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Journal articles on the topic 'CP factorization'

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1

Lü, Gang, Jia-Qi Lei та Xin-Heng Guo. "CP Violation forB0→ρ0(ω)ρ0(ω)→π+π-π+π-in QCD Factorization". Advances in High Energy Physics 2014 (2014): 1–8. http://dx.doi.org/10.1155/2014/785648.

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In the QCD factorization (QCDF) approach we study the direct CP violation inB-0→ρ0(ω)ρ0(ω)→π+π-π+π-via theρ-ωmixing mechanism. We find that the CP violation can be enhanced by doubleρ-ωmixing when the masses of theπ+π-pairs are in the vicinity of theωresonance, and the maximum CP violation can reach 28%. We also compare the results from the naive factorization and the QCD factorization.
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2

Lihua, Gui, Zhao Xuyang, Zhao Qibin, and Cao Jianting. "Non-local Image Denoising by Using Bayesian Low-rank Tensor Factorization on High-order Patches." International Journal of Computer Science Issues 15, no. 5 (2018): 16–25. https://doi.org/10.5281/zenodo.1467648.

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Removing the noise from an image is vitally important in many real-world computer vision applications. One of the most effective method is block matching collaborative filtering, which employs low-rank approximation to the group of similar patches gathered by searching from the noisy image. However, the main drawback of this method is that the standard deviation of noises within the image is assumed to be known in advance, which is impossible for many real applications. In this paper, we propose a non-local filtering method by using the low-rank tensor decomposition method. For tensor decompos
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3

Liu, Chang, Kun He, Ji Liu Zhou, and Yan Li Zhu. "Facial Expression Recognition Based on Orthogonal Nonnegative CP Factorization." Advanced Materials Research 143-144 (October 2010): 111–15. http://dx.doi.org/10.4028/www.scientific.net/amr.143-144.111.

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Facial Expression recognition based on Non-negative Matrix Factorization (NMF) requires the object images should be vectorized. The vectorization leads to information loss, since local structure of the images is lost. Moreover, NMF can not guarantee the uniqueness of the decomposition. In order to remedy these limitations, the facial expression image was considered as a high-order tensor, and an Orthogonal Non-negative CP Factorization algorithm (ONNCP) was proposed. With the orthogonal constrain, the low-dimensional presentations of samples were non-negative in ONNCP. The convergence characte
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Cheng, Hai-Yang, and Chun-Khiang Chua. "The B-CP Puzzles in QCD Factorization." Nuclear Physics B - Proceedings Supplements 207-208 (October 2010): 391–94. http://dx.doi.org/10.1016/j.nuclphysbps.2010.10.102.

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5

Huang, Xingfang, Shuang Xu, Chunxia Zhang, and Jiangshe Zhang. "Robust CP Tensor Factorization With Skew Noise." IEEE Signal Processing Letters 27 (2020): 785–89. http://dx.doi.org/10.1109/lsp.2020.2991581.

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6

Cui, GaoChao, Li Zhu, LiHua Gui, QiBin Zhao, JianHai Zhang, and JianTing Cao. "Multidimensional clinical data denoising via Bayesian CP factorization." Science China Technological Sciences 63, no. 2 (2019): 249–54. http://dx.doi.org/10.1007/s11431-018-9493-9.

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7

Safir, A. Salim. "CP violation in B decays within QCD factorization." European Physical Journal C 33, S1 (2004): s373—s375. http://dx.doi.org/10.1140/epjcd/s2004-03-1831-x.

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8

Wu, Yuankai, Huachun Tan, Yong Li, Jian Zhang, and Xiaoxuan Chen. "A Fused CP Factorization Method for Incomplete Tensors." IEEE Transactions on Neural Networks and Learning Systems 30, no. 3 (2019): 751–64. http://dx.doi.org/10.1109/tnnls.2018.2851612.

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9

Brandts, Jan, and Michal Křížek. "Factorization of cp-rank-3 completely positive matrices." Czechoslovak Mathematical Journal 66, no. 3 (2016): 955–70. http://dx.doi.org/10.1007/s10587-016-0303-9.

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10

Rajarama Bhat, B. V., and Hiroyuki Osaka. "A factorization property of positive maps on C*-algebras." International Journal of Quantum Information 18, no. 05 (2020): 2050019. http://dx.doi.org/10.1142/s0219749920500197.

