dubbed as the r0 or 'GOOFy' symmetries. Here, 1-loop properties of the r0 invariant 2-Higgs Doublet Model and a minimal symmetric model are discussed. It is concluded that the symmetry is present at the 1-loop provided the UV cut-off squared transforms non-trivially under r0. The minimal model requires the presence of two real fields.
Open AccessImaginary scaling
Recently, a hitherto unknown class of RG-stable relations between parameters of bosonic field theories have been identified and dubbed as the r0 or 'GOOFy' symmetries. Here, 1-loop properties of the r0 invariant 2-Higgs Doublet Model and a minimal symmetric model are discussed. It is concluded that the symmetry is present at the 1-loop provided the UV cut-off squared transforms non-trivially under r0. The minimal model requires the presence of two real fields.
- Open Access
- 6 March 2024
- Published by Springer Nature in The European Physical Journal C
- Vol. 84 (3) , 1-30
New symmetries of the two-Higgs-doublet model
The Two Higgs Doublet Model invariant under the gauge group $$SU(2)\times U(1)$$ is known to have six additional global discrete or continuous symmetries of its scalar sector. We have discovered regions of parameter space of the model which are basis and renormalization group invariant to all orders of perturbation theory in the scalar and gauge sectors, but correspond to none of the hitherto considered symmetries. We therefore identify seven new symmetries of the model and discuss their phenomenology. Soft symmetry breaking is required for some of these models so that electroweak symmetry breaking can occur. We show that, at least at the two-loop level, it is possible to extend some of these symmetries to include fermions.- 6 March 2024
- Published by Springer Nature in The European Physical Journal C
- Vol. 84 (3) , 1-30
Open AccessNew symmetries of the two-Higgs-doublet model
The Two Higgs Doublet Model invariant under the gauge group $$SU(2)\times U(1)$$ is known to have six additional global discrete or continuous symmetries of its scalar sector. We have discovered regions of parameter space of the model which are basis and renormalization group invariant to all orders of perturbation theory in the scalar and gauge sectors, but correspond to none of the hitherto considered symmetries. We therefore identify seven new symmetries of the model and discuss their phenomenology. Soft symmetry breaking is required for some of these models so that electroweak symmetry breaking can occur. We show that, at least at the two-loop level, it is possible to extend some of these symmetries to include fermions. - Open Access
- 31 January 2024
- Published by Sissa Medialab Srl
- Vol. 431, 031
Revisiting two dark matter candidates in $S_3$-symmetric three-Higgs-doublet models
Models with an extended scalar electroweak sector are well motivated. Such models could accommodate a dark matter candidate if there is an additional scalar representation with a vanishing vacuum expectation value and, in addition, there are no couplings between fermions and the dark matter candidate. The most natural way to have these conditions implemented is to consider models where an underlying symmetry is imposed. Governed by this, we consider a three-Higgs-doublet model with an $S_3$ symmetry. Within this framework there are different implementations which could possibly accommodate a dark matter candidate. The family of $S_3$-symmetric three-Higgs-doublet implementations arises due to different vacua and, as a result, different minimisation conditions. In this framework the dark matter candidate falls into the class of weakly interacting massive particles. The dark matter candidate is associated with an $\mathbb{Z}_2$ symmetry which survives spontaneous symmetry breaking and is a remnant of the $S_3$ symmetry. We explore two cases, they share many aspects of the Type-I two-Higgs-doublet model plus an inert SU(2) doublet. The main difference between these two cases is the presence of an irremovable phase, which leads to CP violation in one of the implementations. The two candidate cases differ from other previously studied models with three scalar doublets by the fact that they do not allow for heavy dark matter candidates, $\mathcal{O}(500)\text{ GeV}$. Valid dark matter regions were identified as $m_\mathrm{DM} \in [52.5,\,89]~\text{GeV}$ for a model without CP violation and $m_\mathrm{DM} \in [6.5,\,44.5]~\text{GeV}$ for a model with CP violation. In the present work we refine the parameter space by applying additional checks to our previous work coming from LHC data and from indirect detection data.- 31 January 2024
- Published by Sissa Medialab Srl
- Vol. 431, 031
Open AccessRevisiting two dark matter candidates in $S_3$-symmetric three-Higgs-doublet models
