Celso C. Nishi
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
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Celso C. Nishi has a total of 53 co-authors. Here are the top co-authors by number of shared publications:
- Alex Gomes Dias
Centro de Ciências Naturais e Humanas Universidade Federal do ABC UFABC 09210-580 Santo André-SP Brazil
12 shared publications - Adriano Cherchiglia
Universidade Estadual de Campinas
11 shared publications - Igor P. Ivanov
School of Physics and Astronomy Sun Yat-Sen University 519082 Zhuhai China
11 shared publications - Bruce L. Sánchez-Vega
UFMG
7 shared publications - G. De Conto
Centro de Ciências Naturais e Humanas Universidade Federal do ABC Santo André-SP Brasil
7 shared publications - Adriano Cherchiglia
Centro de Ciências Naturais e Humanas Universidade Federal do ABC 09.210-170 Santo André-SP Brasil
5 shared publications
Latest Publications
- Open Access
- 15 June 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (1)
Nelson-Barr models with vectorlike quark doublets
We investigate Nelson-Barr (NB) solutions to the strong C P problem in which spontaneous C P violation is transmitted to the Standard Model (SM) through mixing with a vectorlike partner of the SM quark doublet. We show that these constructions constitute compelling and phenomenologically viable alternatives to the more widely studied singlet-based NB models. A key result of our analysis is that an accidental symmetry of the renormalizable theory delays the leading contributions to θ ¯ until three loops, naturally suppressing hadronic C P violation. We outline the main phenomenological constraints, including future electric dipole moment experiments, as well as the main differences between these scenarios and generic models with doublet vectorlike quarks.
- 15 June 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (1)
Open AccessNelson-Barr models with vectorlike quark doublets
We investigate Nelson-Barr (NB) solutions to the strong C P problem in which spontaneous C P violation is transmitted to the Standard Model (SM) through mixing with a vectorlike partner of the SM quark doublet. We show that these constructions constitute compelling and phenomenologically viable alternatives to the more widely studied singlet-based NB models. A key result of our analysis is that an accidental symmetry of the renormalizable theory delays the leading contributions to θ ¯ until three loops, naturally suppressing hadronic C P violation. We outline the main phenomenological constraints, including future electric dipole moment experiments, as well as the main differences between these scenarios and generic models with doublet vectorlike quarks.
- Open Access
- 27 October 2025
- Published by American Physical Society (APS) in Physical Review D
- Vol. 112 (7)
Aligned Zee-Grimus-Neufeld model for ( g − 2 ) μ
The recent result of the Fermilab Muon g-2 experiment is still in conflict with the standard model (SM) prediction if dispersive methods are used as input for the hadronic vacuum polarization. We seek models where the same set of mediators around the weak scale or above contribute to neutrino masses and to the muon g − 2 through a chiral enhanced contribution. As family lepton number violation is inherent to the former, non-negligible charged lepton flavor violation will be induced. We arrive at the following field content additional to the SM: one Higgs doublet, one singly charged scalar, and one right-handed neutrino. Neutrino masses will be generated by a combination of mechanisms: the tree-level seesaw, Zee mechanism, and Grimus-Neufeld mechanism, while lepton flavor violation will be minimized by considering Yukawa-aligned Higgs doublets. The setting is flexible enough to account for ( g − 2 ) μ , the Cabibbo angle anomaly, and the W mass deviation, while avoiding dangerous charged lepton flavor violation.
- 27 October 2025
- Published by American Physical Society (APS) in Physical Review D
- Vol. 112 (7)
Open AccessAligned Zee-Grimus-Neufeld model for ( g − 2 ) μ
The recent result of the Fermilab Muon g-2 experiment is still in conflict with the standard model (SM) prediction if dispersive methods are used as input for the hadronic vacuum polarization. We seek models where the same set of mediators around the weak scale or above contribute to neutrino masses and to the muon g − 2 through a chiral enhanced contribution. As family lepton number violation is inherent to the former, non-negligible charged lepton flavor violation will be induced. We arrive at the following field content additional to the SM: one Higgs doublet, one singly charged scalar, and one right-handed neutrino. Neutrino masses will be generated by a combination of mechanisms: the tree-level seesaw, Zee mechanism, and Grimus-Neufeld mechanism, while lepton flavor violation will be minimized by considering Yukawa-aligned Higgs doublets. The setting is flexible enough to account for ( g − 2 ) μ , the Cabibbo angle anomaly, and the W mass deviation, while avoiding dangerous charged lepton flavor violation.
