query: OPE of stress tensor in CFT
positive_passages.docid: 151454
positive_passages.text: Weyl anomaly in 2d CFT (string theory lectures by D.Tong)
negative_passages.docid: 95981
negative_passages.text: Gravity in 2d space and inverse linear law
negative_passages.docid: 148263
negative_passages.text: Interacting Fields in QFT
negative_passages.docid: 258
negative_passages.text: Existence of orthogonal coordinates on a Riemannian manifold
negative_passages.docid: 39094
negative_passages.text: Lie bracket of vector fields on $\Bbb R^{n}$
negative_passages.docid: 74566
negative_passages.text: Electromagnetic Tensor in Cylindrical Coordinates
negative_passages.docid: 130830
negative_passages.text: Counting degrees of freedom for gravitational waves as a gauge field
negative_passages.docid: 30669
negative_passages.text: Introduction to string theory
negative_passages.docid: 106047
negative_passages.text: Does every element of tensor product look like this?
negative_passages.docid: 58435
negative_passages.text: Condition for a tensor to be decomposable
negative_passages.docid: 87750
negative_passages.text: Hom / tensor adjunction for $O_X$ modules?
negative_passages.docid: 79914
negative_passages.text: Hom and tensor with a flat module
negative_passages.docid: 111559
negative_passages.text: How to get space component of weak field (linearized) metric?
negative_passages.docid: 11773
negative_passages.text: Levi-Civita connection between conformal metrics
negative_passages.docid: 80596
negative_passages.text: Ambiguities in the energy-momentum tensor
negative_passages.docid: 25195
negative_passages.text: $2 \otimes_{R} 2 + x \otimes_{R} x$ is not a simple tensor in $I \otimes_R I$
negative_passages.docid: 38412
negative_passages.text: Basis for tensor products