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Angular sampling was evaluated in the determination of dasometric variables in Tectona grandis
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201
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202por Bjoern, Mikkel“…These proceedings describe two LHCb measurements of the CKM angle $\gamma$: a measurement with $B^0\to D K^{*0}$ decays where the $D$ meson decays into two- and four-body final states, using proton-proton collision data corresponding to an integrated luminosity of $5\,\text{fb}^{-1}$, and a measurement using $B^\pm\to DK^\pm$ decays where the $D$ decays into the final states $K_\text{S}^0\pi^+\pi^-$ and $K_\text{S}^0K^+K^-$, using data corresponding to an integrated luminosity of $2\,\text{fb}^{-1}$. …”
Publicado 2020
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203
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204por Krupa, Wojciech“…The tree-level measurement of the CKM angle γ is one of the most important tests of CP violation in the Standard Model. …”
Publicado 2022
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205por Arbuzov, A B, Fadin, V S, Kuraev, E A, Lipatov, L N, Merenkov, N P, Trentadue, L G“…We present the results of our calculations to a one, two, and three loop approximation of the e^+e^-\rightarrow e^+e^- Bhabha scattering cross-section at small angles. All terms contributing to the radiatively corrected cross-section, within an accuracy of \delta\sigma/ \sigma = 0.1 \% , are explicitely evaluated and presented in an analytic form. …”
Publicado 1995
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206“…In our work we show how to include wide-angle effects into the 3-dimensional observed galaxy bispectrum. …”
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207por Florian, Rehm, Vallecorsa Sofia, Grossi Michele, Kerstin, Borras, Krücker Dirk, Schnake Simon, Alexis-Harilaos, Verney-Provatas“…The Quantum Angle Generator (QAG) is a new generative model for quantum computers. …”
Publicado 2022
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208
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209
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210
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211por Alvsvaag, S J, Maeland, O A, Klovning, A, Benvenuti, Alberto C, Giordano, V, Guerzoni, M, Navarria, Francesco Luigi, Verardi, M G, Camporesi, T, Vallazza, E, Bozzo, M, Cereseto, R, Barreira, G, Espirito-Santo, M C, Maio, A, Onofre, A, Peralta, L, Pimenta, M, Tomé, B, Carling, H, Falk, E, Hedberg, V, Jarlskog, G, Kronkvist, I J, Bonesini, M, Chignoli, F, Ferrari, P, Gumenyuk, S A, Leoni, R, Mazza, R, Negri, P, Paganoni, M, Petrovykh, L P, Dharmasiri, D R, Nossum, B, Read, A L, Skaali, B, Castellani, L, Pegoraro, M, Fenyuk, A, Guz, Yu, Ivaniouchenkov, Yu, Karyukhin, A N, Obraztsov, V F, Vlasov, E, Zaitsev, A, Bigi, M, Cassio, V, Gamba, D, Migliore, E, Romero, A, Simonetti, L, Torassa, E, Trapani, P P, Bari, M D, Della Ricca, G, Lanceri, L, Poropat, P, Prest, MEnlace del recurso
Publicado 1995
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212por Alvsvaag, S J, Maeland, O A, Klovning, A, Benvenuti, Alberto C, Giordano, V, Guerzoni, M, Navarria, Francesco Luigi, Verardi, M G, Camporesi, T, Vallazza, E, Bozzo, M, Cereseto, R, Barreira, G, Espirito-Santo, M C, Maio, A, Onofre, A, Pimenta, M, Tomé, B, Carling, H, Falk, E, Hedberg, V, Jarlskog, G, Kronkvist, I J, Bonesini, M, Chignoli, F, Ferrari, P, Gumenyuk, S A, Leoni, R, Mazza, R, Negri, P, Paganoni, M, Petrovykh, L P, Dharmasiri, D R, Nossum, B, Read, A L, Skaali, B, Castellani, L, Pegoraro, M, Fenyuk, A, Guz, Yu, Ivaniouchenkov, Yu, Karyukhin, A N, Obraztsov, V F, Vlasov, E, Zaitsev, A, Bigi, M, Cassio, V, Gamba, D, Migliore, E, Romero, A, Simonetti, L, Torassa, E, Trapani, P P, Bari, M D, Della Ricca, G, Lanceri, L, Poropat, P, Prest, MEnlace del recurso
Publicado 1995
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213
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214“…We consider a family of non-supersymmetric MQCD five-brane configurations introduced by Witten, and discuss the dependence of the curves on the microscopic Theta angle and its relation with CP. We find evidence for a non-trivial spectral-flow of the curves (vacua) and for the level-crossing of adjacent curves at a particular value of the Theta angle, with spontaneous breaking of CP symmetry, providing an MQCD analog of the phase transitions in Theta proposed by 't Hooft.…”
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215por Fleischer, Robert“…The determination of the angle $\gamma$ of the unitarity triangle of the CKM matrix is regarded as a challenge for future $B$-physics experiments. …”
Publicado 1998
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216“…The theoretical accuracy of the program TOPAZ0 in the large-angle Bhabha channel is estimated. The physical error associated with the full Bhabha cross section and its forward and backward components separately is given for some event selections and several energy points of interest for LEP1 physics, both for the $s$ and non-$s$ contributions to the cross section.…”
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