... of the Weyl-squared term. We introduce the |
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Inflationary perturbations in no-scale theories Inflationary perturbations in no-scale theories Salvio, Alberto |
momentum 4.7 $$\begin{aligned} \pi ... |
... S Q We define $$\overline{M}$$ M ¯ as a new |
conjugate
Correspondence of phase transition points and singularities of thermodynamic geometry of black holes Correspondence of phase transition points and singularities of thermodynamic geometry of black holes Mansoori, Seyed Ali Hosseini; Mirza, Behrouz |
potential of $$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 ... |
... Gribov type, displaying unphysical complex |
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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. ... |
... 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 $$ p μ are the |
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Lagrangian for Frenkel electron and position’s non-commutativity due to spin Lagrangian for Frenkel electron and position’s non-commutativity due to spin Deriglazov, Alexei A.; Pupasov-Maksimov, Andrey M. |
momenta for $$\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)$$ ( X m , P m ) and the ... |
... the Hamiltonian that we will construct is |
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Chern–Simons theory with vector fermion matter Chern–Simons theory with vector fermion matter Giombi, Simone; Minwalla, Shiraz; Prakash, Shiroman; Trivedi, Sandip P.; Wadia, Spenta R.; Yin, Xi |
to this variable. ... |
... dependence in the action. As a result the |
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Hamiltonian formalism of bimetric gravity in vierbein formulation Hamiltonian formalism of bimetric gravity in vierbein formulation Klusoň, Josef |
momentum vanishes and is the primary ... |
... per unit mass. A new field $$\theta $$ θ , |
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New approach to nonrelativistic ideal magnetohydrodynamics New approach to nonrelativistic ideal magnetohydrodynamics Banerjee, Rabin; Kumar, Kuldeep |
to $$\rho $$ ρ , is introduced, taking the ... |
... a right-chiral fermion would be the complex |
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Number of fermion generations from a novel grand unified model Number of fermion generations from a novel grand unified model Byakti, Pritibhajan; Emmanuel-Costa, David; Mazumdar, Arindam; Pal, Palash B. |
of that of the left-chiral antifermion, and ... |