Definitions for Topological Entanglement Entropy and Holography
DefinitionQAlgorithms_Papers_Independent_Intakethird100_P58The objects the formalized statements of Topological Entanglement Entropy and Holography (arXiv:0805.1891) are stated in. Each was checked against the paper by a blind read-back and a moderator.
RotationalModel: The three reduced actions: (3.13), (3.17), and (4.8), PDF pp.9,10,15.radialDegree: Radius power from the round angular factor; PDF pp.7,15.warp: Coefficient multiplying the squared inverse-profile derivative; PDF pp.9,11,15.warpDerivative: Derivative of the warp coefficient, used in the direct-profile equation.profileDensity: Actual inverse-profile action density, with the source's z parametrization.InverseEquation: Euler--Lagrange equation of the reduced inverse-profile action. This is (3.20) for D3 and the undivided variational form of (4.9) for D4.DirectEquation: Direct-profile Euler--Lagrange equation, (3.7), (3.18), or (4.12). It also applies to annular graphs, whose inverse is not a single-valued function.height: Invert the actual strictly decreasing radius graph on its physical interval. On that graph's range the defining set is a nonempty bounded singleton. Values outside the range are unused. This definition does not introduce a free inverse.RegularGraph: Common regularity, anchoring, stationarity, and finite regulated area conditions. The ODE is imposed only at positive z strictly before the endpoint. A smooth extension through z=0 fixes total derivatives there without prescribing UV coefficients. The disk endpoint may have a singular inverse derivative.IsDisk: Regular disk cap, with the direct profile constructed by inversion. The physical compactified disks have b<1; the singular joining limit is excluded. The zero axis slope is a one-sided derivative, not the derivative of a default extension. Source: PDF pp.7--10,16.IsCylinder: Regular compactified cylinder, with positive endpoint radius and smooth inverse profile at z=1. This does not assume the endpoint expansion. Source: PDF pp.10--11,16.IsProfile: The two regular source topologies, without claiming exactly two solutions.regulatedAction: Unnormalized regulated action integral. Only positive cutoffs below b are used.uv: UV subtraction in the inverse-profile integral; (3.15), (3.23), (4.17). For D3 the dimensionless compactification radius is 1/2.conformalEntropy: Conformal reduced entropy, no end-cap term; (3.13), PDF p.9.d3Entropy: Compactified D3 reduced entropy in the (3.17)/(3.23) normalization. The extra pi in (3.19) is not used.D4Parameters: Independent positive D4 scales with alpha-prime=1; PDF pp.14,20.d4U0: D4 tip scale U0=4pilambda/(9*R4^2), (4.2).d4Newton: Ten-dimensional Newton constant from (4.26); used only for N>=1.d4Prefactor: The explicitly reduced (4.8) prefactor, with R^6=(pi*lambda)^2. No incorrect round-sphere volume is assumed to derive this expression.d4Entropy: D4 entropy for the source's reduced action (4.8).conformalF: Corrected conformal variable x=1-r/R in (3.9). The printed x=1-R/r on PDF p.7 has the wrong sign in the physical interior.FirstD4Coefficient: The first D4 large-radius coefficient equation (4.19), with regular endpoint and boundary data only. Its vanishing is a theorem conclusion, not a hypothesis.SecondD4Coefficient: The next regular coefficient problem (4.20), after the leading coefficient vanishes.d4G: The explicit regular coefficient (4.23), PDF p.20.d4GPrime: Simplified derivative (4.22), including its regular value at z=1.d4ConstantDensity: Radius-independent integrand of (4.24), before its disputed printed evaluation.ShrinkingOscillations: Usual qualitative diminishing-envelope oscillation: a finite limit, with values strictly on both sides in every punctured neighborhood. No rate, exact decimal, or monotonicity of successive numerical extrema is added.IsAnnulus: Nontrivial stationary annular surface, PDF pp.11,22--25 (and conformal pp.8--9). There is no global-minimality field.
import Mathlib
/-!
Reduced rotational profile problems in Pakman--Parnachev, arXiv:0805.1891v2.
The actions below are the paper's explicitly chosen reduced actions, not a derivation
of their disputed absolute geometric normalization. All lengths in the compactified
models are dimensionless. Logarithms are natural. No claim identifies arbitrary
stationary profiles with global entropy minimizers.