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The purpose of this short paper is to clarify and present a general version of an interesting observation by [Piani and Mora, Phys. Rev. A 75 (2007) 012305], linking complete positivity of linear maps on matrix algebras to decomposability of their ampliations. Let [Formula: see text], [Formula: see text] be unital C*-algebras and let [Formula: see text] be positive linear maps from [Formula: see text] to [Formula: see text] [Formula: see text]. We obtain conditions under which any positive map [Formula: see text] from the minimal C*-tensor product [Formula: see text] to [Formula: see text], su
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11

Raslan, E. H., and H. R. Khan. "Branching ratio and CP violation in Bs0 → K∗0K̄∗0 decay in the framework of QCD factorization." Modern Physics Letters A 35, no. 24 (2020): 2050201. http://dx.doi.org/10.1142/s0217732320502016.

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We present an analytic calculation of Branching Ratio (BR) and Charge-Parity (CP) violating asymmetries of the [Formula: see text] meson decay into the two light vectors [Formula: see text] by calculating the helicity amplitude in the framework of quantum chromodynamics (QCD) factorization approach. We find the BR of [Formula: see text] which is in full agreement with the recent theoretical predictions and experimental measurements. We also calculate the direct CP violation, CP violation in mixing and CP violation due to interference which are [Formula: see text], [Formula: see text], and [For
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12

Xing, Zhi-zhong. "Measuring CP violation and testing factorization in and decays." Physics Letters B 443, no. 1-4 (1998): 365–72. http://dx.doi.org/10.1016/s0370-2693(98)01285-4.

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13

Neubert, Matthias. "QCD factorization and CP asymmetries in hadronic B decays." Nuclear Physics B - Proceedings Supplements 99, no. 3 (2001): 113–20. http://dx.doi.org/10.1016/s0920-5632(01)01369-x.

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14

Zhou, Ruofei, Gang Wang, Bo Li, Jinlong Wang, Tianzhu Liu, and Chungang Liu. "Key-Frame Detection and Super-Resolution of Hyperspectral Video via Sparse-Based Cumulative Tensor Factorization." Mathematical Problems in Engineering 2020 (July 14, 2020): 1–20. http://dx.doi.org/10.1155/2020/9548749.

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Thanks to the rapid development of hyperspectral sensors, hyperspectral videos (HSV) can now be collected with high temporal and spectral resolutions and utilized to handle invisible dynamic monitoring missions, such as chemical gas plume tracking. However, using such sequential large-scale data effectively is challenged, because the direct process of these data requires huge demands in terms of computational loads and memory. This paper presents a key-frame and target-detecting algorithm based on cumulative tensor CANDECOMP/PARAFAC (CP) factorization (CTCF) to select the frames where the targ
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15

Afshar, Ardavan, Kejing Yin, Sherry Yan, et al. "SWIFT: Scalable Wasserstein Factorization for Sparse Nonnegative Tensors." Proceedings of the AAAI Conference on Artificial Intelligence 35, no. 8 (2021): 6548–56. http://dx.doi.org/10.1609/aaai.v35i8.16811.

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Existing tensor factorization methods assume that the input tensor follows some specific distribution (i.e. Poisson, Bernoulli, and Gaussian), and solve the factorization by minimizing some empirical loss functions defined based on the corresponding distribution. However, it suffers from several drawbacks: 1) In reality, the underlying distributions are complicated and unknown, making it infeasible to be approximated by a simple distribution. 2) The correlation across dimensions of the input tensor is not well utilized, leading to sub-optimal performance. Although heuristics were proposed to i
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16

LOISEAU, B., B. EL-BENNICH, A. FURMAN, R. KAMIŃSKI, L. LEŚNIAK та B. MOUSSALLAM. "πK INTERACTION EFFECTS ON CP VIOLATION IN B → Kπ+π- DECAYS". Modern Physics Letters A 24, № 11n13 (2009): 960–63. http://dx.doi.org/10.1142/s0217732309000371.

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We apply QCD factorization to the quasi two-body B → (Kπ)π decays where the (Kπ)-pair effective mass is limited to 1.8 GeV. Our strong interaction phases constrained by theory and πK experimental data yield useful information for studies of CP violation.
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17

Zhao, Qibin, Liqing Zhang, and Andrzej Cichocki. "Bayesian CP Factorization of Incomplete Tensors with Automatic Rank Determination." IEEE Transactions on Pattern Analysis and Machine Intelligence 37, no. 9 (2015): 1751–63. http://dx.doi.org/10.1109/tpami.2015.2392756.

