Each result cited is universally quantified over the data in its own statement.
Throughout, H = H β H=H_{\beta} H = H β , and a k j a_{kj} a kj , S S S and d N d_{N} d N are as in The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity ; W N W_{N} W N is open and nonempty by The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §open , and Π N \Pi_{N} Π N is as in The Logarithmic Energy of N Ordered Particles on the Weyl Chamber §energy . We write n Π = ∑ ( i , j ) ∈ Π N 1 n_{\Pi}=\sum_{(i,j)\in\Pi_{N}}1 n Π = ∑ ( i , j ) ∈ Π N 1 , N R = ∑ k = 1 N 1 N_{\mathbb{R}}=\sum_{k=1}^{N}1 N R = ∑ k = 1 N 1 (a real number), q 0 ( x ) = ∥ x ∥ 2 q_{0}(x)=\lVert x\rVert^{2} q 0 ( x ) = ∥ x ∥ 2 , q ( x ) = 1 + ∥ x ∥ 2 q(x)=1+\lVert x\rVert^{2} q ( x ) = 1 + ∥ x ∥ 2 and l ( x ) = log q ( x ) l(x)=\log q(x) l ( x ) = log q ( x ) . For a function φ \varphi φ of class C 2 C^{2} C 2 on W N W_{N} W N we abbreviate F ( x , φ ( x ) , D φ ( x ) , D 2 φ ( x ) ) F(x,\varphi(x),D\varphi(x),D^{2}\varphi(x)) F ( x , φ ( x ) , D φ ( x ) , D 2 φ ( x )) to F [ φ ] ( x ) F[\varphi](x) F [ φ ] ( x ) . Elementary order arithmetic is by Elementary Order Arithmetic in an Ordered Field , Elementary Arithmetic in an Ordered Field and Properties of the Absolute Value in an Ordered Field .
Step 0 (conventions and elementary facts). (a) Signs. 0 ≤ d N 0\le d_{N} 0 ≤ d N and 0 ≤ N R 0\le N_{\mathbb{R}} 0 ≤ N R , being finite sums of numbers equal to 0 0 0 or 1 1 1 (claim 5 of Properties of Finite Sums ). Π N \Pi_{N} Π N contains ( 1 , 2 ) (1,2) ( 1 , 2 ) , the sum of 1 1 1 over { ( 1 , 2 ) } \{(1,2)\} {( 1 , 2 )} is 1 1 1 by claim 1 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set , so 1 ≤ n Π 1\le n_{\Pi} 1 ≤ n Π by Nonnegativity and Monotonicity of a Sum over a Finite Index Set §monotone . For x ∈ W N x\in W_{N} x ∈ W N we have 0 ≤ ∥ x ∥ 2 0\le\lVert x\rVert^{2} 0 ≤ ∥ x ∥ 2 , so 1 ≤ q ( x ) 1\le q(x) 1 ≤ q ( x ) and 0 < q ( x ) − 1 ≤ 1 0<q(x)^{-1}\le1 0 < q ( x ) − 1 ≤ 1 by Order Reversal under Reciprocals, and Summability of the Reciprocals of the Squares §reciprocal . Finally 0 ≤ ∣ g ( x ) ∣ ≤ M 0\le|g(x)|\le M 0 ≤ ∣ g ( x ) ∣ ≤ M at any point x x x of W N W_{N} W N , so 0 ≤ M 0\le M 0 ≤ M .