-/
noncomputable section
namespace QAlgorithms.Papers.Independent.Intakethird100.P58
open Set Filter MeasureTheory
open scoped Topology
/-- The three reduced actions: (3.13), (3.17), and (4.8), PDF pp.9,10,15. -/
inductive RotationalModel where
| conformal
| d3
| d4
deriving DecidableEq
/-- Radius power from the round angular factor; PDF pp.7,15. -/
def radialDegree : RotationalModel → ℕ
| .conformal => 1
| .d3 => 1
| .d4 => 2
/-- Coefficient multiplying the squared inverse-profile derivative; PDF pp.9,11,15. -/
def warp : RotationalModel → ℝ → ℝ
| .conformal, _ => 1
| .d3, z => 1 - z ^ 4
| .d4, z => z * (1 - z ^ 3)
/-- Derivative of the warp coefficient, used in the direct-profile equation. -/
def warpDerivative : RotationalModel → ℝ → ℝ
| .conformal, _ => 0
| .d3, z => -4 * z ^ 3
| .d4, z => 1 - 4 * z ^ 3
example : warp .d3 1 = 0 ∧ warp .d4 1 = 0 := by
norm_num [warp]
example : radialDegree .d4 = 2 := by
rfl
example : warpDerivative .d4 1 = -3 := by
norm_num [warpDerivative]
/-- Actual inverse-profile action density, with the source's z parametrization. -/
def profileDensity (m : RotationalModel) (r : ℝ → ℝ) (z : ℝ) : ℝ :=
r z ^ radialDegree m / z ^ 3 * Real.sqrt (1 + warp m z * deriv r z ^ 2)
example (c z : ℝ) : profileDensity .d3 (fun _ => c) z = c / z ^ 3 := by
simp [profileDensity, radialDegree]
/-- Euler--Lagrange equation of the reduced inverse-profile action.
This is (3.20) for D3 and the undivided variational form of (4.9) for D4. -/
def InverseEquation (m : RotationalModel) (r : ℝ → ℝ) (z : ℝ) : Prop :=
deriv (fun u => r u ^ radialDegree m * warp m u * deriv r u /
(u ^ 3 * Real.sqrt (1 + warp m u * deriv r u ^ 2))) z =
(radialDegree m : ℝ) * r z ^ (radialDegree m - 1) /
z ^ 3 * Real.sqrt (1 + warp m z * deriv r z ^ 2)
/-- Direct-profile Euler--Lagrange equation, (3.7), (3.18), or (4.12).
It also applies to annular graphs, whose inverse is not a single-valued function. -/
def DirectEquation (m : RotationalModel) (Z : ℝ → ℝ) (t : ℝ) : Prop :=
deriv (fun u => u ^ radialDegree m * deriv Z u /
(Z u ^ 3 * Real.sqrt (warp m (Z u) + deriv Z u ^ 2))) t =
t ^ radialDegree m *
(warpDerivative m (Z t) /
(2 * Z t ^ 3 * Real.sqrt (warp m (Z t) + deriv Z t ^ 2)) -
3 * Real.sqrt (warp m (Z t) + deriv Z t ^ 2) / Z t ^ 4)
/-- Invert the actual strictly decreasing radius graph on its physical interval.
On that graph's range the defining set is a nonempty bounded singleton. Values
outside the range are unused. This definition does not introduce a free inverse. -/
def height (r : ℝ → ℝ) (b t : ℝ) : ℝ :=
sInf {z : ℝ | z ∈ Icc 0 b ∧ r z = t}
/-- Common regularity, anchoring, stationarity, and finite regulated area conditions.
The ODE is imposed only at positive z strictly before the endpoint. A smooth
extension through z=0 fixes total derivatives there without prescribing UV coefficients.
The disk endpoint may have a singular inverse derivative. -/
def RegularGraph (m : RotationalModel) (R b : ℝ) (r : ℝ → ℝ) : Prop :=
0 < R ∧ 0 < b ∧ r 0 = R ∧ ContinuousOn r (Icc 0 b) ∧
StrictAntiOn r (Icc 0 b) ∧
(∀ z ∈ Ico 0 b, ContDiffAt ℝ 2 r z) ∧
(∀ z ∈ Ioo 0 b, 0 < r z ∧ InverseEquation m r z) ∧
(∀ a : ℝ, 0 < a → a < b → IntervalIntegrable (profileDensity m r) volume a b)
/-- Regular disk cap, with the direct profile constructed by inversion.