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18

Raslan, E. H., та H. R. Khan. "Branching Ratio and CP Violation in B s 0 ¯ → ϕϕ Decay in the Framework of QCD Factorization". Atoms 8, № 2 (2020): 22. http://dx.doi.org/10.3390/atoms8020022.

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We present an analytic calculation of Branching Ratio (BR) and Charge-Parity (CP) violating asymmetries of the B s 0 ¯ meson decay into the two light vectors ϕ ϕ . In doing this we calculate the helicity amplitude of the present decay in the framework of QCD factorization approach. We find the BR of B s 0 ¯ → ϕ ϕ = ( 1.56 ± 0.23 ) × 10 − 5 . We also calculate the direct CP violation, CP violation in mixing and CP violation due to interference which are A C P dir = 0.00355 ± 0.00152 , A C P mix = − 0.00629 ± 0.03119 and A C P Δ Γ = 0.99997 ± 0.00019 , respectively. Our results are in agreement
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19

GIRI, ANJAN K., та RUKMANI MOHANTA. "DIRECT CP VIOLATION AND NEW PHYSICS EFFECTS IN THE DECAY MODE B+→ϕK+". Modern Physics Letters A 19, № 25 (2004): 1903–18. http://dx.doi.org/10.1142/s021773230401518x.

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We study the direct CP violation effect in the decay mode B+→ϕK+. This decay mode is dominated by the loop induced [Formula: see text] penguin diagram with a tiny contribution from the annihilation diagram. Therefore, the standard model expectation of direct CP violation is negligibly small. Using QCD factorization approach we find the CP asymmetry in the standard model to be at percent level. We consider then two scenarios beyond the standard model, the model with an extra vector-like down quark (VLDQ) and the R-parity violating supersymmetric model (RPV) and show that the direct CP violating
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20

LÜ, GANG, ZHEN-HUA ZHANG, XIU-YING LIU та LI-YING ZHANG. "NEW RESULT OF DIRECT CP VIOLATION IN B → π+π-π+π-". International Journal of Modern Physics A 26, № 17 (2011): 2899–912. http://dx.doi.org/10.1142/s0217751x11053626.

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In the framework of factorization, based on the first-order of isospin violation, we study direct CP violation in the decay of [Formula: see text] including the effect of ρ–ω mixing. The CP violation depends strongly on Cabibbo–Kobayashi–Maskawa (CKM) matrix elements and the effective parameter, Nc. Recently, the experimental data for the branching ratios of [Formula: see text] are accurate and we can give the strong constraint on the range of Nc. We find that the CP violating asymmetry is large and ranges from -82% to -98% via ρ–ω mixing mechanism when the invariant mass of the π+π- pair is i
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21

PAGÉ, VÉRONIQUE. "NEW PHYSICS SIGNALS THROUGH CP VIOLATION IN B→ρπ". International Journal of Modern Physics A 19, № 31 (2004): 5477–84. http://dx.doi.org/10.1142/s0217751x04022724.

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We describe here a method for detecting physics beyond the standard model via CP violation in B→ρπ decays. Using a Dalitz-plot analysis to obtain α, along with an analytical extraction of the various tree (T) and penguin (P) amplitudes, we obtain a criterion for the absence of new physics (NP). This criterion involves the comparison of the measured |P/T| ratio with its value as predicted by QCD factorization. We show that the detection of NP via this method has a good efficiency when compared with the corresponding technique using B→ππ decays.
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22

DAS, PRASANTA KUMAR. "FINDING γ FROM THE η-η′ MIXING WITHIN QCD FACTORIZATION". International Journal of Modern Physics A 22, № 14n15 (2007): 2493–511. http://dx.doi.org/10.1142/s0217751x07036543.

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We propose a method to determine the weak CP violating angle γ by analyzing the charmless nonleptonic B→(η, η′)K decay within the QCD factorization framework. We obtain constraints in the γ–θ (the octet-singlet mixing angle in η-η′ sector) contour plane by using the world average data of direct CP-asymmetry Acp(B→(η, η′)K) and the branching ratio BR (B+→(η, η′)K+). For Acp(B→η(η′)K) = -0.33±0.12(0.031±0.021), we find that γ lies in between 60°(20°) and 160°(160°) for θ = -21.3° for μ = mb/2, whereas for μ = mband the same θ, it lies in between 75°(20°) and 150°(160°). We discuss the two mixing
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23

Lü, Gang, та Qin-Qin Zhi. "Direct CP Violation from Isospin Symmetry Breaking Effects for the Decay Process B-s→P(V)π0 in PQCD". Advances in High Energy Physics 2019 (21 травня 2019): 1–14. http://dx.doi.org/10.1155/2019/6927130.

