Existence and profile covariance of the modified scalar scattering matrix and interacting fields

Let η\boldsymbol{\eta} be a profile, let CFC\in\mathcal{F} be a polynomial in fields and their derivatives, and let Ψ,ΨD2\Psi,\Psi'\in\mathcal{D}_2. A renormalization scheme for time-ordered products is sought such that the adiabatic limits defining Smod(η)S_{\mathrm{mod}}(\eta) and Cret/adv,mod(η;x)C_{\mathrm{ret}/\mathrm{adv},\mathrm{mod}}(\eta;x) exist in the stated formal distributional spaces. Existence and covariance conjecture. There exists such a renormalization scheme for which

(ΨSmod(η)Ψ):=limϵ0(ΨSmod(η,gϵ)Ψ)(\Psi|S_{\mathrm{mod}}(\eta)\Psi'):=\lim_{\epsilon\searrow0}(\Psi|S_{\mathrm{mod}}(\eta,g_\epsilon)\Psi')

exists in Ce\mathbb{C}\llbracket e\rrbracket and defines Smod(η)L(D2,D2)eS_{\mathrm{mod}}(\eta)\in L(\mathcal{D}_2,\mathcal{D}_2^*)\llbracket e\rrbracket, while the corresponding limits for every hS(R4)h\in\mathcal{S}(\mathbb{R}^4) exist in S(R4)e\mathcal{S}'(\mathbb{R}^4)\llbracket e\rrbracket and define Cret/adv,mod(η;x)S(R4,L(D2,D2))eC_{\mathrm{ret}/\mathrm{adv},\mathrm{mod}}(\eta;x)\in\mathcal{S}'(\mathbb{R}^4,L(\mathcal{D}_2,\mathcal{D}_2^*))\llbracket e\rrbracket. For any two profiles η,η\eta,\eta', these objects satisfy

Smod(η)=Vout(η,η)Smod(η)Vin(η,η),S_{\mathrm{mod}}(\eta')=V_{\mathrm{out}}(\eta',\eta)S_{\mathrm{mod}}(\eta)V_{\mathrm{in}}(\eta,\eta'),

and

Cret/adv,mod(η;x)=Vin/out(η,η)Cret/adv,mod(η;x)Vin/out(η,η).C_{\mathrm{ret}/\mathrm{adv},\mathrm{mod}}(\eta';x)=V_{\mathrm{in}/\mathrm{out}}(\eta',\eta)C_{\mathrm{ret}/\mathrm{adv},\mathrm{mod}}(\eta;x)V_{\mathrm{in}/\mathrm{out}}(\eta,\eta').

This is presented as the desired construction of the modified scattering matrix and interacting fields in the scalar model; the supplied text gives no evidence that the assertion has been proved or disproved.

Sources & referencesView supporting material

Primary source

Paweł Duch, “Infrared problem in perturbative quantum field theory”, arXiv:1906.00940 (2021).

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