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Physlib.QFT.PerturbationTheory.WickContraction.SubContraction

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definition

Sub-contraction of φsΛ\varphi s\Lambda defined by SφsΛ.1S \subseteq \varphi s\Lambda.1

#subContraction

Let φs\varphi s be a sequence of field operators and φsΛ\varphi s\Lambda be a Wick contraction on φs\varphi s. Given a subset SS of the set of contracted pairs φsΛ.1\varphi s\Lambda.1, the sub-contraction is the Wick contraction on the same sequence φs\varphi s whose set of contracted pairs is exactly SS.

theorem

aΛS    aΛa \in \Lambda|_S \implies a \in \Lambda

#mem_of_mem_subContraction

Let φs\varphi s be a sequence of field operators. Let Λ\Lambda be a Wick contraction on φs\varphi s, and let Λ.1\Lambda.1 denote the set of its contracted pairs (where each pair is represented as a set of indices). For any subset of pairs SΛ.1S \subseteq \Lambda.1, let ΛS\Lambda|_S be the sub-contraction formed by the pairs in SS. If a set of indices aa is a contracted pair in the sub-contraction ΛS\Lambda|_S, then aa is also a contracted pair in the original contraction Λ\Lambda.

definition

Quotient contraction of φsΛ\varphi s\Lambda by SφsΛ.1S \subseteq \varphi s\Lambda.1

#quotContraction

Let φs\varphi s be a sequence of field operators and Λ\Lambda be a Wick contraction on φs\varphi s. Given a subset SΛS \subseteq \Lambda of the contracted pairs, the quotient contraction is the Wick contraction defined on the sequence of operators [ΛS]uc[\Lambda|_S]^{uc} that remain after the contractions in SS have been performed. This contraction consists of all pairs in Λ\Lambda that are not in SS, with their indices relabeled to correspond to their positions in the uncontracted list.

theorem

aquotContraction(S)    uncontractedListEmd(a)Λa \in \text{quotContraction}(S) \implies \text{uncontractedListEmd}(a) \in \Lambda

#mem_of_mem_quotContraction

Let φs\varphi s be a sequence of field operators and Λ\Lambda be a Wick contraction on φs\varphi s, where Λ.1\Lambda.1 denotes the set of contracted pairs. Let SΛ.1S \subseteq \Lambda.1 be a subset of these pairs. The quotient contraction of Λ\Lambda by SS is a Wick contraction defined on the sequence of operators that remain uncontracted after the pairs in SS are removed. If aa is a contracted pair in this quotient contraction, then the set of indices obtained by mapping aa back to the original sequence using the embedding uncontractedListEmd\text{uncontractedListEmd} is a contracted pair in the original contraction Λ\Lambda. In mathematical notation, if a(quotContraction S).1a \in (\text{quotContraction } S).1, then {uncontractedListEmd(i)ia}Λ.1\{\text{uncontractedListEmd}(i) \mid i \in a\} \in \Lambda.1.

theorem

Every contracted pair aΛa \in \Lambda belongs to either the sub-contraction SS or the quotient contraction Λ/S\Lambda/S

#mem_subContraction_or_quotContraction

Let φs\varphi s be a sequence of field operators and Λ\Lambda be a Wick contraction on φs\varphi s. Given a subset SΛS \subseteq \Lambda of the contracted pairs, any contracted pair aΛa \in \Lambda either belongs to the sub-contraction defined by SS, or it corresponds to a pair in the quotient contraction of Λ\Lambda by SS. Specifically, if aΛa \in \Lambda, then: aSa,map(uncontractedListEmd,a)=a and aquotContraction(S) a \in S \lor \exists a', \text{map}(\text{uncontractedListEmd}, a') = a \text{ and } a' \in \text{quotContraction}(S) where uncontractedListEmd\text{uncontractedListEmd} is the embedding that maps the indices of the operators remaining after the contractions in SS back to their original indices in the sequence φs\varphi s.

theorem

The aa-th uncontracted field of a sub-contraction is the field φs[uncontractedListEmd(a)]\varphi s[\text{uncontractedListEmd}(a)]

#subContraction_uncontractedList_get

Let φs\varphi s be a sequence of field operators and Λ\Lambda be a Wick contraction on φs\varphi s. Let SΛ.1S \subseteq \Lambda.1 be a subset of the contracted pairs of Λ\Lambda, which defines a sub-contraction. For any index aa into the list of operators remaining uncontracted after this sub-contraction (denoted as [subContraction(S)]uc[\text{subContraction}(S)]^{uc}), the operator at that position is equal to the operator in the original sequence φs\varphi s at the index uncontractedListEmd(a)\text{uncontractedListEmd}(a), where uncontractedListEmd\text{uncontractedListEmd} is the embedding from the indices of the uncontracted list back to the indices of the original sequence. In formula terms: [subContraction(S)]auc=φsuncontractedListEmd(a) [\text{subContraction}(S)]^{uc}_a = \varphi s_{\text{uncontractedListEmd}(a)}

theorem

The first field of a pair in a sub-contraction ΛS\Lambda|_S is the same as in the original contraction Λ\Lambda

#subContraction_fstFieldOfContract

Let φs\varphi s be a sequence of field operators and Λ\Lambda be a Wick contraction on φs\varphi s. Let SΛ.1S \subseteq \Lambda.1 be a subset of the contracted pairs of Λ\Lambda, defining a sub-contraction ΛS\Lambda|_S. For any pair aa in the set of contracted pairs of the sub-contraction, the first field operator of the pair aa in ΛS\Lambda|_S is equal to the first field operator of aa in the original contraction Λ\Lambda. In formula terms: (ΛS).fstFieldOfContract(a)=Λ.fstFieldOfContract(a) (\Lambda|_S).\text{fstFieldOfContract}(a) = \Lambda.\text{fstFieldOfContract}(a) where fstFieldOfContract\text{fstFieldOfContract} identifies the first operator (typically the one with the smaller index) in a contracted pair.

