... Similarly, the decay amplitudes of the CP- |
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Isospin analysis of charmless B-meson decays Isospin analysis of charmless B-meson decays Charles, J.; Deschamps, O.; Descotes-Genon, S.; Niess, V. |
isodoublet ( $$\bar{B}^0$$ B ¯ 0 , $$B^-$$ ... |
... of the Weyl-squared term. We introduce the |
conjugate
Inflationary perturbations in no-scale theories Inflationary perturbations in no-scale theories Salvio, Alberto |
momentum 4.7 $$\begin{aligned} \pi ... |
... Gribov type, displaying unphysical complex |
conjugate
A study of the Higgs and confining phases in Euclidean SU(2) Yang–Mills theories in 3d by taking into account the Gribov horizon A study of the Higgs and confining phases in Euclidean SU(2) Yang–Mills theories in 3d by taking into account the Gribov horizon Capri, M. A. L.; Dudal, D.; Gómez, A. J.; Guimaraes, M. S.; Justo, I. F.; Sorella, S. P. |
poles. ... |
... A ¯ ( DP ) = ∑ i A i ¯ F i ¯ ( DP ) for CP- |
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Disentangling weak and strong interactions in $$B\rightarrow K^{*}(\rightarrow K\pi )\pi $$$B\to {K}^{\ast}(\to K\mathit{\pi})\mathit{\pi}$ Dalitz-plot analyses Disentangling weak and strong interactions in $$B\rightarrow K^{*}(\rightarrow K\pi )\pi $$$B\to {K}^{\ast}(\to K\mathit{\pi})\mathit{\pi}$ Dalitz-plot analyses Charles, Jérôme; Descotes-Genon, Sébastien; Ocariz, José; Pérez Pérez, Alejandro; For the CKMfitter Group |
amplitudes. ... |
... S Q We define $$\overline{M}$$ M ¯ as a new |
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Correspondence of phase transition points and singularities of thermodynamic geometry of black holes Correspondence of phase transition points and singularities of thermodynamic geometry of black holes Mansoori, Seyed Ali Hosseini; Mirza, Behrouz |
potential of $$M(S,Q)$$ M ( S , Q ) in ... |
... by one parton in the amplitude and complex |
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Hard four-jet production in pA collisions Hard four-jet production in pA collisions Blok, B.; Strikman, M.; Wiedemann, U. A. |
amplitude and it is ... |
... of these q a(j) up to j=l−1 will have a |
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Realisation of a Lorentz algebra in Lorentz violating theory Realisation of a Lorentz algebra in Lorentz violating theory Ganguly, Oindrila |
momentum p a(j). ... |
... the continuum Lagrangian coordinate and |
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Hamiltonian approach to GR – Part 2: covariant theory of quantum gravity Hamiltonian approach to GR – Part 2: covariant theory of quantum gravity Cremaschini, Claudio; Tessarotto, Massimo |
canonical momentum, both realized by means ... |
... of the screening gluon in the complex |
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Generation of central exclusive final states Generation of central exclusive final states Lönnblad, Leif; Žlebčík, Radek |
amplitude. ... |
... measure the value of associated canonically |
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Bell violation in the sky Bell violation in the sky Choudhury, Sayantan; Panda, Sudhakar; Singh, Rajeev |
momentum. ... |
... [39] and its components is the complex |
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Graphical calculus of volume, inverse volume and Hamiltonian operators in loop quantum gravity Graphical calculus of volume, inverse volume and Hamiltonian operators in loop quantum gravity Yang, Jinsong; Ma, Yongge |
of (generalized) Clebsch–Gordan ... |
... a → U H ( Q ¯ ) a S Q ¯ † . Their hermitian |
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Quarkonium Contribution to Meson Molecules Quarkonium Contribution to Meson Molecules Cincioglu, E.; Nieves, J.; Ozpineci, A.; Yilmazer, A. U. |
fields are defined by 7 $$\begin{aligned} ... |
... that includes the coupling strength and its |
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Thermodynamics of Horndeski black holes with non-minimal derivative coupling Thermodynamics of Horndeski black holes with non-minimal derivative coupling Miao, Yan-Gang; Xu, Zhen-Ming |
. ... |