(b) Logarithm. By The Function s log s s\log s s log s : Continuity, Young's Inequality and Lower Bounds, with the Elementary Bounds for the Exponential and the Logarithm §log , 1 − t − 1 ≤ log t ≤ t − 1 1-t^{-1}\le\log t\le t-1 1 − t − 1 ≤ log t ≤ t − 1 for positive t t t , and log ( s t ) = log s + log t \log(st)=\log s+\log t log ( s t ) = log s + log t for positive s , t s,t s , t by The Natural Logarithm . Hence: (b1) if 0 < y ≤ z 0<y\le z 0 < y ≤ z then log y ≤ log z \log y\le\log z log y ≤ log z , because log z = log y + log ( z y − 1 ) \log z=\log y+\log(zy^{-1}) log z = log y + log ( z y − 1 ) and log ( z y − 1 ) ≥ 1 − y z − 1 ≥ 0 \log(zy^{-1})\ge1-yz^{-1}\ge0 log ( z y − 1 ) ≥ 1 − y z − 1 ≥ 0 , as y z − 1 ≤ 1 yz^{-1}\le1 y z − 1 ≤ 1 ; (b2) log ( t 2 ) = 2 log t \log(t^{2})=2\log t log ( t 2 ) = 2 log t for positive t t t ; (b3) 0 ≤ 1 − q ( x ) − 1 ≤ l ( x ) 0\le1-q(x)^{-1}\le l(x) 0 ≤ 1 − q ( x ) − 1 ≤ l ( x ) ; (b4) 0 < 1 − 2 − 1 ≤ log 2 0<1-2^{-1}\le\log2 0 < 1 − 2 − 1 ≤ log 2 .
(c) Calculus. If φ , ψ \varphi,\psi φ , ψ are of class C 2 C^{2} C 2 on an open set and c ∈ R c\in\mathbb{R} c ∈ R , then c φ + ψ c\varphi+\psi c φ + ψ is of class C 2 C^{2} C 2 , with gradient c D φ + D ψ cD\varphi+D\psi cD φ + D ψ and Hessian c D 2 φ + D 2 ψ cD^{2}\varphi+D^{2}\psi c D 2 φ + D 2 ψ : this is claims 1 and 3 of Constants, Coordinate Functions, Sums and Products of C k C^k C k Functions on a Euclidean Open Set , applied to first and to iterated partial derivatives, read through Gradient of a Real-Valued Function on a Euclidean Open Set and Hessian Matrix of a C^2 Function . A constant function is smooth (claim 2 of Constants, Coordinate Functions, Sums and Products of C k C^k C k Functions on a Euclidean Open Set ), hence of class C 2 C^{2} C 2 by Smooth Map on a Euclidean Open Set , and its partial derivatives vanish, its difference quotients in Partial Derivative on a Euclidean Open Set being 0 0 0 . Traces satisfy tr ( c X + Y ) = c tr X + tr Y \operatorname{tr}(cX+Y)=c\operatorname{tr}X+\operatorname{tr}Y tr ( c X + Y ) = c tr X + tr Y by claim 1 of Basic Properties of the Trace . By claim 1 of Elementary Properties of the Euclidean Norm on R n \mathbb{R}^n R n , ∥ z ∥ 2 = z ⋅ z \lVert z\rVert^{2}=z\cdot z ∥ z ∥ 2 = z ⋅ z , so by Bilinearity and Symmetry of the Dot Product on R n \mathbb{R}^n R n
∥ c z + z ′ ∥ 2 = c 2 ∥ z ∥ 2 + 2 c z ⋅ z ′ + ∥ z ′ ∥ 2 . \lVert cz+z'\rVert^{2}=c^{2}\lVert z\rVert^{2}+2c\,z\cdot z'+\lVert z'\rVert^{2}. ∥ cz + z ′ ∥ 2 = c 2 ∥ z ∥ 2 + 2 c z ⋅ z ′ + ∥ z ′ ∥ 2 .
(d) The squared norm. By claim 2 of Elementary Properties of the Euclidean Norm on R n \mathbb{R}^n R n , q 0 ( x ) = 1 ⋅ d E ( x , 0 R N ) 2 q_{0}(x)=1\cdot d_{E}(x,0_{\mathbb{R}^{N}})^{2} q 0 ( x ) = 1 ⋅ d E ( x , 0 R N ) 2 , so by A Scaled Squared Distance to a Point is of Class C 2 C^2 C 2 , with Gradient and Hessian (with c = 1 c=1 c = 1 and a a a the origin), on every open subset of R N \mathbb{R}^{N} R N the function q 0 q_{0} q 0 is of class C 2 C^{2} C 2 with D q 0 ( x ) = 2 x Dq_{0}(x)=2x D q 0 ( x ) = 2 x and D 2 q 0 ( x ) = 2 I N D^{2}q_{0}(x)=2I_{N} D 2 q 0 ( x ) = 2 I N . By (c), the same holds for q = 1 + q 0 q=1+q_{0} q = 1 + q 0 on W N W_{N} W N .