The physical compactified disks have b<1; the singular joining limit is excluded.
The zero axis slope is a one-sided derivative, not the derivative of a default extension.
Source: PDF pp.7--10,16. -/
def IsDisk (m : RotationalModel) (R b : ℝ) (r : ℝ → ℝ) : Prop :=
RegularGraph m R b r ∧ r b = 0 ∧ (m = .conformal ∨ b < 1) ∧
ContDiffOn ℝ 2 (height r b) (Ico 0 R) ∧
HasDerivWithinAt (height r b) 0 (Ici 0) 0
/-- Regular compactified cylinder, with positive endpoint radius and smooth inverse
profile at z=1. This does not assume the endpoint expansion. Source: PDF pp.10--11,16. -/
def IsCylinder (m : RotationalModel) (R : ℝ) (r : ℝ → ℝ) : Prop :=
(m = .d3 ∨ m = .d4) ∧ RegularGraph m R 1 r ∧
0 < r 1 ∧ ContDiffAt ℝ 2 r 1
example : ¬ IsCylinder .conformal 1 (fun _ => 1) := by
simp [IsCylinder]
/-- The two regular source topologies, without claiming exactly two solutions. -/
def IsProfile (m : RotationalModel) (R b : ℝ) (r : ℝ → ℝ) : Prop :=
IsDisk m R b r ∨ (b = 1 ∧ IsCylinder m R r)
/-- Unnormalized regulated action integral. Only positive cutoffs below b are used. -/
def regulatedAction (m : RotationalModel) (r : ℝ → ℝ) (a b : ℝ) : ℝ :=
∫ z in a..b, profileDensity m r z
/-- UV subtraction in the inverse-profile integral; (3.15), (3.23), (4.17).
For D3 the dimensionless compactification radius is 1/2. -/
def uv (m : RotationalModel) (R a : ℝ) : ℝ :=
match m with
| .conformal => R / (2 * a ^ 2) + Real.log (a / R) / (8 * R)
| .d3 => R / (2 * a ^ 2) + Real.log (a / R) / (8 * R)
| .d4 => R ^ 2 / (2 * a ^ 2) - 3 / (2 * a) + Real.log a / (8 * R ^ 2)
example : uv .d4 1 1 = -1 := by
norm_num [uv]
/-- Conformal reduced entropy, no end-cap term; (3.13), PDF p.9. -/
def conformalEntropy (N : ℕ) (l : ℝ) (r : ℝ → ℝ) (a b : ℝ) : ℝ :=
4 * (N : ℝ) ^ 2 * l / (15 * Real.pi) * regulatedAction .conformal r a b
/-- Compactified D3 reduced entropy in the (3.17)/(3.23) normalization.
The extra pi in (3.19) is not used. -/
def d3Entropy (N : ℕ) (r : ℝ → ℝ) (a b : ℝ) : ℝ :=
4 * (N : ℝ) ^ 2 / 15 * regulatedAction .d3 r a b
/-- Independent positive D4 scales with alpha-prime=1; PDF pp.14,20. -/
structure D4Parameters where
coupling : ℝ
circleRadius : ℝ
coupling_pos : 0 < coupling
circleRadius_pos : 0 < circleRadius
/-- D4 tip scale U0=4*pi*lambda/(9*R4^2), (4.2). -/
def d4U0 (P : D4Parameters) : ℝ :=
4 * Real.pi * P.coupling / (9 * P.circleRadius ^ 2)
/-- Ten-dimensional Newton constant from (4.26); used only for N>=1. -/
def d4Newton (P : D4Parameters) (N : ℕ) : ℝ :=
8 * Real.pi ^ 6 * P.coupling ^ 2 / (N : ℝ) ^ 2
/-- The explicitly reduced (4.8) prefactor, with R^6=(pi*lambda)^2.