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We investigate the direct CP violation for the decay process of B-s→P(V)π0 (P,V refer to the pseudoscalar meson and vector meson, resp.) via isospin symmetry breaking effects from the π0-η-η′ mixing mechanism in PQCD factorization approach. Isospin symmetry breaking arises from the electroweak interaction and the u-d quark mass difference by the strong interaction, which are known to be tiny. However, we find that isospin symmetry breaking at the leading order shifts the CP violation due to the new strong phases.
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24

Raslan, E. H., та H. R. Khan. "Study of the branching ratio and CP asymmetries in Bs0¯ → ωϕ decay within QCD factorization". Modern Physics Letters A 35, № 38 (2020): 2050312. http://dx.doi.org/10.1142/s0217732320503125.

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We study analytically the Branching Ratio (BR) and Charge-Parity (CP) asymmetries of the [Formula: see text] decay mode within QCDF approach. We find the [Formula: see text]. We also find the values of CP asymmetries are [Formula: see text], [Formula: see text] and [Formula: see text]. The reported results are consistent with the recent theoretical predictions and can be used as a reference values in the forthcoming experiments.
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25

Bekius, Annike, Coen S. Zandvoort, Jennifer N. Kerkman, et al. "Neuromuscular Control before and after Independent Walking Onset in Children with Cerebral Palsy." Sensors 21, no. 8 (2021): 2714. http://dx.doi.org/10.3390/s21082714.

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Early brain lesions which produce cerebral palsy (CP) may affect the development of walking. It is unclear whether or how neuromuscular control, as evaluated by muscle synergy analysis, differs in young children with CP compared to typically developing (TD) children with the same walking ability, before and after the onset of independent walking. Here we grouped twenty children with (high risk of) CP and twenty TD children (age 6.5–52.4 months) based on their walking ability, supported or independent walking. Muscle synergies were extracted from electromyography data of bilateral leg muscles u
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26

DASS, G. V., and K. V. L. SARMA. "FACTORIZATION OF THE CHARGE CORRELATION FUNCTION IN $B^0 {\bar B}^0$ OSCILLATIONS." Modern Physics Letters A 13, no. 36 (1998): 2937–43. http://dx.doi.org/10.1142/s0217732398003119.

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Extraction of the mass difference Δm from [Formula: see text] oscillations involves tagging of bottom flavor at production and at decay. The charge correlation function is the asymmetry between the unmixed and mixed events. In their data using the lepton-jet-method, the ALEPH collaboration recently verified that this asymmetry factorizes into two parts, one depending on the production tag and the other on the decay tag. Except for this particular "verification", analyses of experiments on the time-dependence of beon oscillations have been assuming this factorization, without statement or expla
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27

Zhou, Hang, Bo Zheng та Zhen-Hua Zhang. "Analysis of CP Violation in D0→K+K-π0". Advances in High Energy Physics 2018 (22 листопада 2018): 1–11. http://dx.doi.org/10.1155/2018/7627308.

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We study the CP violation induced by the interference between two intermediate resonances K⁎(892)+ and K⁎(892)- in the phase space of singly-Cabibbo-suppressed decay D0→K+K-π0. We adopt the factorization-assisted topological approach in dealing with the decay amplitudes of D0→K±K⁎(892)∓. The CP asymmetries of two-body decays are predicted to be very tiny, which are (-1.27±0.25)×10-5 and (3.86±0.26)×10-5, respectively, for D0→K+K⁎(892)- and D0→K-K⁎(892)+, while the differential CP asymmetry of D0→K+K-π0 is enhanced because of the interference between the two intermediate resonances, which can r
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28

LÜ, CAI-DIAN. "QCD IN HADRONIC B DECAYS." Modern Physics Letters A 22, no. 07n10 (2007): 615–21. http://dx.doi.org/10.1142/s0217732307023201.

