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Flux quantization on 11-dimensional superspace
Flux quantization of the C-field in 11d supergravity is arguably necessary for the (UV-)completion of the theory, in that it determines the torsion...
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An inequality for entangled qutrits in SU(3) basis
It is well known from the representation theory of particle physics that the tensor product of two fundamental representation of SU(2) and SU(3)...
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Hardware efficient decomposition of the Laplace operator and its application to the Helmholtz and the Poisson equation on quantum computer
With the rapid advancement of quantum computers in the past few years, there is ongoing development of algorithms aimed at solving problems that are...
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Quantum related-key differential cryptanalysis
Quantum computation models have profoundly impacted cryptanalysis. Differential cryptanalysis is one of the most fundamental methods in cryptanalysis...
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A string theory for two dimensional Yang-Mills theory. Part I
Two dimensional gauge theories with charged matter fields are useful toy models for studying gauge theory dynamics, and in particular for studying...
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Soft algebras for leaf amplitudes
Celestial MHV amplitudes are comprised of non-distributional leaf amplitudes associated to an AdS 3 leaf of a foliation of flat spacetime. It is shown...
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Quantum Harmonic Oscillator in a Time Dependent Noncommutative Background
This work explores the behaviour of a noncommutative harmonic oscillator in a time-dependent background, as previously investigated in Dey and Fring...
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Fermi gas formalism for D-type quiver Chern-Simons theory with non-uniform ranks
We construct the Fermi gas formalism for the partition function of supersymmetric Chern-Simons theories with affine D -type quiver diagrams with...
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The 1 → 3 massive splitting functions from QCD factorization and SCET
Splitting functions are universal functions describing the collinear dynamics of gauge theories, and as such are crucial ingredients for a wide...
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Hadamard products and BPS networks
We study examples of fourth-order Picard-Fuchs operators that are Hadamard products of two second-order Picard-Fuchs operators. Each second-order...
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A semi-analytical x-space solution for parton evolution — Application to non-singlet and singlet DGLAP equation
We present a novel semi-analytical method for parton evolution. It is based on constructing a family of analytic functions spanning x -space which is...
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An improved framework for computing waveforms
We combine the observable-based formalism (KMOC), the analytic properties of the scattering amplitude, generalised unitarity and the heavy-mass...
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Two-loop integrals for \( t\overline{t} \)+jet production at hadron colliders in the leading colour approximation
We compute the differential equations for the two remaining integral topologies contributing to the leading colour two-loop amplitudes for pp →
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A meta-trained generator for quantum architecture search
Variational Quantum Algorithms (VQAs) have made great success in the Noisy Intermediate-Scale Quantum (NISQ) era due to their relative resilience to...
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A description of χcJ → VV decays within the effective field theory framework
We study χ cJ → VV decays using the QCD effective field theory approach. The helicity suppressed decay amplitudes are also considered. The...
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Erratum to: An explicit expression of generating function for one-loop tensor reduction
A correction to this paper has been published: https://doi.org/10.1007/JHEP02(2024)158
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The NNLO soft function for N-jettiness in hadronic collisions
We compute the N-jettiness soft function in hadronic collisions to next-to-next-to-leading order (NNLO) in the strong-coupling expansion. Our...
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Multiparton Cwebs at five loops
Scattering amplitudes involving multiple partons are plagued with infrared singularities. The soft singularities of the amplitude are captured by the...
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Entanglement islands and cutoff branes from path-integral optimization
Recently it was proposed that, the AdS/BCFT correspondence can be simulated by a holographic Weyl transformed CFT 2 , where the cut-off brane plays the...