No incorrect round-sphere volume is assumed to derive this expression. -/
def d4Prefactor (P : D4Parameters) (N : ℕ) : ℝ :=
Real.pi ^ 3 * (Real.pi * P.coupling) ^ 2 * d4U0 P * P.circleRadius /
(2 * d4Newton P N)
/-- D4 entropy for the source's reduced action (4.8). -/
def d4Entropy (P : D4Parameters) (N : ℕ) (r : ℝ → ℝ) (a b : ℝ) : ℝ :=
d4Prefactor P N * regulatedAction .d4 r a b
example (P : D4Parameters) : d4Newton P 0 = 0 := by
simp [d4Newton]
/-- Corrected conformal variable x=1-r/R in (3.9).
The printed x=1-R/r on PDF p.7 has the wrong sign in the physical interior. -/
def conformalF (R b : ℝ) (r : ℝ → ℝ) (x : ℝ) : ℝ :=
height r b (R * (1 - x)) / (2 * R * Real.sqrt x)
/-- The first D4 large-radius coefficient equation (4.19), with regular endpoint
and boundary data only. Its vanishing is a theorem conclusion, not a hypothesis. -/
def FirstD4Coefficient (f : ℝ → ℝ) : Prop :=
f 0 = 0 ∧ (∀ z ∈ Icc (0 : ℝ) 1, ContDiffAt ℝ 2 f z) ∧
∀ z ∈ Ioo (0 : ℝ) 1,
4 * deriv f z + 2 * z ^ 3 * deriv f z + 5 * z * deriv f z ^ 3 -
7 * z ^ 4 * deriv f z ^ 3 + 2 * z ^ 7 * deriv f z ^ 3 -
2 * z * deriv (deriv f) z + 2 * z ^ 4 * deriv (deriv f) z = 0
/-- The next regular coefficient problem (4.20), after the leading coefficient vanishes. -/
def SecondD4Coefficient (g : ℝ → ℝ) : Prop :=
g 0 = 0 ∧ (∀ z ∈ Icc (0 : ℝ) 1, ContDiffAt ℝ 2 g z) ∧
∀ z ∈ Ioo (0 : ℝ) 1,
4 + 4 * deriv g z + 2 * z ^ 3 * deriv g z -
2 * z * deriv (deriv g) z + 2 * z ^ 4 * deriv (deriv g) z = 0
/-- The explicit regular coefficient (4.23), PDF p.20. -/
def d4G (z : ℝ) : ℝ :=
-Real.arctan ((1 + 2 * z) / Real.sqrt 3) / Real.sqrt 3 -
Real.log (1 + z + z ^ 2) / 2 + Real.pi / (6 * Real.sqrt 3)
/-- Simplified derivative (4.22), including its regular value at z=1. -/
def d4GPrime (z : ℝ) : ℝ :=
-(1 + z) / (1 + z + z ^ 2)
example : d4GPrime 1 = -(2 : ℝ) / 3 := by
norm_num [d4GPrime]
/-- Radius-independent integrand of (4.24), before its disputed printed evaluation. -/
def d4ConstantDensity (z : ℝ) : ℝ :=
(4 * d4G z + z * (1 - z ^ 3) * d4GPrime z ^ 2) / (2 * z ^ 3)
/-- Usual qualitative diminishing-envelope oscillation: a finite limit, with
values strictly on both sides in every punctured neighborhood. No rate, exact
decimal, or monotonicity of successive numerical extrema is added. -/
def ShrinkingOscillations (f : ℝ → ℝ) (side : Set ℝ) (endpoint limit : ℝ) : Prop :=
Tendsto f (nhdsWithin endpoint side) (nhds limit) ∧
∀ delta : ℝ, 0 < delta →
(∃ x ∈ side, 0 < |x - endpoint| ∧ |x - endpoint| < delta ∧ f x < limit) ∧
(∃ x ∈ side, 0 < |x - endpoint| ∧ |x - endpoint| < delta ∧ limit < f x)
/-- Nontrivial stationary annular surface, PDF pp.11,22--25 (and conformal pp.8--9).