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The perturbative QCD approach is based on kT factorization, including the Sudakov form factors so that to avoid the endpoint singularity. In this approach, we calculate the charmless B decays like B → ππ decays etc. to produce the right number of branching ratios and also CP asymmetry parameters. For final states with at least one charmed meson, like B → Dπ decays, our results also agree with the experiments.
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29

Raslan, E. H., та H. R. Khan. "Study of the branching ratios and CP asymmetries in Bs0¯ → K∗0ρ0(ω) decays within QCD factorization". International Journal of Modern Physics A 35, № 26 (2020): 2050163. http://dx.doi.org/10.1142/s0217751x20501638.

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We study analytically the branching ratio (BR) and charge parity (CP[Formula: see text]) asymmetries of the [Formula: see text] and [Formula: see text] decay modes within QCDF approach. We find the [Formula: see text] and [Formula: see text]. We also find the values of CP asymmetries are [Formula: see text], [Formula: see text], [Formula: see text], [Formula: see text], [Formula: see text], and [Formula: see text]. The reported results are consistent with the recent theoretical predictions and can be used as a reference values in the forthcoming experiments.
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30

KHALIL, SHAABAN. "SUPERSYMMETRIC CONTRIBUTIONS TO THE CP ASYMMETRY OF THE B→ϕKS AND B→η'KS". Modern Physics Letters A 19, № 37 (2004): 2745–55. http://dx.doi.org/10.1142/s0217732304015907.

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We analyse the CP asymmetry of the B→ϕKS and B→η'KS processes in general supersymmetric models. We consider both gluino and chargino exchanges in a model-independent way by using the mass insertion approximation method. We adopt the QCD factorization method for evaluating the corresponding hadronic matrix elements. We show that chromomagnetic type of operator may play an important role in accounting for the deviation of the mixing CP asymmetry between B→ϕKS and B→J/ψKS processes observed by Belle and BaBar experiments. We also show that due to the different parity in the final states of these
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31

Cherniuk, Daria, Stanislav Abukhovich, Anh-Huy Phan, Ivan Oseledets, Andrzej Cichocki, and Julia Gusak. "Quantization Aware Factorization for Deep Neural Network Compression." Journal of Artificial Intelligence Research 81 (December 20, 2024): 973–88. https://doi.org/10.1613/jair.1.16167.

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Tensor decomposition of convolutional and fully-connected layers is an effective way to reduce parameters and FLOP in neural networks. Due to memory and power consumption limitations of mobile or embedded devices, the quantization step is usually necessary when pre-trained models are deployed. A conventional post-training quantization approach applied to networks with decomposed weights yields a drop in accuracy. This motivated us to develop an algorithm that finds tensor approximation directly with quantized factors and thus benefit from both compression techniques while keeping the predictio
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32

Qin, Qin, Hsiang-Nan Li, Cai-Dian Lü, and Fu-Sheng Yu. "Study on branching ratios and direct CP asymmetries of D → PV decays." International Journal of Modern Physics: Conference Series 29 (January 2014): 1460209. http://dx.doi.org/10.1142/s2010194514602099.

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We study the non-leptonic two-body decays of D mesons decaying into one pseudoscalar meson (P) and one vector meson (V) in the factorization-asisted topological-amplitude approach. In this approach, the decay amplitudes are factorized into two parts, the short-distance contribution (Wilson coefficients) and the long-distance contribution (hadronic matrix elements). We predict the branching ratios of D → PV decays using a global fit with the non-perturbative parameters. Our results agree well with the experimental data. We also predict the direct CP asymmetries by combining short-distance dynam
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33

Amirkhanlou, Elnaz, та Behnam Mohammadi. "The slope of the time-dependent asymmetry, Δ YK+K− and Δ Yπ+π−, in D 0 → K + K and D 0 → π + π decays". Physica Scripta 97, № 7 (2022): 075302. http://dx.doi.org/10.1088/1402-4896/ac758d.