Step 1 (the profile; claim 1). Let r = κ 2 + 8 θ c r=\sqrt{\kappa^{2}+8\theta c} r = κ 2 + 8 θ c and r ′ = λ 2 + 8 θ ω r'=\sqrt{\lambda^{2}+8\theta\omega} r ′ = λ 2 + 8 θ ω , so r 2 = κ 2 + 8 θ c r^{2}=\kappa^{2}+8\theta c r 2 = κ 2 + 8 θ c and r ′ 2 = λ 2 + 8 θ ω r'^{2}=\lambda^{2}+8\theta\omega r ′ 2 = λ 2 + 8 θ ω by Existence and Uniqueness of the Nonnegative Square Root . Since β = 1 2 ( κ + r ) \beta=\tfrac12(\kappa+r) β = 2 1 ( κ + r ) gives β − κ = 1 2 ( r − κ ) \beta-\kappa=\tfrac12(r-\kappa) β − κ = 2 1 ( r − κ ) ,
β ( β − κ ) = 1 4 ( r + κ ) ( r − κ ) = 1 4 ( r 2 − κ 2 ) = 2 θ c . \beta(\beta-\kappa)=\tfrac14(r+\kappa)(r-\kappa)=\tfrac14(r^{2}-\kappa^{2})=2\theta c . β ( β − κ ) = 4 1 ( r + κ ) ( r − κ ) = 4 1 ( r 2 − κ 2 ) = 2 θ c .
Since a = ( 4 θ ) − 1 ( r ′ − λ ) a=(4\theta)^{-1}(r'-\lambda) a = ( 4 θ ) − 1 ( r ′ − λ ) gives 2 θ a + λ = 1 2 ( r ′ + λ ) 2\theta a+\lambda=\tfrac12(r'+\lambda) 2 θ a + λ = 2 1 ( r ′ + λ ) ,
2 θ a 2 + λ a = a ( 2 θ a + λ ) = ( 8 θ ) − 1 ( r ′ − λ ) ( r ′ + λ ) = ( 8 θ ) − 1 ( r ′ 2 − λ 2 ) = ω . 2\theta a^{2}+\lambda a=a(2\theta a+\lambda)=(8\theta)^{-1}(r'-\lambda)(r'+\lambda)=(8\theta)^{-1}(r'^{2}-\lambda^{2})=\omega . 2 θ a 2 + λa = a ( 2 θ a + λ ) = ( 8 θ ) − 1 ( r ′ − λ ) ( r ′ + λ ) = ( 8 θ ) − 1 ( r ′ 2 − λ 2 ) = ω .
Let V 1 ( t ) = θ a t 2 V_{1}(t)=\theta a\,t^{2} V 1 ( t ) = θ a t 2 for t ∈ R t\in\mathbb{R} t ∈ R . By A Scaled Squared Distance to a Point is of Class C 2 C^2 C 2 , with Gradient and Hessian with n = 1 n=1 n = 1 , c = θ a c=\theta a c = θ a and a a a the origin (and claims 1 and 2 of Elementary Properties of the Euclidean Norm on R n \mathbb{R}^n R n in R 1 \mathbb{R}^{1} R 1 ), V 1 V_{1} V 1 is of class C 2 C^{2} C 2 on R \mathbb{R} R with V 1 ′ ( t ) = 2 θ a t V_{1}'(t)=2\theta a\,t V 1 ′ ( t ) = 2 θ a t and V 1 ′ ′ ( t ) = 2 θ a V_{1}''(t)=2\theta a V 1 ′′ ( t ) = 2 θ a . Moreover ∣ t ∣ 2 = t 2 |t|^{2}=t^{2} ∣ t ∣ 2 = t 2 (claims 1 and 4 of Properties of the Absolute Value in an Ordered Field ), so
0 ≤ ( 2 θ a ∣ t ∣ − 1 ) 2 = 4 θ 2 a 2 t 2 − 4 θ a ∣ t ∣ + 1 , 0\le(2\theta a|t|-1)^{2}=4\theta^{2}a^{2}t^{2}-4\theta a|t|+1 , 0 ≤ ( 2 θ a ∣ t ∣ − 1 ) 2 = 4 θ 2 a 2 t 2 − 4 θ a ∣ t ∣ + 1 ,