theorem

The second field of a pair in a sub-contraction ΛS\Lambda|_S is the same as in the original contraction Λ\Lambda

#subContraction_sndFieldOfContract

Let φs\varphi s be a sequence of field operators and Λ\Lambda be a Wick contraction on φs\varphi s. Let SΛ.1S \subseteq \Lambda.1 be a subset of the contracted pairs of Λ\Lambda, which defines a sub-contraction ΛS\Lambda|_S. For any pair aa in the set of contracted pairs of the sub-contraction, the second field operator of the pair aa in ΛS\Lambda|_S is equal to the second field operator of the same pair in the original contraction Λ\Lambda. In formula terms: (ΛS).sndFieldOfContract(a)=Λ.sndFieldOfContract(a) (\Lambda|_S).\text{sndFieldOfContract}(a) = \Lambda.\text{sndFieldOfContract}(a) where sndFieldOfContract\text{sndFieldOfContract} identifies the second field operator (typically the one with the larger index) in a contracted pair.

theorem

Mapping the first field of a quotient contraction pair back to the original indices

#quotContraction_fstFieldOfContract_uncontractedListEmd

Let φs\varphi s be a sequence of field operators and Λ\Lambda be a Wick contraction on φs\varphi s, where Λ.1\Lambda.1 denotes the set of contracted pairs. Let SΛ.1S \subseteq \Lambda.1 be a subset of these pairs, and let Λ/S\Lambda/S (denoted `quotContraction S hs`) be the quotient contraction on the sequence of operators that remain uncontracted after the pairs in SS are removed. Let ee be the embedding `uncontractedListEmd` which maps indices from the uncontracted sequence back to the original sequence. For any pair aa in the quotient contraction Λ/S\Lambda/S, the image under ee of the first operator's index in aa is equal to the index of the first operator of the corresponding pair in the original contraction Λ\Lambda. In mathematical notation: e((Λ/S).fstFieldOfContract(a))=Λ.fstFieldOfContract({e(i)ia}) e\left((\Lambda/S).\text{fstFieldOfContract}(a)\right) = \Lambda.\text{fstFieldOfContract}\left(\{e(i) \mid i \in a\}\right) where fstFieldOfContract\text{fstFieldOfContract} identifies the first operator (typically the one with the smaller index) in a contracted pair.

theorem

The second field of a quotient contraction corresponds to the second field of the original contraction via embedding

#quotContraction_sndFieldOfContract_uncontractedListEmd

Let φs\varphi s be a sequence of field operators and Λ\Lambda be a Wick contraction on φs\varphi s. Let SΛ.1S \subseteq \Lambda.1 be a subset of the contracted pairs of Λ\Lambda, and let quotContraction(S)\text{quotContraction}(S) be the Wick contraction defined on the sequence of operators that remain after the contractions in SS have been performed. Let uncontractedListEmd\text{uncontractedListEmd} be the embedding function that maps the index of an operator in the uncontracted sequence back to its original index in φs\varphi s. For any pair aa in the quotient contraction, the image of its second field operator's index under uncontractedListEmd\text{uncontractedListEmd} is equal to the index of the second field operator of the corresponding mapped pair in the original contraction Λ\Lambda. In mathematical notation: uncontractedListEmd(sndFieldOfContractΛ/S(a))=sndFieldOfContractΛ({uncontractedListEmd(i)ia}) \text{uncontractedListEmd}\left( \text{sndFieldOfContract}_{\Lambda/S}(a) \right) = \text{sndFieldOfContract}_{\Lambda}\left( \{ \text{uncontractedListEmd}(i) \mid i \in a \} \right) where sndFieldOfContract\text{sndFieldOfContract} identifies the index of the second field in a contracted pair (typically the one with the larger index).

theorem

Quotient Contractions Preserve Grading Compliance

#quotContraction_gradingCompliant

Let φs\varphi s be a sequence of field operators and Λ\Lambda be a Wick contraction on φs\varphi s. Suppose that Λ\Lambda is grading compliant, meaning its contracted pairs satisfy the required statistical properties according to the fields involved. For any subset SΛ.1S \subseteq \Lambda.1 of the contracted pairs, let Λ/S\Lambda/S (the quotient contraction) be the Wick contraction defined on the sequence of operators [subContraction(S)]uc[\text{subContraction}(S)]^{uc} that remain after the contractions in SS have been performed. Then the quotient contraction Λ/S\Lambda/S is also grading compliant.

theorem

aΛ/S    map(a)ΛSa \in \Lambda/S \iff \text{map}(a) \in \Lambda \setminus S

#mem_quotContraction_iff

Let φs\varphi s be a sequence of field operators and Λ\Lambda be a Wick contraction on φs\varphi s. Let SΛS \subseteq \Lambda be a subset of the contracted pairs. The quotient contraction Λ/S\Lambda/S is the Wick contraction defined on the operators remaining uncontracted by SS. Let uncontractedListEmd\text{uncontractedListEmd} be the embedding that maps the indices of these uncontracted operators back to their original positions in φs\varphi s. For any set of indices aa in the uncontracted list, aa is a contracted pair in the quotient contraction Λ/S\Lambda/S if and only if its image under uncontractedListEmd\text{uncontractedListEmd} is a contracted pair in Λ\Lambda that is not in SS: a(Λ/S)    map(uncontractedListEmd,a)ΛS a \in (\Lambda/S) \iff \text{map}(\text{uncontractedListEmd}, a) \in \Lambda \setminus S