- Open Access
- 19 September 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (9) , e22
Effective description of Nelson-Barr models and the theta parameter
Nelson-Barr theories solve the strong CP problem with CP spontaneously broken at Λcp and transmitted to the CP conserving version of the SM through vector-like quarks (VLQs). For an arbitrary number of CP breaking scalars and VLQs, we perform the full one-loop matching calculations at Λcp up to dimension five operators and the relevant matching calculations at the VLQ scale relevant to tracking the contributions to the parameter $$ \overline{\theta} $$ . In the EFT after the CP breaking scalars have been integrated out, we confirm that the running of $$ \overline{\theta} $$ at one-loop is induced by CP violating dimension five operators and similarly by dimension six operator after matching to the SMEFT. In the latter, an additional contribution enters in the matching to $$ \overline{\theta} $$ at tree-level due to a dimension five operator. Analyzing the experimental constraint from $$ \overline{\theta} $$ for generic settings, we see that a large separation between Λcp and the VLQ scale already suppresses the one-loop contribution to $$ \overline{\theta} $$ sufficiently. We confirm that a simple extension based on a nonconventional CP has vanishing one-loop contribution to $$ \overline{\theta} $$ . Part of our results can be also applied to generic VLQ extensions of the SM.- 19 September 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (9) , e22
Open AccessEffective description of Nelson-Barr models and the theta parameter
Nelson-Barr theories solve the strong CP problem with CP spontaneously broken at Λcp and transmitted to the CP conserving version of the SM through vector-like quarks (VLQs). For an arbitrary number of CP breaking scalars and VLQs, we perform the full one-loop matching calculations at Λcp up to dimension five operators and the relevant matching calculations at the VLQ scale relevant to tracking the contributions to the parameter $$ \overline{\theta} $$ . In the EFT after the CP breaking scalars have been integrated out, we confirm that the running of $$ \overline{\theta} $$ at one-loop is induced by CP violating dimension five operators and similarly by dimension six operator after matching to the SMEFT. In the latter, an additional contribution enters in the matching to $$ \overline{\theta} $$ at tree-level due to a dimension five operator. Analyzing the experimental constraint from $$ \overline{\theta} $$ for generic settings, we see that a large separation between Λcp and the VLQ scale already suppresses the one-loop contribution to $$ \overline{\theta} $$ sufficiently. We confirm that a simple extension based on a nonconventional CP has vanishing one-loop contribution to $$ \overline{\theta} $$ . Part of our results can be also applied to generic VLQ extensions of the SM. - Open Access
- 27 November 2024
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2024 (11) , 1-33
Flavor invariants for the SM with one singlet vector-like quark
We study the flavor invariants of the SM augmented by one singlet vector-like quark. Aided by the Hilbert series, we construct all the basic invariants with which any flavor invariant can be written as a polynomial. In special, this theory contains one CP odd invariant of degree six which has degree much lower than the usual Jarlskog invariant of the SM. We find the nonlinear polynomial relations (syzygies) of lowest degrees involving these basic invariants, including the expression of the square of the CP odd invariant of lowest degree in terms of CP even invariants. The SU(3) identity underlying this syzygy is uncovered in terms of invariant tensors, which can be applied to rewrite any square of a CP odd invariant of the same form, involving three hermitean matrices of size three. We demonstrate by an example that there is CP violation that is not detected by the CP odd invariants proposed in the literature so far but it can be detected with the full list of CP odd invariants found here.
- 27 November 2024
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2024 (11) , 1-33
Open AccessFlavor invariants for the SM with one singlet vector-like quark
We study the flavor invariants of the SM augmented by one singlet vector-like quark. Aided by the Hilbert series, we construct all the basic invariants with which any flavor invariant can be written as a polynomial. In special, this theory contains one CP odd invariant of degree six which has degree much lower than the usual Jarlskog invariant of the SM. We find the nonlinear polynomial relations (syzygies) of lowest degrees involving these basic invariants, including the expression of the square of the CP odd invariant of lowest degree in terms of CP even invariants. The SU(3) identity underlying this syzygy is uncovered in terms of invariant tensors, which can be applied to rewrite any square of a CP odd invariant of the same form, involving three hermitean matrices of size three. We demonstrate by an example that there is CP violation that is not detected by the CP odd invariants proposed in the literature so far but it can be detected with the full list of CP odd invariants found here.