and dividing by 4 θ a > 0 4\theta a>0 4 θ a > 0 gives 1 ⋅ ∣ t ∣ − ( 4 θ a ) − 1 ≤ V 1 ( t ) 1\cdot|t|-(4\theta a)^{-1}\le V_{1}(t) 1 ⋅ ∣ t ∣ − ( 4 θ a ) − 1 ≤ V 1 ( t ) . Let P ^ ( x ) = H ( x ) + ∑ k = 1 N V 1 ( x k ) \widehat{P}(x)=H(x)+\sum_{k=1}^{N}V_{1}(x_{k}) P ( x ) = H ( x ) + ∑ k = 1 N V 1 ( x k ) . By claim 3 of Properties of Finite Sums and claim 1 of Elementary Properties of the Euclidean Norm on R n \mathbb{R}^n R n , ∑ k = 1 N V 1 ( x k ) = θ a ∥ x ∥ 2 \sum_{k=1}^{N}V_{1}(x_{k})=\theta a\lVert x\rVert^{2} ∑ k = 1 N V 1 ( x k ) = θ a ∥ x ∥ 2 , so P ^ = θ P \widehat{P}=\theta P P = θP . By The Confined Logarithmic Energy on the Weyl Chamber: Regularity, Penalty Property, Monotone Gradient and the Dissipation Inequality §penalty with a 0 = 1 a_{0}=1 a 0 = 1 and b 0 = ( 4 θ a ) − 1 b_{0}=(4\theta a)^{-1} b 0 = ( 4 θ a ) − 1 , P ^ \widehat{P} P is a penalty on W N W_{N} W N . Hence P = θ − 1 P ^ P=\theta^{-1}\widehat{P} P = θ − 1 P is of class C 2 C^{2} C 2 by (c) and Penalty on an Open Subset of Euclidean Space §regularity ; and for t ∈ R t\in\mathbb{R} t ∈ R , multiplying by θ \theta θ and by θ − 1 \theta^{-1} θ − 1 (claim 5 of Elementary Arithmetic in an Ordered Field ) shows { x ∈ W N : P ( x ) ≤ t } = { x ∈ W N : P ^ ( x ) ≤ θ t } \{x\in W_{N}:P(x)\le t\}=\{x\in W_{N}:\widehat{P}(x)\le\theta t\} { x ∈ W N : P ( x ) ≤ t } = { x ∈ W N : P ( x ) ≤ θt } , which is compact by Penalty on an Open Subset of Euclidean Space §sublevel . So P P P is a penalty on W N W_{N} W N , and claim 1 holds.
Step 2 (derivatives of P P P ). By The Confined Logarithmic Energy on the Weyl Chamber: Regularity, Penalty Property, Monotone Gradient and the Dissipation Inequality §regularity with this V 1 V_{1} V 1 and The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §derivatives , ∂ k P ^ ( x ) = 2 θ a x k + ∂ k H ( x ) \partial_{k}\widehat{P}(x)=2\theta a\,x_{k}+\partial_{k}H(x) ∂ k P ( x ) = 2 θ a x k + ∂ k H ( x ) and tr ( D 2 P ^ ( x ) ) = β S ( x ) + ∑ k = 1 N 2 θ a = β S ( x ) + 2 θ a N R \operatorname{tr}(D^{2}\widehat{P}(x))=\beta S(x)+\sum_{k=1}^{N}2\theta a=\beta S(x)+2\theta a N_{\mathbb{R}} tr ( D 2 P ( x )) = βS ( x ) + ∑ k = 1 N 2 θ a = βS ( x ) + 2 θ a N R . By (c),
D P ( x ) = θ − 1 D H ( x ) + 2 a x , tr ( D 2 P ( x ) ) = θ − 1 β S ( x ) + 2 a N R . DP(x)=\theta^{-1}DH(x)+2a\,x,\qquad \operatorname{tr}\bigl(D^{2}P(x)\bigr)=\theta^{-1}\beta S(x)+2aN_{\mathbb{R}} . D P ( x ) = θ − 1 DH ( x ) + 2 a x , tr ( D 2 P ( x ) ) = θ − 1 βS ( x ) + 2 a N R .