There is no global-minimality field. -/
def IsAnnulus (m : RotationalModel) (Ri Re : ℝ) (Z : ℝ → ℝ) : Prop :=
0 < Ri ∧ Ri < Re ∧ ContinuousOn Z (Icc Ri Re) ∧ Z Ri = 0 ∧ Z Re = 0 ∧
∀ t ∈ Ioo Ri Re, ContDiffAt ℝ 2 Z t ∧ 0 < Z t ∧
(m = .conformal ∨ Z t < 1) ∧ DirectEquation m Z t
end QAlgorithms.Papers.Independent.Intakethird100.P58
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What the Lean code literally says, in plain math · gpt-6.1-sol
QAlgorithms.Papers.Independent.Intakethird100.P58.D4Parameters
This defines a structure whose data consist of two real numbers, called the coupling and the circle radius , together with proofs of the strict inequalities and . Thus every element of this structure carries both positive real parameters and evidence of their positivity.
QAlgorithms.Papers.Independent.Intakethird100.P58.DirectEquation
For every rotational model , every function , and every real , the direct-equation predicate means precisely the equality
where , ; , , ; and , , , for all real . No differentiability, positivity, or nonzero-denominator hypotheses are included. Every derivative is assigned value where the relevant function is not differentiable, division by zero has value , and square roots of nonpositive arguments have value . Thus the equality is meaningful also when , when , or when the square-root argument is nonpositive; its right-hand side is in each of these cases.
QAlgorithms.Papers.Independent.Intakethird100.P58.FirstD4Coefficient
For any function , this defines the proposition that , that is twice continuously differentiable at every real point , and that at every ,
The differentiability requirement at both endpoints is with respect to the full real domain, rather than merely within . The differential equation is required only on the open interval, and no value at is prescribed.
QAlgorithms.Papers.Independent.Intakethird100.P58.InverseEquation
For every rotational model , every function , and every real , the inverse-equation predicate means precisely the equality
where , , and , , . Thus the exponent is for the first two models and for the third, with even when . No differentiability or positivity assumptions accompany the equality: every derivative displayed is assigned value where the function being differentiated is not differentiable, division by zero has value , and square roots of nonpositive real numbers have value . The predicate therefore also applies at , where its right-hand side is .
QAlgorithms.Papers.Independent.Intakethird100.P58.IsAnnulus
For a model chosen from , real numbers , and a function , this predicate requires , continuity of on , and . At every , it additionally requires that be twice continuously differentiable at as a function on , that , that either or , and that
where the model determines the quantities by
The differential equation and the differentiability requirements are imposed only in the open interval; at its endpoints, the stated requirements are continuity and zero boundary values.
QAlgorithms.Papers.Independent.Intakethird100.P58.IsCylinder
For a model , a real number , and a function , the cylinder predicate holds exactly when or , , the endpoint is positive, , is continuous on , whenever , and is twice continuously differentiable at every point of ; for every , and
for every real with , the function is Lebesgue integrable from to ; and and is twice continuously differentiable at as well. Here and when , while and when . Derivatives in the formulas are assigned value where differentiability fails, division by zero has value , and square roots of nonpositive arguments have value . The equation is required only for , and the integrability condition does not include .
QAlgorithms.Papers.Independent.Intakethird100.P58.IsDisk
For a model , real numbers , and a function , the disk predicate means that , , , is continuous on , for every , and is twice continuously differentiable at every point of ; for every , and
and for every real with , the function is Lebesgue integrable from to . Here , , or according as is , , or , respectively. In addition, , either or , and the function
is twice continuously differentiable within and has derivative at when restricted to . The infimum defining is assigned value if its defining set is empty; its definition is for every real . Derivatives in the displayed equation and integrand are assigned value where differentiability fails, division by zero has value , and square roots of nonpositive arguments have value . No equation is imposed at or , no integrability down to is required, and the stated regularity of excludes .
QAlgorithms.Papers.Independent.Intakethird100.P58.IsProfile
For a model , real numbers , and a function , the profile predicate holds exactly when the following common requirements hold and at least one of the two alternatives below holds: , , , is continuous on , whenever , is twice continuously differentiable at every point of , and for every , and
also, for every real with , the function is Lebesgue integrable from to . Here , , or according as is , , or , respectively. The first alternative is that , either or , and the function is twice continuously differentiable within and has derivative at within . The second alternative is that , or , , and is twice continuously differentiable at . The height function is defined for every real , with value when its defining set is empty. Derivatives in the equation and integrand are assigned value where differentiability fails, division by zero has value , and square roots of nonpositive arguments have value . Neither alternative requires the displayed equation at either endpoint or integrability from .