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Abstract The most precise measurement of the the slope of the time-dependent asymmetry defined by the parameter Δ Y f ( f = K + K − , π + π − ), of the decay rates of D 0 and D ¯ 0 mesons into the final states in the decays D 0 → K + K − and D 0 → π + π − were recently reported by LHCb collaboration with the values of Δ Y K + K − = ( − 2.3 ± 1.5 ± 0.3 ) × 1 0 − 4 and Δ Y π + π − = ( − 4.0 ± 2.8 ± 0.4 ) × 1 0 − 4 . In this study, we have obtained Δ Y K + K − = ( − 2.27 ± 1.12 ) × 1 0 − 4 and Δ Y π + π − = ( − 3.15 ± 1.72 ) × 1 0 − 4 where Δ Y constrains possible CP violation. The CP violation i
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34

Loiseau, Benoît, Diogo Boito, Jean-Pierre Dedonder, et al. "Parametrizations of three-body hadronic B- and D-decay amplitudes." EPJ Web of Conferences 202 (2019): 06014. http://dx.doi.org/10.1051/epjconf/201920206014.

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A short review of our recent work on amplitude parametrizations of three-body hadronic weak B and D decays is presented. The final states are here composed of three light mesons, namely the various charge πππ, Kππ and KK$ \bar K $ states. These parametrizations are derived from previous calculations based on a quasi-two-body factorization approach where the two-body hadronic final state interactions are fully taken into account in terms of unitary S- and P-wave ππ, πK and K$ \bar K $ form factors. They are an alternative to the isobar-model description and can be useful in the interpretation o
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35

Yu, Yi, Xiang Chen, Shuai Cao, De Wu, Xu Zhang, and Xun Chen. "Gait synergetic neuromuscular control in children with cerebral palsy at different gross motor function classification system levels." Journal of Neurophysiology 121, no. 5 (2019): 1680–91. http://dx.doi.org/10.1152/jn.00580.2018.

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Cerebral palsy (CP) is a neural developmental disease featured with gait abnormalities. CP gait assessment is usually performed with the Gross Motor Function Classification System (GMFCS) in clinics, which does not involve a thorough assessment of neuromuscular control. To understand how the neuromuscular control disorders lead to gait abnormalities, we explored the relationship between GMFCS levels and the gait synergetic control characteristics in this study. In total, 18 children with CP at different GMFCS levels (mean age: 4.41±1.30 yr) and 8 age-matched typically developing (TD) children
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36

GUO, PENG, XIAO-GANG HE та XUE-QIAN LI. "DOES THE ΔI = 1/2 RULE HOLD IN D AND B→ππ DECAYS?" International Journal of Modern Physics A 21, № 01 (2006): 57–66. http://dx.doi.org/10.1142/s0217751x06025031.

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Although two pion decays of K, D and B have similar isospin structures, there are dramatic differences in the ratios RK and RD,B of amplitudes from ΔI = 3/2 and ΔI = 1/2 interactions. In K→ππ decays there is the famous ΔI = 1/2 rule with RK ≈ 1/22, whereas in B(D) → ππ decays the ratios RD,B are of order one and therefore there is no such a rule. In this work we study decay amplitudes in B(D)→ππ using QCD factorization calculations paying particular attention to discrepancies between data and theoretical estimates. Since isospin does not play a special role in factorization calculations, no ΔI
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37

Liao, Xiangwen, Lingying Zhang, Jingjing Wei, Dingda Yang, and Guolong Chen. "Recommending Mobile Microblog Users via a Tensor Factorization Based on User Cluster Approach." Wireless Communications and Mobile Computing 2018 (October 3, 2018): 1–11. http://dx.doi.org/10.1155/2018/9434239.

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User influence is a very important factor for microblog user recommendation in mobile social network. However, most existing user influence analysis works ignore user’s temporal features and fail to filter the marketing users with low influence, which limits the performance of recommendation methods. In this paper, a Tensor Factorization based User Cluster (TFUC) model is proposed. We firstly identify latent influential users by neural network clustering. Then, we construct a features tensor according to latent influential user’s opinion, activity, and network centrality information. Furthermo
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38

Dutta, Bhaskar, C. S. Kim, Sechul Oh та Guohuai Zhu. "CP asymmetries of B→ϕK and B→η(′)K decays using a global fit in QCD factorization". Physics Letters B 601, № 3-4 (2004): 144–50. http://dx.doi.org/10.1016/j.physletb.2004.09.045.

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SU, FANG, YUE-LIANG WU, YI-BO YANG та CI ZHUANG. "QCD FACTORIZATION BASED ON SIX-QUARK OPERATOR EFFECTIVE HAMILTONIAN FROM PERTURBATIVE QCD AND CHARMLESS BOTTOM MESON DECAYS B(s)→ππ, πK, KK". International Journal of Modern Physics A 25, № 01 (2010): 69–111. http://dx.doi.org/10.1142/s0217751x10048044.

