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Buchholz psi functions information


Buchholz's psi-functions are a hierarchy of single-argument ordinal functions introduced by German mathematician Wilfried Buchholz in 1986. These functions are a simplified version of the -functions, but nevertheless have the same strength[clarification needed] as those. Later on this approach was extended by Jäger[1] and Schütte.[2]

  1. ^ Jäger, G (1984). "ρ-inaccessible ordinals, collapsing functions and a recursive notation system". Archiv für Mathematische Logik und Grundlagenforschung. 24 (1): 49–62. doi:10.1007/BF02007140. S2CID 38619369.
  2. ^ Buchholz, W.; Schütte, K. (1983). "Ein Ordinalzahlensystem ftir die beweistheoretische Abgrenzung der H~-Separation und Bar-Induktion". Sitzungsberichte der Bayerischen Akademie der Wissenschaften, Math.-Naturw. Klasse.

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Buchholz psi functions

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Buchholz's psi-functions are a hierarchy of single-argument ordinal functions ψ ν ( α ) {\displaystyle \psi _{\nu }(\alpha )} introduced by German mathematician...

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Buchholz

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Buchholz (surname) Buchholz hydra, a mathematical game on a labeled tree Buchholz psi functions, a system of ordinal collapsing functions Buchholz's ID...

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Buchholz hydra

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proof. Here, ψ 0 {\displaystyle \psi _{0}}  denotes Buchholz's function, and ψ 0 ( ε Ω ω + 1 ) {\displaystyle \psi _{0}(\varepsilon _{\Omega _{\omega...

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Ordinal collapsing function

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of infinity (KP). Buchholz's ψ {\displaystyle \psi }  is a hierarchy of single-argument functions ψ ν : O n → O n {\displaystyle \psi _{\nu }:{\mathsf...

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Ordinal notation

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Feferman. Feferman introduced theta functions, described in Buchholz (1986) as follows. For an ordinal α, θα is a function mapping ordinals to ordinals. Often...

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Large countable ordinal

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1 ) {\displaystyle \psi _{0}(\varepsilon _{\Omega _{\omega }+1})} . It is the supremum of the range of Buchholz's psi functions. It was first named by...

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Hydra game

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"Rapidly Growing Ramsey Functions". Annals of Mathematics. 113 (2): 267–314. doi:10.2307/2006985. ISSN 0003-486X. JSTOR 2006985. Buchholz, Wilfried (1984-11-27)...

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Feynman diagram

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{\psi }}M\psi +{\bar {\eta }}\psi +{\bar {\psi }}\eta }\,D{\bar {\psi }}\,D\psi =\int e^{\left({\bar {\psi }}+{\bar {\eta }}M^{-1}\right)M\left(\psi +M^{-1}\eta...

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Second quantization

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_{1}\psi _{2}+\psi _{1}\psi _{2}\psi _{1})+{\frac {1}{\sqrt {3}}}(\psi _{1}\psi _{2}\psi _{1}+\psi _{2}\psi _{1}\psi _{1}+\psi _{2}\psi _{1}\psi _{1})\right)\\=&{\frac...

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Ordinal analysis

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ψ ( ε Ω + 1 ) {\displaystyle \psi (\varepsilon _{\Omega +1})} in Madore's ψ. 4.^ Uses Madore's ψ rather than Buchholz's ψ. 5.^ Can also be commonly written...

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Quantum field theory

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\end{aligned}}} Since interacting correlation functions can be expressed in terms of free correlation functions, only the latter need to be evaluated in order...

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Gauge fixing

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gauge functions which satisfy the wave equation ∂ 2 ψ ∂ t 2 = c 2 ∇ 2 ψ {\displaystyle {\frac {\partial ^{2}\psi }{\partial t^{2}}}=c^{2}\nabla ^{2}\psi }...

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Relativistic wave equations

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to the equations, universally denoted as ψ or Ψ (Greek psi), are referred to as "wave functions" in the context of RQM, and "fields" in the context of...

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Small Veblen ordinal

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{\displaystyle \psi (\Omega ^{\Omega ^{\omega }})} is the limit of ordinals that can be described using a version of Veblen functions with finitely many...

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Canonical quantization

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on functions f in classical phase space, then the following properties are usually considered desirable: Q x ψ = x ψ {\displaystyle Q_{x}\psi =x\psi }...

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Propagator

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often called (causal) Green's functions (called "causal" to distinguish it from the elliptic Laplacian Green's function). In non-relativistic quantum...

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Wightman axioms

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2 ‖ Φ ‖ 2 {\displaystyle P{\big (}[\Psi ],[\Phi ]{\big )}={\frac {|\langle \Psi ,\Phi \rangle |^{2}}{\lVert \Psi \rVert ^{2}\lVert \Phi \rVert ^{2}}}}...

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Path integral formulation

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0 ) = x x ( t ) = y e i S D x , {\displaystyle \psi _{t}(y)=\int \psi _{0}(x)K(x-y;t)\,dx=\int \psi _{0}(x)\int _{x(0)=x}^{x(t)=y}e^{iS}\,{\mathcal {D}}x...

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Quantum electrodynamics

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}F^{\mu \nu }+i{\bar {\psi }}\gamma ^{\mu }\partial _{\mu }\psi -e{\bar {\psi }}\gamma ^{\mu }A_{\mu }\psi -m{\bar {\psi }}\psi } = − 1 4 F μ ν F μ ν +...

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Gauge theory

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{\displaystyle {\mathcal {S}}=\int {\bar {\psi }}\left(i\hbar c\,\gamma ^{\mu }\partial _{\mu }-mc^{2}\right)\psi \,\mathrm {d} ^{4}x} The global symmetry...

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Renormalization

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{\psi }}m\psi \right)_{B}=Z_{0}{\bar {\psi }}m\psi } ( ψ ¯ ( ∂ μ + i e A μ ) ψ ) B = Z 1 ψ ¯ ( ∂ μ + i e A μ ) ψ {\displaystyle \left({\bar {\psi }}\left(\partial...

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Infraparticle

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ψ ( x → ) {\displaystyle \delta \psi ({\vec {x}})=iq\alpha ({\vec {x}})\psi ({\vec {x}})} where α is some function of position? The Noether charge is...

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Coupling constant

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4 μ 0 F μ ν F μ ν {\displaystyle T={\bar {\psi }}(i\hbar c\gamma ^{\sigma }\partial _{\sigma }-mc^{2})\psi -{1 \over 4\mu _{0}}F_{\mu \nu }F^{\mu \nu...

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