QAlgorithms.Papers.Independent.Intakethird100.P58.RegularGraph
For a model , real numbers , and a function , the regular-graph predicate holds exactly when , , , is continuous on , whenever , and is twice continuously differentiable at every ; additionally, for every , one has and
finally, for every real satisfying , the function
is Lebesgue integrable on the interval from to . Here for , for , and for , so is respectively . All derivatives in these formulas are totalized by assigning value where differentiability fails, division by zero has value , and square roots of nonpositive arguments have value . The twice-continuous-differentiability requirement includes as a point of the full real domain but excludes ; the equation and strict positivity of are required only on , and no integrability requirement down to is included.
QAlgorithms.Papers.Independent.Intakethird100.P58.RotationalModel
The type of rotational models has exactly three distinct values, named , , and . Equality between any two values of this type is decidable.
QAlgorithms.Papers.Independent.Intakethird100.P58.SecondD4Coefficient
For any function , this defines the proposition that , that is twice continuously differentiable at every real point , and that at every ,
The differentiability requirement at both endpoints is with respect to the full real domain, rather than merely within . The differential equation is required only on the open interval, and no value at is prescribed.
QAlgorithms.Papers.Independent.Intakethird100.P58.ShrinkingOscillations
For an arbitrary function , an arbitrary set , and arbitrary real numbers and , this predicate means that converges to as its argument approaches within , and that it takes values strictly below and strictly above at points of arbitrarily close to, but distinct from, . More explicitly, the convergence requires that for every there is an such that every with satisfies ; additionally, for every real , there exist such that
The endpoint need not belong to ; if it does, the convergence requirement forces . The witness requirements exclude an empty set or a set with no points distinct from sufficiently close to .
QAlgorithms.Papers.Independent.Intakethird100.P58.conformalEntropy
For every natural number , including , every real number , every function , and every pair of real endpoints , this defines
The natural number is viewed as a real number in this expression. No sign, differentiability, or integrability assumptions are imposed. The derivative is assigned zero wherever it does not exist, and division by zero is zero, so the integrand is zero at . The integral is the oriented Lebesgue interval integral, assigned zero if its integrand is not integrable between the endpoints; equal endpoints give zero. The resulting expression is also zero whenever or .
QAlgorithms.Papers.Independent.Intakethird100.P58.conformalF
For any real numbers and any function , this defines
No continuity, monotonicity, positivity, or existence of a point in the displayed set is assumed. If the set is nonempty, it is bounded below and its ordinary real infimum is used; if it is empty, its assigned infimum is zero, including when . The real square root is zero for , and division by zero is zero. Thus the defined value is zero whenever , , or the displayed set is empty.
QAlgorithms.Papers.Independent.Intakethird100.P58.d3Entropy
For every natural number , including , every function , and every pair of real endpoints , this defines
Here is viewed as a real number. No positivity, differentiability, or integrability hypotheses are required. The derivative is assigned zero wherever it does not exist, division by zero is zero, and the real square root is zero for nonpositive arguments; hence the integrand is zero at . The integral is the oriented Lebesgue interval integral, assigned zero when its integrand is not integrable between the endpoints; equal endpoints give zero. For , the defined value is zero.
QAlgorithms.Papers.Independent.Intakethird100.P58.d4ConstantDensity
For every real number , this defines
Here is the natural logarithm. The definition includes : division by zero in the real-number operations used here yields , so the defined density has value at .
QAlgorithms.Papers.Independent.Intakethird100.P58.d4Entropy
For every parameter structure , consisting of real numbers and together with proofs of these inequalities, every natural number , every function , and all real endpoints , this defines
with viewed as a real number. No regularity or sign assumptions on , and no restrictions on the endpoints, are imposed. The derivative is assigned zero wherever it does not exist, division by zero is zero, and the real square root is zero for nonpositive arguments; the integrand is therefore zero at . The integral is the oriented Lebesgue interval integral and is assigned zero if its integrand is not integrable between the endpoints; equal endpoints give zero. The case is included and makes the prefactor, and hence the defined value, zero.
QAlgorithms.Papers.Independent.Intakethird100.P58.d4G
For every real number , this defines the real-valued function
where is the natural logarithm and is the nonnegative square root of . The definition applies to all real ; its logarithm has a strictly positive argument for every such .