By (c), The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §calogero and The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §euler ,
∥ D P ( x ) ∥ 2 = θ − 2 ∥ D H ( x ) ∥ 2 + 4 a θ − 1 D H ( x ) ⋅ x + 4 a 2 ∥ x ∥ 2 = θ − 2 β 2 S ( x ) − 2 a θ − 1 β d N + 4 a 2 ∥ x ∥ 2 . \lVert DP(x)\rVert^{2}=\theta^{-2}\lVert DH(x)\rVert^{2}+4a\theta^{-1}DH(x)\cdot x+4a^{2}\lVert x\rVert^{2}=\theta^{-2}\beta^{2}S(x)-2a\theta^{-1}\beta d_{N}+4a^{2}\lVert x\rVert^{2}. ∥ D P ( x ) ∥ 2 = θ − 2 ∥ DH ( x ) ∥ 2 + 4 a θ − 1 DH ( x ) ⋅ x + 4 a 2 ∥ x ∥ 2 = θ − 2 β 2 S ( x ) − 2 a θ − 1 β d N + 4 a 2 ∥ x ∥ 2 .
Step 3 (the key identity). Let s , k ∈ R s,k\in\mathbb{R} s , k ∈ R and φ = s P + k \varphi=sP+k φ = s P + k . By (c), φ \varphi φ is of class C 2 C^{2} C 2 with D φ = s D P D\varphi=sDP D φ = sD P and D 2 φ = s D 2 P D^{2}\varphi=sD^{2}P D 2 φ = s D 2 P , and ∥ s D P ∥ 2 = s 2 ∥ D P ∥ 2 \lVert sDP\rVert^{2}=s^{2}\lVert DP\rVert^{2} ∥ sD P ∥ 2 = s 2 ∥ D P ∥ 2 . Insert Step 2 into the operator , write λ s P = λ s θ − 1 H + λ s a ∥ x ∥ 2 \lambda sP=\lambda s\theta^{-1}H+\lambda sa\lVert x\rVert^{2} λ s P = λ s θ − 1 H + λ s a ∥ x ∥ 2 , and use c = ( 2 θ ) − 1 ( β 2 − κ β ) c=(2\theta)^{-1}(\beta^{2}-\kappa\beta) c = ( 2 θ ) − 1 ( β 2 − κ β ) from Step 1. Collecting the coefficients of S ( x ) S(x) S ( x ) and of ∥ x ∥ 2 \lVert x\rVert^{2} ∥ x ∥ 2 gives, for x ∈ W N x\in W_{N} x ∈ W N ,
F [ φ ] ( x ) = e ( s ) S ( x ) + f ( s ) ∥ x ∥ 2 + λ s θ − 1 H ( x ) − s 2 a β d N − κ s a N R + λ k − g ( x ) , F[\varphi](x)=e(s)S(x)+f(s)\lVert x\rVert^{2}+\lambda s\theta^{-1}H(x)-s^{2}a\beta d_{N}-\kappa saN_{\mathbb{R}}+\lambda k-g(x), F [ φ ] ( x ) = e ( s ) S ( x ) + f ( s ) ∥ x ∥ 2 + λ s θ − 1 H ( x ) − s 2 a β d N − κ s a N R + λk − g ( x ) ,
e ( s ) = ( 2 θ ) − 1 ( ( s β ) 2 − κ s β − β 2 + κ β ) , f ( s ) = 2 θ a 2 s 2 + λ a s − ω . e(s)=(2\theta)^{-1}\bigl((s\beta)^{2}-\kappa s\beta-\beta^{2}+\kappa\beta\bigr),\qquad f(s)=2\theta a^{2}s^{2}+\lambda as-\omega . e ( s ) = ( 2 θ ) − 1 ( ( s β ) 2 − κ s β − β 2 + κ β ) , f ( s ) = 2 θ a 2 s 2 + λa s − ω .
Here e ( 1 ) = 0 e(1)=0 e ( 1 ) = 0 , and f ( 1 ) = 0 f(1)=0 f ( 1 ) = 0 by Step 1.