Models with an extended scalar electroweak sector are well motivated. Such models could accommodate a dark matter candidate if there is an additional scalar representation with a vanishing vacuum expectation value and, in addition, there are no couplings between fermions and the dark matter candidate. The most natural way to have these conditions implemented is to consider models where an underlying symmetry is imposed. Governed by this, we consider a three-Higgs-doublet model with an $S_3$ symmetry. Within this framework there are different implementations which could possibly accommodate a dark matter candidate. The family of $S_3$-symmetric three-Higgs-doublet implementations arises due to different vacua and, as a result, different minimisation conditions. In this framework the dark matter candidate falls into the class of weakly interacting massive particles. The dark matter candidate is associated with an $\mathbb{Z}_2$ symmetry which survives spontaneous symmetry breaking and is a remnant of the $S_3$ symmetry. We explore two cases, they share many aspects of the Type-I two-Higgs-doublet model plus an inert SU(2) doublet. The main difference between these two cases is the presence of an irremovable phase, which leads to CP violation in one of the implementations. The two candidate cases differ from other previously studied models with three scalar doublets by the fact that they do not allow for heavy dark matter candidates, $\mathcal{O}(500)\text{ GeV}$. Valid dark matter regions were identified as $m_\mathrm{DM} \in [52.5,\,89]~\text{GeV}$ for a model without CP violation and $m_\mathrm{DM} \in [6.5,\,44.5]~\text{GeV}$ for a model with CP violation. In the present work we refine the parameter space by applying additional checks to our previous work coming from LHC data and from indirect detection data. - Open Access
- 30 October 2023
- Published by American Physical Society (APS) in Physical Review D
- Vol. 108 (7) , 075029
Weinberg’s 3HDM potential with spontaneous violationWe study the potential of Weinberg’s -symmetric three-Higgs-doublet model. The potential is designed to accommodate violation in the scalar sector within a gauge theory, while at the same time allowing for natural flavor conservation. This framework allows for both explicit and spontaneous violation. can be explicitly violated when the coefficients of the potential are taken to be complex. With coefficients chosen to be real, can be spontaneously violated via complex vacuum expectation values (VEVs). In the absence of the terms leading to the possibility of violation, either explicit or induced by complex VEVs, the potential has two global symmetries. In this case, spontaneous symmetry breaking would, in general, give rise to massless states. In a realistic implementation, those terms must be included, thus preventing the existence of Goldstone bosons. A scan over parameters, imposing the existence of a neutral state at 125 GeV that is nearly even shows that, in the absence of fine-tuning, the scalar spectrum contains one or two states with masses below 125 GeV that have a significant -odd component. These light states would have a low production rate via the Bjorken process and could thus have escaped detection at the Large Electron-Positron Collider. At the LHC, the situation is less clear. While we do not here aim for a full phenomenological study of the light states, we point out that the decay channel would be challenging to measure because of suppressed couplings to .- 30 October 2023
- Published by American Physical Society (APS) in Physical Review D
- Vol. 108 (7) , 075029
Open AccessWeinberg’s 3HDM potential with spontaneous violationWe study the potential of Weinberg’s -symmetric three-Higgs-doublet model. The potential is designed to accommodate violation in the scalar sector within a gauge theory, while at the same time allowing for natural flavor conservation. This framework allows for both explicit and spontaneous violation. can be explicitly violated when the coefficients of the potential are taken to be complex. With coefficients chosen to be real, can be spontaneously violated via complex vacuum expectation values (VEVs). In the absence of the terms leading to the possibility of violation, either explicit or induced by complex VEVs, the potential has two global symmetries. In this case, spontaneous symmetry breaking would, in general, give rise to massless states. In a realistic implementation, those terms must be included, thus preventing the existence of Goldstone bosons. A scan over parameters, imposing the existence of a neutral state at 125 GeV that is nearly even shows that, in the absence of fine-tuning, the scalar spectrum contains one or two states with masses below 125 GeV that have a significant -odd component. These light states would have a low production rate via the Bjorken process and could thus have escaped detection at the Large Electron-Positron Collider. At the LHC, the situation is less clear. While we do not here aim for a full phenomenological study of the light states, we point out that the decay channel would be challenging to measure because of suppressed couplings to .