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- EReal.abs_fun f x = ↑‖f x‖
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- Complex.re_fun f x = (f x).re
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- Complex.im_fun f x = (f x).im
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- Complex.conj_fun f x = (starRingEnd ℂ) (f x)
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- EReal.pos_fun f x = ↑(max (f x) 0)
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- EReal.neg_fun f x = ↑(max (-f x) 0)
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- Real.complex_fun f x = ↑(f x)
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- Real.EReal_fun f x = ↑(f x)
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Definition 1.3.2
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- RealSimpleFunction f = ∃ (k : ℕ) (c : Fin k → ℝ) (E : Fin k → Set (EuclideanSpace' d)), (∀ (i : Fin k), LebesgueMeasurable (E i)) ∧ f = ∑ i : Fin k, c i • (E i).indicator'
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- ComplexSimpleFunction f = ∃ (k : ℕ) (c : Fin k → ℂ) (E : Fin k → Set (EuclideanSpace' d)), (∀ (i : Fin k), LebesgueMeasurable (E i)) ∧ f = ∑ i : Fin k, c i • Complex.indicator (E i)
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- ⋯ = ⋯
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- RealSimpleFunction.coe_complex f = { coe := ⋯ }
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- hf.integ = ∑ i : Fin (Exists.choose hf), ⋯.choose i * Lebesgue_measure (⋯.choose i)
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The atom indexed by n is the intersection over all $i$ of ($E_i$ if bit $i$ is 1, else $E_i^c$)
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Helper: construct atom index from membership pattern. The atom index encodes x's membership in each set as bits.
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The atom index is bounded by 2^(k+k')
Atoms are measurable if the original sets are
Indicator function evaluates to c if x ∈ E
Indicator function evaluates to 0 if x ∉ E
The weighted measure sum for a representation
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- UnsignedSimpleFunction.IntegralWellDef.weightedMeasureSum c E = ∑ i : Fin k, c i * Lebesgue_measure (E i)
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Core lemma: Two representations of the same function give the same weighted measure sum. This is the heart of Lemma 1.3.4 (Venn diagram argument).
The atom for a single family of sets, using k' = 0 in the general atom definition
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- UnsignedSimpleFunction.IntegralWellDef.singleAtom E n = UnsignedSimpleFunction.IntegralWellDef.atom E (fun (x : Fin 0) => ∅) ⟨↑n, ⋯⟩
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Single atoms are pairwise disjoint
Every point is in exactly one singleAtom
Lemma 1.3.4 (Well-definedness of simple integral)
Definition 1.3.5
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- AlmostEverywhereEqual f g = AlmostAlways fun (x : EuclideanSpace' d) => f x = g x
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Almost everywhere equality is reflexive
Almost everywhere equality is symmetric
Almost everywhere equality is transitive
Almost everywhere equality is an equivalence relation
Exercise 1.3.1 (i) (Unsigned linearity)
Exercise 1.3.1 (i) (Unsigned linearity)
Exercise 1.3.1 (ii) (Finiteness)
Exercise 1.3.1 (iii) (Vanishing)
Exercise 1.3.1 (iv) (Equivalence)
Exercise 1.3.1 (v) (Monotonicity)
Exercise 1.3.1(vi) (Compatibility with Lebesgue measure)
Exercise 1.3.1(vi) (Compatibility with Lebesgue measure)
Definition 1.3.6 (Absolutely convergent simple integral)
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- hf.AbsolutelyIntegrable = (⋯.integ < ⊤)
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Definition 1.3.6 (Absolutely convergent simple integral)
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- hf.AbsolutelyIntegrable = (⋯.integ < ⊤)
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Single atoms are measurable
On a point in singleAtom n, the original sum equals atomValue n
The original function equals the sum over atoms with atomValue coefficients
Disjoint representation: any RealSimpleFunction has an equivalent representation
with pairwise disjoint, measurable sets.
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- ⋯ = ⋯
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- ⋯ = ⋯
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- ⋯ = ⋯
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- ⋯ = ⋯
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Exercise 1.3.2 (i) (*-linearity)
Exercise 1.3.2 (i) (*-linearity)
Exercise 1.3.2 (i) (*-linearity)
Exercise 1.3.2 (ii) (equivalence)
Exercise 1.3.2(iii) (Compatibility with Lebesgue measure)
Exercise 1.3.2(iii) (Compatibility with Lebesgue measure)