docs: Fix typos in docs
This commit is contained in:
parent
cc20d096ea
commit
d2ce55ddd0
27 changed files with 67 additions and 63 deletions
|
@ -43,7 +43,7 @@ The structure `FieldSpecification` is defined to have the following content:
|
|||
index of the field and its conjugate.
|
||||
- For every field `f` in `Field`, a type `AsymptoticLabel f` whose elements label the different
|
||||
types of incoming asymptotic field operators associated with the
|
||||
field `f` (this is also matches the types of outgoing asymptotic field operators).
|
||||
field `f` (this also matches the types of outgoing asymptotic field operators).
|
||||
For example,
|
||||
- For `f` a *real-scalar field*, `AsymptoticLabel f` will have a unique element.
|
||||
- For `f` a *complex-scalar field*, `AsymptoticLabel f` will have two elements, one for the
|
||||
|
@ -81,7 +81,7 @@ variable (𝓕 : FieldSpecification)
|
|||
element labelled `outAsymp f e p` corresponding to an outgoing asymptotic field operator of the
|
||||
field `f`, of label `e` (e.g. specifying the spin), and momentum `p`.
|
||||
|
||||
As some intuition, if `f` corresponds to a Weyl-fermion field, then
|
||||
As an example, if `f` corresponds to a Weyl-fermion field, then
|
||||
- For `inAsymp f e p`, `e` would correspond to a spin `s`, and `inAsymp f e p` would, once
|
||||
represented in the operator algebra,
|
||||
be proportional to the creation operator `a(p, s)`.
|
||||
|
@ -120,7 +120,7 @@ def fieldOpToField : 𝓕.FieldOp → 𝓕.Field
|
|||
- For `φ` an element of `𝓕.FieldOp`, `𝓕 |>ₛ φ` is `fieldOpStatistic φ`.
|
||||
- For `φs` a list of `𝓕.FieldOp`, `𝓕 |>ₛ φs` is the product of `fieldOpStatistic φ` over
|
||||
the list `φs`.
|
||||
- For a function `f : Fin n → 𝓕.FieldOp` and a finset `a` of `Fin n`, `𝓕 |>ₛ ⟨f, a⟩` is the
|
||||
- For a function `f : Fin n → 𝓕.FieldOp` and a finite set `a` of `Fin n`, `𝓕 |>ₛ ⟨f, a⟩` is the
|
||||
product of `fieldOpStatistic (f i)` for all `i ∈ a`. -/
|
||||
def fieldOpStatistic : 𝓕.FieldOp → FieldStatistic := 𝓕.statistic ∘ 𝓕.fieldOpToField
|
||||
|
||||
|
|
|
@ -66,18 +66,18 @@ def fieldOpToCreateAnnihilateTypeCongr : {i j : 𝓕.FieldOp} → i = j →
|
|||
For a field specification `𝓕`, the (sigma) type `𝓕.CrAnFieldOp`
|
||||
corresponds to the type of creation and annihilation parts of field operators.
|
||||
It formally defined to consist of the following elements:
|
||||
- for each in incoming asymptotic field operator `φ` in `𝓕.FieldOp` an element
|
||||
- for each incoming asymptotic field operator `φ` in `𝓕.FieldOp` an element
|
||||
written as `⟨φ, ()⟩` in `𝓕.CrAnFieldOp`, corresponding to the creation part of `φ`.
|
||||
Here `φ` has no annihilation part. (Here `()` is the unique element of `Unit`.)
|
||||
- for each position field operator `φ` in `𝓕.FieldOp` an element of `𝓕.CrAnFieldOp`
|
||||
written as `⟨φ, .create⟩`, corresponding to the creation part of `φ`.
|
||||
- for each position field operator `φ` in `𝓕.FieldOp` an element of `𝓕.CrAnFieldOp`
|
||||
written as `⟨φ, .annihilate⟩`, corresponding to the annihilation part of `φ`.
|
||||
- for each out outgoing asymptotic field operator `φ` in `𝓕.FieldOp` an element
|
||||
- for each outgoing asymptotic field operator `φ` in `𝓕.FieldOp` an element
|
||||
written as `⟨φ, ()⟩` in `𝓕.CrAnFieldOp`, corresponding to the annihilation part of `φ`.
|
||||
Here `φ` has no creation part. (Here `()` is the unique element of `Unit`.)
|
||||
|
||||
As some intuition, if `f` corresponds to a Weyl-fermion field, it would contribute
|
||||
As an example, if `f` corresponds to a Weyl-fermion field, it would contribute
|
||||
the following elements to `𝓕.CrAnFieldOp`
|
||||
- an element corresponding to incoming asymptotic operators for each spin `s`: `a(p, s)`.
|
||||
- an element corresponding to the creation parts of position operators for each each Lorentz
|
||||
|
|
|
@ -20,7 +20,7 @@ variable {𝓕 : FieldSpecification}
|
|||
- `φ₀` is a field creation operator
|
||||
- `φ₁` is a field annihilation operator.
|
||||
|
||||
Thus, colloquially `𝓕.normalOrderRel φ₀ φ₁` says the creation operators are 'less then'
|
||||
Thus, colloquially `𝓕.normalOrderRel φ₀ φ₁` says the creation operators are less than
|
||||
annihilation operators. -/
|
||||
def normalOrderRel : 𝓕.CrAnFieldOp → 𝓕.CrAnFieldOp → Prop :=
|
||||
fun a b => CreateAnnihilate.normalOrder (𝓕 |>ᶜ a) (𝓕 |>ᶜ b)
|
||||
|
|
|
@ -198,10 +198,10 @@ lemma timeOrderList_eq_maxTimeField_timeOrderList (φ : 𝓕.FieldOp) (φs : Lis
|
|||
- `φ₀` is an *outgoing* asymptotic operator
|
||||
- `φ₁` is an *incoming* asymptotic field operator
|
||||
- `φ₀` and `φ₁` are both position field operators where
|
||||
the `SpaceTime` point of `φ₀` has a time *greater* then or equal to that of `φ₁`.
|
||||
the `SpaceTime` point of `φ₀` has a time *greater* than or equal to that of `φ₁`.
|
||||
|
||||
Thus, colloquially `𝓕.crAnTimeOrderRel φ₀ φ₁` if `φ₀` has time *greater* then or equal to `φ₁`.
|
||||
The use of *greater* then rather then *less* then is because on ordering lists of operators
|
||||
Thus, colloquially `𝓕.crAnTimeOrderRel φ₀ φ₁` if `φ₀` has time *greater* than or equal to `φ₁`.
|
||||
The use of *greater* than rather then *less* than is because on ordering lists of operators
|
||||
it is needed that the operator with the greatest time is to the left.
|
||||
-/
|
||||
def crAnTimeOrderRel (a b : 𝓕.CrAnFieldOp) : Prop := 𝓕.timeOrderRel a.1 b.1
|
||||
|
|
Loading…
Add table
Add a link
Reference in a new issue