Step 4 (two bounds on H H H ). (U) For every positive μ \mu μ and x ∈ W N x\in W_{N} x ∈ W N ,
H ( x ) ≤ β n Π 2 μ S ( x ) + β n Π 2 ( log μ − 1 ) . H(x)\le\tfrac{\beta n_{\Pi}}{2\mu}S(x)+\tfrac{\beta n_{\Pi}}{2}(\log\mu-1). H ( x ) ≤ 2 μ β n Π S ( x ) + 2 β n Π ( log μ − 1 ) .
Indeed, let ( i , j ) ∈ Π N (i,j)\in\Pi_{N} ( i , j ) ∈ Π N and t = x i − x j > 0 t=x_{i}-x_{j}>0 t = x i − x j > 0 , so a i j ( x ) = t − 1 a_{ij}(x)=t^{-1} a ij ( x ) = t − 1 . The lower bound of (b) at μ t 2 \mu t^{2} μ t 2 , together with (b2), gives log μ + 2 log t = log ( μ t 2 ) ≥ 1 − μ − 1 a i j ( x ) 2 \log\mu+2\log t=\log(\mu t^{2})\ge1-\mu^{-1}a_{ij}(x)^{2} log μ + 2 log t = log ( μ t 2 ) ≥ 1 − μ − 1 a ij ( x ) 2 , so − log t ≤ 1 2 ( μ − 1 a i j ( x ) 2 − 1 + log μ ) -\log t\le\tfrac12(\mu^{-1}a_{ij}(x)^{2}-1+\log\mu) − log t ≤ 2 1 ( μ − 1 a ij ( x ) 2 − 1 + log μ ) . Squares are nonnegative, so a i j ( x ) 2 ≤ ∑ j ′ = 1 N a i j ′ ( x ) 2 ≤ S ( x ) a_{ij}(x)^{2}\le\sum_{j'=1}^{N}a_{ij'}(x)^{2}\le S(x) a ij ( x ) 2 ≤ ∑ j ′ = 1 N a i j ′ ( x ) 2 ≤ S ( x ) by claims 5 and 6 of Properties of Finite Sums . Hence − log ( x i − x j ) ≤ 1 2 ( μ − 1 S ( x ) − 1 + log μ ) -\log(x_{i}-x_{j})\le\tfrac12(\mu^{-1}S(x)-1+\log\mu) − log ( x i − x j ) ≤ 2 1 ( μ − 1 S ( x ) − 1 + log μ ) for every ( i , j ) ∈ Π N (i,j)\in\Pi_{N} ( i , j ) ∈ Π N . Summing over Π N \Pi_{N} Π N (Nonnegativity and Monotonicity of a Sum over a Finite Index Set §comparison , and claims 3 and 4 of Properties of a Sum over a Finite Index Set ) and multiplying by β \beta β gives (U).
(L) For every x ∈ W N x\in W_{N} x ∈ W N ,
H ( x ) ≥ − β n Π log 2 − β n Π 2 l ( x ) . H(x)\ge-\beta n_{\Pi}\log2-\tfrac{\beta n_{\Pi}}{2}\,l(x). H ( x ) ≥ − β n Π log 2 − 2 β n Π l ( x ) .
Indeed, for ( i , j ) ∈ Π N (i,j)\in\Pi_{N} ( i , j ) ∈ Π N , claims 2, 3 and 5 of Properties of the Absolute Value in an Ordered Field and claim 4 of Elementary Properties of the Euclidean Norm on R n \mathbb{R}^n R n give 0 < x i − x j ≤ ∣ x i ∣ + ∣ x j ∣ ≤ 2 ∥ x ∥ 0<x_{i}-x_{j}\le|x_{i}|+|x_{j}|\le2\lVert x\rVert 0 < x i − x j ≤ ∣ x i ∣ + ∣ x j ∣ ≤ 2 ∥ x ∥ , so ( x i − x j ) 2 ≤ 4 ∥ x ∥ 2 ≤ 4 q ( x ) (x_{i}-x_{j})^{2}\le4\lVert x\rVert^{2}\le4q(x) ( x i − x j ) 2 ≤ 4 ∥ x ∥ 2 ≤ 4 q ( x ) by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field . By (b1) and (b2), 2 log ( x i − x j ) ≤ log 4 + l ( x ) = 2 log 2 + l ( x ) 2\log(x_{i}-x_{j})\le\log4+l(x)=2\log2+l(x) 2 log ( x i − x j ) ≤ log 4 + l ( x ) = 2 log 2 + l ( x ) . Summing over Π N \Pi_{N} Π N as in (U) and multiplying by − β -\beta − β gives (L).