QAlgorithms.Papers.Independent.Intakethird100.P58.d4GPrime
For every real number , this defines the real-valued function
Its denominator is strictly positive for every real , so the formula applies without any restriction on .
QAlgorithms.Papers.Independent.Intakethird100.P58.d4Newton
For every parameter structure , consisting of real numbers and together with proofs of these inequalities, and every natural number , this defines
where is viewed as a real number. The circle radius is part of the input structure although it does not occur in the formula. The case is included and gives zero, because division by zero is defined to be zero.
QAlgorithms.Papers.Independent.Intakethird100.P58.d4Prefactor
For every parameter structure , consisting of real numbers and together with proofs of these inequalities, and every natural number , viewed as a real number in the formula, this defines
There is no assumption that is positive. All divisions use the convention that division by zero is zero; consequently, when , both the inner quotient in the denominator and the entire displayed quotient evaluate to zero.
QAlgorithms.Papers.Independent.Intakethird100.P58.d4U0
For every parameter structure , consisting of real numbers and together with proofs of these inequalities, this defines
QAlgorithms.Papers.Independent.Intakethird100.P58.height
For every function and every pair of real numbers , the height is defined to be
No continuity, monotonicity, positivity, or existence of a solution is assumed. When the set is nonempty, it is bounded and this is its real infimum, which need not itself belong to the set. When the set is empty, the defined value is ; this includes every when . For , the set is either empty or , so the height is for every .
QAlgorithms.Papers.Independent.Intakethird100.P58.large_Nc_scaling
Use either the choice , , called the case, or the choice , , called the case, and write
For each choice, say that real numbers and a function satisfy the profile conditions when all of the following hold: , , , is continuous and strictly decreasing on , is twice continuously differentiable at every point of , and, for every , and
Also require that be interval integrable with respect to Lebesgue measure from to for every real , and require one of two alternatives: either , , and the function
is twice continuously differentiable on and has derivative zero at within ; or , , and is twice continuously differentiable at . Here the real infimum is the total infimum operation, taking value zero for an empty set. The theorem asserts the conjunction of two statements. First, for every real and every satisfying these profile conditions in the case, there exists a real such that, for every natural number ,
Second, for every parameter pair with real coupling and circle radius , every real , and every satisfying these profile conditions in the case, there exists a real such that, for every natural number , on setting
one has
In each statement is chosen independently of , although it may depend on the previously quantified profile and, in the second statement, on ; neither statement requires the limit assertion for .
QAlgorithms.Papers.Independent.Intakethird100.P58.profileDensity
For every rotational model , every function , and every real , the profile density is the real number
where , , and , , . No differentiability, positivity, or nonzero-denominator assumptions are imposed. Here and in the formula, the derivative is assigned the value at a point where is not differentiable, division by zero has value , and the real square root has value for a nonpositive argument; in particular, the density is defined at and has value there.
QAlgorithms.Papers.Independent.Intakethird100.P58.radialDegree
For a rotational model , whose possible values are , , and , the natural number called its radial degree is defined by
QAlgorithms.Papers.Independent.Intakethird100.P58.regulatedAction
For any model among , any function , and any real endpoints , this defines
These are oriented Lebesgue interval integrals: reversing the endpoints reverses the sign, and equal endpoints give zero. No regularity, integrability, or positivity hypotheses are imposed. Here is assigned zero wherever is not differentiable, division by zero is zero, and the real square root is zero for nonpositive arguments; in particular, each displayed integrand is zero at . If the integrand is not integrable on the interval between the endpoints, the interval integral is assigned zero.
QAlgorithms.Papers.Independent.Intakethird100.P58.uv
For any model among and any real numbers , this defines
There are no positivity or nonzero assumptions on or . Every division by zero evaluates to zero; the real logarithm satisfies and, for nonzero real , means . Thus the definition includes zero and negative inputs.
QAlgorithms.Papers.Independent.Intakethird100.P58.warp
For every rotational model and every real number , the real number is defined by
There is no restriction on , including no positivity restriction on or on the resulting value.
QAlgorithms.Papers.Independent.Intakethird100.P58.warpDerivative
For every rotational model and every real number , the real number is defined by
These formulas define the function for all real .
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.