... interpretation, as it exhibits complex |
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SU(2)×U(1) Yang–Mills theories in 3d with Higgs field and Gribov ambiguity SU(2)×U(1) Yang–Mills theories in 3d with Higgs field and Gribov ambiguity Capri, M. A. L.; Dudal, D.; Guimaraes, M. S.; Justo, I. F.; Sorella, S. P.; Vercauteren, D. |
poles. ... |
... ^\mu $$ π μ and $$p^\mu $$ p μ are the |
conjugate
Lagrangian for Frenkel electron and position’s non-commutativity due to spin Lagrangian for Frenkel electron and position’s non-commutativity due to spin Deriglazov, Alexei A.; Pupasov-Maksimov, Andrey M. |
momenta for $$\omega ^\mu $$ ω μ and the ... |
... the equations 83 84 85 Φ 1 is thus a self- |
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Projection operator approach to the quantization of higher spin fields Projection operator approach to the quantization of higher spin fields Tóth, Gábor Zsolt |
field, whereas Φ 2 is anti-self- ... |
... then 10 where π ij and π Φ are the momenta |
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Hamiltonian dynamics and Noether symmetries in Extended Gravity Cosmology Hamiltonian dynamics and Noether symmetries in Extended Gravity Cosmology Capozziello, S.; Laurentis, M.; Odintsov, S. D. |
to h ij and Φ, respectively. ... |
... effective thermodynamic volume which is the |
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Charged de Sitter-like black holes: quintessence-dependent enthalpy and new extreme solutions Charged de Sitter-like black holes: quintessence-dependent enthalpy and new extreme solutions Azreg-Aïnou, Mustapha |
variable of the negative quintessential ... |
... $$\bar{\kappa }$$ κ ¯ will be the complex |
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On the six-dimensional Kerr theorem and twistor equation On the six-dimensional Kerr theorem and twistor equation Carneiro da Cunha, Bruno |
of each other if we want the null vector to ... |
... fermions, one can check that the canonical |
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Myers–Pospelov model as an ensemble of Pais–Uhlenbeck oscillators: unitarity and Lorentz invariance violation Myers–Pospelov model as an ensemble of Pais–Uhlenbeck oscillators: unitarity and Lorentz invariance violation Lopez-Sarrion, Justo; Reyes, Carlos M. |
momentum for ψ + is $i \psi_{+}^{\dag}$ , ... |
... $$ Λ as a thermodynamic pressure and its |
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Maxwell’s equal-area law for Gauss–Bonnet–Anti-de Sitter black holes Maxwell’s equal-area law for Gauss–Bonnet–Anti-de Sitter black holes Belhaj, A.; Chabab, M.; El moumni, H.; Masmar, K.; Sedra, M. B. |
quantity as a thermodynamic volume, we ... |
... ( ≡ Π 1 a T a ) are the momenta canonically |
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Hamiltonian, path integral and BRST formulations of large $$N$$$N$ scalar QCD$$_{2}$$${}_{2}$ on the light-front and spontaneous symmetry breaking Hamiltonian, path integral and BRST formulations of large $$N$$$N$ scalar QCD$$_{2}$$${}_{2}$ on the light-front and spontaneous symmetry breaking Kulshreshtha, Usha; Kulshreshtha, Daya Shankar; Vary, James P. |
, respectively, to $$\phi , \phi ^{\dagger ... |
... constraints. The world-sheet fields are the |
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Ambitwistor superstring in the Green–Schwarz formulation Ambitwistor superstring in the Green–Schwarz formulation Chandía, Osvaldo; Vallilo, Brenno Carlini |
pairs $$(X^m, P_m)$$ ( X m , P m ) and the ... |
... the Hamiltonian that we will construct is |
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Chern–Simons theory with vector fermion matter Chern–Simons theory with vector fermion matter Giombi, Simone; Minwalla, Shiraz; Prakash, Shiroman; Trivedi, Sandip P.; Wadia, Spenta R.; Yin, Xi |
to this variable. ... |
... dependence in the action. As a result the |
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Hamiltonian formalism of bimetric gravity in vierbein formulation Hamiltonian formalism of bimetric gravity in vierbein formulation Klusoň, Josef |
momentum vanishes and is the primary ... |