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Quantum Field Theory on NC Curved Spacetimes

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Scalar field <strong>on</strong> <strong>NC</strong> CS Deformed Green’s operators<br />

◮ (M, g⋆, ⋆) λ=0 time-oriented, c<strong>on</strong>nected, globally hyperbolic<br />

◮ deformed Klein-Gord<strong>on</strong> operator P⋆ = ∞<br />

λ<br />

n=0<br />

nP (n)<br />

◮ technical assumpti<strong>on</strong>: P (n) : C∞ (M) → C∞ 0<br />

◮ fulfilled for all twists of compact support<br />

(M) for all n > 0<br />

◮ or g⋆ asymptotically (outside compact regi<strong>on</strong>) symmetric under F<br />

◮ based <strong>on</strong> str<strong>on</strong>g results for the commutative case we find:<br />

there exist unique deformed Green’s operators ∆⋆± := ∞<br />

λ<br />

n=0<br />

n∆ (n)±<br />

∆⋆± = ∆± − λ ∆± ◦ P(1) ◦ ∆±<br />

− λ 2 <br />

3<br />

∆± ◦ P(2) ◦ ∆± − ∆± ◦ P(1) ◦ ∆± ◦ P(1) ◦ ∆± + O(λ )<br />

= − λ 1 − λ 2<br />

[higher orders in λ follow the same structure]<br />

<br />

2 − 1 1<br />

<br />

+ O(λ 3 )<br />

A. Schenkel (Würzburg) QFT <strong>on</strong> <strong>NC</strong> CS DESY 2010 5 / 9

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