Step 5 (classical subsolutions of weight below 1 1 1 ). Let s 0 = 2 − 1 ( 1 + κ ( 2 β ) − 1 ) s_{0}=2^{-1}\bigl(1+\kappa(2\beta)^{-1}\bigr) s 0 = 2 − 1 ( 1 + κ ( 2 β ) − 1 ) . As stated in the theorem, 0 ≤ κ < 2 β 0\le\kappa<2\beta 0 ≤ κ < 2 β , so 0 ≤ κ ( 2 β ) − 1 < 1 0\le\kappa(2\beta)^{-1}<1 0 ≤ κ ( 2 β ) − 1 < 1 and, by claim 8 of Elementary Order Arithmetic in an Ordered Field , 0 < s 0 0<s_{0} 0 < s 0 and κ ( 2 β ) − 1 < s 0 < 1 \kappa(2\beta)^{-1}<s_{0}<1 κ ( 2 β ) − 1 < s 0 < 1 . Fix s s s with s 0 ≤ s < 1 s_{0}\le s<1 s 0 ≤ s < 1 ; then κ 2 < s β < β \tfrac{\kappa}{2}<s\beta<\beta 2 κ < s β < β . Since t 2 − κ t − ( u 2 − κ u ) = ( t − u ) ( t + u − κ ) t^{2}-\kappa t-(u^{2}-\kappa u)=(t-u)(t+u-\kappa) t 2 − κ t − ( u 2 − κ u ) = ( t − u ) ( t + u − κ ) ,
e ( s ) = ( 2 θ ) − 1 ( s β − β ) ( s β + β − κ ) < 0 , e(s)=(2\theta)^{-1}(s\beta-\beta)(s\beta+\beta-\kappa)<0, e ( s ) = ( 2 θ ) − 1 ( s β − β ) ( s β + β − κ ) < 0 ,
the first factor being negative and the second positive (as s β > κ 2 s\beta>\tfrac{\kappa}{2} s β > 2 κ and β > κ 2 \beta>\tfrac{\kappa}{2} β > 2 κ ); and
f ( s ) = f ( s ) − f ( 1 ) = ( s − 1 ) ( 2 θ a 2 ( s + 1 ) + λ a ) < 0. f(s)=f(s)-f(1)=(s-1)\bigl(2\theta a^{2}(s+1)+\lambda a\bigr)<0 . f ( s ) = f ( s ) − f ( 1 ) = ( s − 1 ) ( 2 θ a 2 ( s + 1 ) + λa ) < 0.
Put μ s = λ s θ − 1 β n Π ( 2 ( − e ( s ) ) ) − 1 \mu_{s}=\lambda s\theta^{-1}\beta n_{\Pi}\bigl(2(-e(s))\bigr)^{-1} μ s = λ s θ − 1 β n Π ( 2 ( − e ( s )) ) − 1 , which is positive since n Π ≥ 1 n_{\Pi}\ge1 n Π ≥ 1 ; C s = λ s θ − 1 β n Π 2 ( log μ s − 1 ) C_{s}=\lambda s\theta^{-1}\tfrac{\beta n_{\Pi}}{2}(\log\mu_{s}-1) C s = λ s θ − 1 2 β n Π ( log μ s − 1 ) ; and K s = λ − 1 ( ∣ C s ∣ + M ) ≥ 0 K_{s}=\lambda^{-1}(|C_{s}|+M)\ge0 K s = λ − 1 ( ∣ C s ∣ + M ) ≥ 0 . Multiplying (U) with μ = μ s \mu=\mu_{s} μ = μ s by λ s θ − 1 > 0 \lambda s\theta^{-1}>0 λ s θ − 1 > 0 gives λ s θ − 1 H ( x ) ≤ − e ( s ) S ( x ) + C s \lambda s\theta^{-1}H(x)\le-e(s)S(x)+C_{s} λ s θ − 1 H ( x ) ≤ − e ( s ) S ( x ) + C s . By Step 3 with k = − K s k=-K_{s} k = − K s , using f ( s ) ∥ x ∥ 2 ≤ 0 f(s)\lVert x\rVert^{2}\le0 f ( s ) ∥ x ∥ 2 ≤ 0 , − s 2 a β d N ≤ 0 -s^{2}a\beta d_{N}\le0 − s 2 a β d N ≤ 0 , − κ s a N R ≤ 0 -\kappa saN_{\mathbb{R}}\le0 − κ s a N R ≤ 0 (Step 0(a)) and − g ( x ) ≤ M -g(x)\le M − g ( x ) ≤ M ,
F [ s P − K s ] ( x ) ≤ C s − ∣ C s ∣ − M + M ≤ 0 ( x ∈ W N ) . F[sP-K_{s}](x)\le C_{s}-|C_{s}|-M+M\le0\qquad(x\in W_{N}). F [ s P − K s ] ( x ) ≤ C s − ∣ C s ∣ − M + M ≤ 0 ( x ∈ W N ) .
