Quantum Field Theory on NC Curved Spacetimes
Quantum Field Theory on NC Curved Spacetimes
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