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The charmless bottom meson decays are systematically investigated based on an approximate six-quark operator effective Hamiltonian from perturbative QCD. It is shown that within this framework the naive QCD factorization method provides a simple way to evaluate the hadronic matrix elements of two-body mesonic decays. The singularities caused by on mass-shell quark propagator and gluon exchanging interaction are appropriately treated. Such a simple framework allows us to make theoretical predictions for the decay amplitudes with reasonable input parameters. The resulting theoretical predictions
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40

Jin, Su-Ping, та Zhen-Jun Xiao. "Study of B s ⟶ ϕ ℓ + ℓ − Decays in the PQCD Factorization Approach with Lattice QCD Input". Advances in High Energy Physics 2021 (9 листопада 2021): 1–24. http://dx.doi.org/10.1155/2021/3840623.

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In this paper, we studied systematically the semileptonic decays B s ⟶ ϕ l + l − with l − = e − , μ − , τ − by using the perturbative QCD (PQCD) and the “PQCD+Lattice” factorization approach, respectively. We first evaluated all relevant form factors F i q 2 in the low- q 2 region using the PQCD approach, and we also took the available lattice QCD results at the high- q 2 region as additional input to improve the extrapolation of F i q 2 from the low- q 2 region to the endpoint q max 2 . We then calculated the branching ratios and many other physical observables A FB l , F L ϕ , S 3 , 4 , 7 ,
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Cappellini, Germana, Francesca Sylos-Labini, Michael J. MacLellan, et al. "Backward walking highlights gait asymmetries in children with cerebral palsy." Journal of Neurophysiology 119, no. 3 (2018): 1153–65. http://dx.doi.org/10.1152/jn.00679.2017.

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To investigate how early injuries to developing motor regions of the brain affect different forms of gait, we compared the spatiotemporal locomotor patterns during forward (FW) and backward (BW) walking in children with cerebral palsy (CP). Bilateral gait kinematics and EMG activity of 11 pairs of leg muscles were recorded in 14 children with CP (9 diplegic, 5 hemiplegic; 3.0–11.1 yr) and 14 typically developing (TD) children (3.3–11.8 yr). During BW, children with CP showed a significant increase of gait asymmetry in foot trajectory characteristics and limb intersegmental coordination. Furthe
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CHENG, HAI-YANG. "CHARMLESS 3-BODY B DECAYS: RESONANT AND NONRESONANT CONTRIBUTIONS." International Journal of Modern Physics A 23, no. 21 (2008): 3229–36. http://dx.doi.org/10.1142/s0217751x08041888.

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Charmless 3-body decays of B mesons are studied using a simple model based on the framework of the factorization approach. We have identified a large source of the nonresonant signal in the matrix elements of scalar densities, e.g. [Formula: see text]. This explains the dominance of the nonresonant background in B → KKK decays, the sizable nonresonant fraction of order (35 ~ 40)% in K−π+π− and [Formula: see text] modes and the smallness of nonresonant rates in B → πππ decays. We have computed the resonant and nonresonant contributions to charmless 3-body decays and determined the rates for the
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Zhong, Han, Geqi Qi, Wei Guan, and Xiaochen Hua. "Application of Nonnegative Tensor Factorization for Intercity Rail–Air Transport Supply Configuration Pattern Recognition." Sustainability 11, no. 6 (2019): 1803. http://dx.doi.org/10.3390/su11061803.

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With the rapid expansion of the railway represented by high-speed rail (HSR) in China, competition between railway and aviation will become increasingly common on a large scale. Beijing, Shanghai, and Guangzhou are the busiest cities and the hubs of railway and aviation transportation in China. Obtaining their supply configuration patterns can help identify defects in planning. To achieve that, supply level is proposed, which is a weighted supply traffic volume that takes population and distance factors into account. Then supply configuration can be expressed as the distribution of supply leve
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Raslan, E. H., and H. R. Khan. "Branching Ratio and CP Violation in $${B}_{{s}}^{{0}}\rightarrow{\rho}^{{0}}{\phi}$$ Decay in the Framework of QCD Factorization." Physics of Atomic Nuclei 83, no. 5 (2020): 746–54. http://dx.doi.org/10.1134/s106377882005018x.