- Open Access
Vector-like Singlet Quarks: a Roadmap
We review the theory and phenomenology of isosinglet vector-like quarks (VLQs). In recent years, interest in VLQs has been increasing, due to their contributions to new physics effects that can be tested in experiments at LHC and High-Luminosity LHC. The similarities of models with isosinglet VLQs and the seesaw framework in the leptonic sector are pointed out. The existence of VLQs leads to flavour-changing neutral currents at tree level and deviations from unitarity of the CKM matrix, introducing rich phenomenological implications. These new effects are naturally suppressed by the masses of the new quarks, that are constrained to be above the electroweak scale. In addition, striking new effects can be achieved with the inclusion of an extra complex scalar singlet. Such a minimal extension of the SM can give rise to new sources of CP violation with profound theoretical implications, allowing for a solution to the strong CP problem and a possible explanation for the baryon asymmetry of the Universe. We list and explain strong motivations to consider this class of models. We also briefly review how models with VLQs can be matched to the SM effective field theory (SMEFT). A detailed analysis of flavour observables that can be affected by the presence of VLQs is presented. Current bounds from collider searches of VLQs are summarized. We point out that the discovery of VLQs can be within the reach of present or future colliders being planned.
Open AccessVector-like Singlet Quarks: a Roadmap
We review the theory and phenomenology of isosinglet vector-like quarks (VLQs). In recent years, interest in VLQs has been increasing, due to their contributions to new physics effects that can be tested in experiments at LHC and High-Luminosity LHC. The similarities of models with isosinglet VLQs and the seesaw framework in the leptonic sector are pointed out. The existence of VLQs leads to flavour-changing neutral currents at tree level and deviations from unitarity of the CKM matrix, introducing rich phenomenological implications. These new effects are naturally suppressed by the masses of the new quarks, that are constrained to be above the electroweak scale. In addition, striking new effects can be achieved with the inclusion of an extra complex scalar singlet. Such a minimal extension of the SM can give rise to new sources of CP violation with profound theoretical implications, allowing for a solution to the strong CP problem and a possible explanation for the baryon asymmetry of the Universe. We list and explain strong motivations to consider this class of models. We also briefly review how models with VLQs can be matched to the SM effective field theory (SMEFT). A detailed analysis of flavour observables that can be affected by the presence of VLQs is presented. Current bounds from collider searches of VLQs are summarized. We point out that the discovery of VLQs can be within the reach of present or future colliders being planned.
- Open Access
- 17 November 2023
- Published by American Physical Society (APS) in Physical Review D
- Vol. 108 (9) , 095031
Leptonicviolation from the seesaw mechanismThe seesaw extension of the SM explains the tiny neutrino masses, and it is accompanied by many violating phases. We study the case where all leptonic violation arises from the soft breaking in the heavy Majorana mass matrix. Parameter counting reveals that one less parameter is needed to describe this case. This reduction leads to restrictions on the parameter space of heavy neutrinos. We analyze the minimal seesaw case in detail and find that mass degeneracy of heavy neutrinos is not possible for certain values of the phases.- 17 November 2023
- Published by American Physical Society (APS) in Physical Review D
- Vol. 108 (9) , 095031
Open AccessLeptonicviolation from the seesaw mechanismThe seesaw extension of the SM explains the tiny neutrino masses, and it is accompanied by many violating phases. We study the case where all leptonic violation arises from the soft breaking in the heavy Majorana mass matrix. Parameter counting reveals that one less parameter is needed to describe this case. This reduction leads to restrictions on the parameter space of heavy neutrinos. We analyze the minimal seesaw case in detail and find that mass degeneracy of heavy neutrinos is not possible for certain values of the phases. - Open Access
Leptonic CP violation from the seesaw
The seesaw extension of the SM explains the tiny neutrino masses and it is accompanied by many CP violating phases. We study the case where all leptonic CP violation arises from the soft breaking in the heavy Majorana mass matrix. Parameter counting reveals that one less parameter is needed to describe this case. This reduction leads to restrictions on the parameter space of heavy neutrinos. We analyze the minimal seesaw case in detail and find that mass degeneracy of heavy neutrinos is not possible for certain values of the CP phases.
Open AccessLeptonic CP violation from the seesaw
The seesaw extension of the SM explains the tiny neutrino masses and it is accompanied by many CP violating phases. We study the case where all leptonic CP violation arises from the soft breaking in the heavy Majorana mass matrix. Parameter counting reveals that one less parameter is needed to describe this case. This reduction leads to restrictions on the parameter space of heavy neutrinos. We analyze the minimal seesaw case in detail and find that mass degeneracy of heavy neutrinos is not possible for certain values of the CP phases.
