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Peter H. Tsang

Publications and source records attributed to Peter H. Tsang.

7 recordsLinked to original sources

Wave-Tide Locking in Thin Stellar Streams: A Phenomenological Mass Spectrometer for an Intermediate Ultralight Axion

We propose a phenomenological mass estimator for an intermediate ultralight axion dark-matter component using thin stellar streams. The central observation is an analytic relation linking three length scales in a fuzzy-dark-matter stream progenitor: the tidal radius of a bound dark core, its gravitational Bohr radius, and the axion de Broglie wavelength evaluated at the stripped-star velocity scale. If the stream width is (w=C_w r_{\rm t}), with (C_w=O(1)), then [ \frac{r_{\rm t}}{r_{\rm B}} =========================== \frac{4π^2}{C_w^2} \left(\frac{w}{λ_{\rm dB}}\right)^2 . ] Thus (λ_{\rm dB}\sim w) automatically implies (r_{\rm t}/r_{\rm B}\sim25)--(40): the dark wave core survives well inside the tidal boundary while the extended stellar envelope is stripped into a thin stream. This wave--tide locking gives a no-simulation axion-mass estimator, [ m_a \simeq 2.69\times10^{-19},{\rm eV} \left(\frac{\sqrt{2}}{q_κ}\right) \left(\frac{R}{10,{\rm kpc}}\right) \left(\frac{38,{\rm pc}}{w}\right)^2 \left(\frac{w}{\ell_{\rm ripple}}\right) \left(\frac{220,{\rm km,s^{-1}}}{v_c}\right). ] In the simplest locked case (\ell_{\rm ripple}\sim w), a homogeneous first-pass set of narrow stream widths points to (m_a) of a few (10^{-19},{\rm eV}) and hidden-core masses of a few (10^3)--(10^4M_\odot). This is not a detection claim; it is a falsifiable phenomenological test for an ultralight axion component that can be sharpened by homogeneous stream catalogs and Schrödinger--Poisson simulations.

hep-ph

On the QCD Axion Potential in Fried's QCD Functional Formalism

We examine the QCD axion potential in Fried's nonperturbative QCD functional formalism. The axion is introduced in the standard way through (Θ=θ_{\rm QCD}+a/f_a). The question addressed is how the resulting (Θ)-dependence of the QCD vacuum energy is represented after the effective-locality reduction of the gluonic degrees of freedom. The construction is organized around two nonperturbative quantities: the Fried chiral condensate (Σ_{\rm F}=-\langle\bar q q\rangle_{\rm F}), generated by the scalar/pseudoscalar projection of the effective-locality kernel, and the pure-glue topological stiffness (A_{\rm F}=χ_{\rm YM}^{\rm F}), represented in the Halpern formulation by a CP-odd self-dual/anti-self-dual curvature. Under these assumptions, [ χ_{\rm top}^{\rm F} ====================== \left[ A_{\rm F}^{-1} + \sum_f (m_fΣ_{\rm F})^{-1} \right]^{-1}, \qquad m_a^2f_a^2=χ_{\rm top}^{\rm F}. ] This expression has the expected heavy-quark, light-quark, and massless-quark limits. In a separable scalar/pseudoscalar approximation, (Σ_{\rm F}=N_crΛ_{\rm EL}^3 I(r)/(4π^2)), with (r=M_0/Λ_{\rm EL}) fixed by (1=α_χ^{\rm F}J(r)). The result is conditional: a complete first-principles derivation requires computing (Σ_{\rm F}) and (A_{\rm F}) from the full Fried--Gabellini--Grandou--Tsang--Sheu measure. We also note that the Fried-QCD contribution to a multi-axion mass matrix is rank one; additional massive axion-like species require additional independent topological sectors.

hep-ph

Effective locality and chiral symmetry breaking in QCD

A few years ago the use of standard functional manipulations was demonstrated to imply an unexpected property satisfied by the fermionic Green's functions of QCD, and called effective locality. This feature of QCD is non-perturbative as it results from a full integration of the gluonic degrees of freedom. In this paper, at eikonal and quenching approximation at least, the relation of effective locality to dynamical chiral symmetry breaking is examined.

hep-th

Schwinger Generating Functional Derivation of LHC Elastic Proton-Proton Scattering Amplitudes

A recent Schwinger Generating Functional based formulation, by H.M.Fried,Y.Gabellini,T.Grandou and Y-M.Sheu and P.H.Tsang provided gauge-invariant, exact, non-perturbative solutions for QCD. After choosing a renormalization scheme and assuming a simpler 2 body quark-quark scattering problem, this formalism is tested against experimental elastic proton-proton scattering at LHC energies (7, 8, 13 TeV). This formulation was previously compared with ISR energies at (23.5 - 62.5 GeV). The full scattering amplitude with infinite gluons summed, infinite loops summed and their interference terms are needed for LHC differential cross-sections.

hep-ph

Chiral Symmetry Breaking out of QCD Effective Locality

The QCD non-perturbative property of Effective Locality whose essential meaning has been disclosed recently, is here questioned about the chiral symmetry breaking phenomenon, one of the two major issues of the non-perturbative phase of QCD. As a first attempt, quenching and the eikonal approximation are used so as to simplify calculations which are quite involved. Chiral symmetry breaking appears to be realised in close connection to the Effective Locality mass scale, $μ^2$ , as could be expected.

hep-th

Comparison of Gluon Bundle based QCD Curves with ISR Elastic pp Scattering Data

Using previously described functional techniques for exact, non-perturbative, gauge-invariant renormalized QCD processes, a simplified version of the amplitudes - in which forms akin to Pomerons naturally appear - provides fits to ISR Elastic pp scattering data. Extension of this work to LHC reactions is presently underway.

hep-ph