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Jeang, John A., Danny Jomaa, Dana Novikov, et al. "CP-03. EXTRACELLULAR MATRIX REMODELING REVEALS NON-CELL AUTONOMOUS TUMOR FORMATION MECHANISM IN ADAMANTINOMATOUS CRANIOPHARYNGIOMAS." Neuro-Oncology 26, Supplement_4 (2024): 0. http://dx.doi.org/10.1093/neuonc/noae064.041.

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Abstract Adamantinomatous Craniopharyngioma (ACP) is a rare pituitary tumor of the sellar region, with a bimodal presentation pattern in children and middle-aged adults. ACPs are primarily driven by a mutation in CTNNB1 that prevents beta-catenin from degrading properly, resulting in accumulation in the nuclei of epithelial whorl-like structures sometimes referred to as cluster cells. Clinical management is challenging due to the location of the tumor, such that complete surgical resection is often not possible so radiation therapy, which can lead to high morbidity, is also used. Greater insig
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DATTA, ALAKABHA, and DAVID LONDON. "TRIPLE-PRODUCT CORRELATIONS IN B→V1V2 DECAYS AND NEW PHYSICS." International Journal of Modern Physics A 19, no. 15 (2004): 2505–44. http://dx.doi.org/10.1142/s0217751x04018300.

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In this paper we examine T-violating triple-product correlations (TP's) in B→V1V2 decays. TP's are excellent probes of physics beyond the standard model (SM) for two reasons: (i) within the SM, most TP's are expected to be tiny, and (ii) unlike direct CP asymmetries, TP's are not suppressed by the small strong phases which are expected in B decays. TP's are obtained via the angular analysis of B→V1V2. In a general analysis based on factorization, we demonstrate that the most promising decays for measuring TP's in the SM involve excited final-state vector mesons, and we provide estimates of suc
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Li, Yuanlin, M. M. Parmenter, and Pingzhi Yuan. "On *-clean group rings." Journal of Algebra and Its Applications 14, no. 01 (2014): 1550004. http://dx.doi.org/10.1142/s0219498815500048.

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A ring with involution * is called *-clean if each of its elements is the sum of a unit and a projection. Clearly a *-clean ring is clean. Vaš asked whether there exists a clean ring with involution * that is not *-clean. In a recent paper, Gao, Chen and the first author investigated when a group ring RG with classical involution * is *-clean and obtained necessary and sufficient conditions for RG to be *-clean, where R is a commutative local ring and G is one of C3, C4, S3 and Q8. As a consequence, the authors provided many examples of group rings which are clean, but not *-clean. In this pap
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Qi, Jing-Juan, Zhen-Yang Wang, Xin-Heng Guo, Xian-Wei Kang та Zhen-Hua Zhang. "Study of localized CP violation in B− → π−π+π− and the branching ratio of B− → σ(600)π− in the QCD factorization approach". Nuclear Physics B 948 (листопад 2019): 114788. http://dx.doi.org/10.1016/j.nuclphysb.2019.114788.

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Yamada, Shunji, Eisuke Chikayama, and Jun Kikuchi. "Signal Deconvolution and Generative Topographic Mapping Regression for Solid-State NMR of Multi-Component Materials." International Journal of Molecular Sciences 22, no. 3 (2021): 1086. http://dx.doi.org/10.3390/ijms22031086.

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Solid-state nuclear magnetic resonance (ssNMR) spectroscopy provides information on native structures and the dynamics for predicting and designing the physical properties of multi-component solid materials. However, such an analysis is difficult because of the broad and overlapping spectra of these materials. Therefore, signal deconvolution and prediction are great challenges for their ssNMR analysis. We examined signal deconvolution methods using a short-time Fourier transform (STFT) and a non-negative tensor/matrix factorization (NTF, NMF), and methods for predicting NMR signals and physica
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Wu, Jibing, Lianfei Yu, Qun Zhang, et al. "Multityped Community Discovery in Time-Evolving Heterogeneous Information Networks Based on Tensor Decomposition." Complexity 2018 (2018): 1–16. http://dx.doi.org/10.1155/2018/9653404.

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The heterogeneous information networks are omnipresent in real-world applications, which consist of multiple types of objects with various rich semantic meaningful links among them. Community discovery is an effective method to extract the hidden structures in networks. Usually, heterogeneous information networks are time-evolving, whose objects and links are dynamic and varying gradually. In such time-evolving heterogeneous information networks, community discovery is a challenging topic and quite more difficult than that in traditional static homogeneous information networks. In contrast to
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