- Open Access
- 29 August 2023
- Published by American Physical Society (APS) in Physical Review D
- Vol. 108 (3) , 035049
Explicit parametrization of more than one vectorlike quark of Nelson-Barr type
Nelson-Barr models solve the strong problem based on spontaneous violation and generically require vectorlike quarks (VLQs) mixing with standard quarks to transmit the violation. We devise an explicit parametrization for the case of two VLQs of either down or up type and quantitatively study several aspects including the hierarchy of the VLQ Yukawas and their irreducible contribution to . In particular, with the use of the parametrization, we show that a big portion of the parameter space for two up-type VLQs at the TeV scale is still allowed by the constraint on , although this case had been previously shown to be very restricted based on estimates.- 29 August 2023
- Published by American Physical Society (APS) in Physical Review D
- Vol. 108 (3) , 035049
Open AccessExplicit parametrization of more than one vectorlike quark of Nelson-Barr type
Nelson-Barr models solve the strong problem based on spontaneous violation and generically require vectorlike quarks (VLQs) mixing with standard quarks to transmit the violation. We devise an explicit parametrization for the case of two VLQs of either down or up type and quantitatively study several aspects including the hierarchy of the VLQ Yukawas and their irreducible contribution to . In particular, with the use of the parametrization, we show that a big portion of the parameter space for two up-type VLQs at the TeV scale is still allowed by the constraint on , although this case had been previously shown to be very restricted based on estimates. - Open Access
- 25 August 2023
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2023 (8) , 1-33
Connecting (g − 2)μ to neutrino mass in the extended neutrinophilic 2HDM
One simple way to lower the scale of the seesaw mechanism that generates neutrino masses is to attribute part of their smallness to a suppressed vacuum expectation value of a second Higgs doublet as in the neutrinophilic 2HDM or in the type IB seesaw model. On that structure we add one charged singlet scalar to induce a chirally enhanced contribution to (g – 2)μ with the same righthanded neutrinos of the seesaw. We discuss the interplay of generating the necessary contribution to the latter with lepton flavor violation which is also necessarily brought to low scale. We show that it is possible to explain (g –2)μ even for heavy neutrino masses of order of a few TeV.
- 25 August 2023
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2023 (8) , 1-33
Open AccessConnecting (g − 2)μ to neutrino mass in the extended neutrinophilic 2HDM
One simple way to lower the scale of the seesaw mechanism that generates neutrino masses is to attribute part of their smallness to a suppressed vacuum expectation value of a second Higgs doublet as in the neutrinophilic 2HDM or in the type IB seesaw model. On that structure we add one charged singlet scalar to induce a chirally enhanced contribution to (g – 2)μ with the same righthanded neutrinos of the seesaw. We discuss the interplay of generating the necessary contribution to the latter with lepton flavor violation which is also necessarily brought to low scale. We show that it is possible to explain (g –2)μ even for heavy neutrino masses of order of a few TeV.
- Open AccessConnecting $(g-2)_μ$ to neutrino mass in the extended neutrinophilic 2HDMOne simple way to lower the scale of the seesaw mechanism that generates neutrino masses is to attribute part of their smallness to a suppressed vacuum expectation value of a second Higgs doublet as in the neutrinophilic 2HDM or in the type IB seesaw model. On that structure we add one charged singlet scalar to induce a chirally enhanced contribution to $(g-2)_μ$ with the same righthanded neutrinos of the seesaw. We discuss the interplay of generating the necessary contribution to the latter with lepton flavor violation which is also necessarily brought to low scale. We show that it is possible to explain $(g-2)_μ$ even for heavy neutrino masses of order of a few TeV.Open AccessConnecting $(g-2)_μ$ to neutrino mass in the extended neutrinophilic 2HDMOne simple way to lower the scale of the seesaw mechanism that generates neutrino masses is to attribute part of their smallness to a suppressed vacuum expectation value of a second Higgs doublet as in the neutrinophilic 2HDM or in the type IB seesaw model. On that structure we add one charged singlet scalar to induce a chirally enhanced contribution to $(g-2)_μ$ with the same righthanded neutrinos of the seesaw. We discuss the interplay of generating the necessary contribution to the latter with lepton flavor violation which is also necessarily brought to low scale. We show that it is possible to explain $(g-2)_μ$ even for heavy neutrino masses of order of a few TeV.