So s P − K s sP-K_{s} s P − K s is a classical subsolution of F F F on W N W_{N} W N . With s = s 0 < 1 s=s_{0}<1 s = s 0 < 1 this is hypothesis Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables §barrier for w = 1 w=1 w = 1 .
Step 6 (the operator hypotheses). Let b : W N → R N b:W_{N}\to\mathbb{R}^{N} b : W N → R N be the constant map with value the origin and G ( x ) = c S ( x ) + ω q 0 ( x ) + g ( x ) G(x)=cS(x)+\omega q_{0}(x)+g(x) G ( x ) = c S ( x ) + ω q 0 ( x ) + g ( x ) . By claim 4 of Bilinearity and Symmetry of the Dot Product on R n \mathbb{R}^n R n (with μ = 0 \mu=0 μ = 0 ), b ( x ) ⋅ p = 0 b(x)\cdot p=0 b ( x ) ⋅ p = 0 , so F F F is the operator of The Viscous Hamilton-Jacobi Operator with a Drift that is One-Sided Lipschitz on Sublevel Sets Satisfies the Operator Hypotheses of the Weighted-Penalty Comparison Principle with n = N n=N n = N , D = W N D=W_{N} D = W N , the penalty P P P , and λ , θ , κ , b , G \lambda,\theta,\kappa,b,G λ , θ , κ , b , G . The map b b b is continuous, and it is one-sided Lipschitz on sublevel sets with c R = 0 c_{R}=0 c R = 0 , since ( b ( x ) − b ( y ) ) ⋅ ( x − y ) = 0 (b(x)-b(y))\cdot(x-y)=0 ( b ( x ) − b ( y )) ⋅ ( x − y ) = 0 . For continuity of G G G : H H H is of class C 2 C^{2} C 2 by The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §derivatives , so D H DH DH is continuous on W N W_{N} W N by Continuity of the Value, Gradient and Hessian Maps of a Differentiable Function §hessian ; q 0 q_{0} q 0 is continuous on R N \mathbb{R}^{N} R N by The Squared Euclidean Norm is Smooth and claim 3 of Euclidean Space is Open in Itself, and C k C^k C k Maps are Continuous ; so q 0 ∘ D H q_{0}\circ DH q 0 ∘ DH and the restriction of q 0 q_{0} q 0 to W N W_{N} W N are continuous on W N W_{N} W N by claims 3 and 4 of Semicontinuity and Continuity Under Composition with a Continuous Map . By The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §calogero , G = c β − 2 ( q 0 ∘ D H ) + ω q 0 + g G=c\beta^{-2}(q_{0}\circ DH)+\omega q_{0}+g G = c β − 2 ( q 0 ∘ DH ) + ω q 0 + g . A combination c 1 f 1 + c 2 f 2 + c 3 f 3 c_{1}f_{1}+c_{2}f_{2}+c_{3}f_{3} c 1 f 1 + c 2 f 2 + c 3 f 3 of real functions continuous on W N W_{N} W N is continuous (Continuous Map Between Metric Spaces , with the metric of The Absolute Value Metric on the Real Line ): given x x x and ε > 0 \varepsilon>0 ε > 0 , take for each i i i a δ i \delta_{i} δ i that works for f i f_{i} f i at x x x with ε ( 3 ( 1 + ∣ c i ∣ ) ) − 1 \varepsilon\bigl(3(1+|c_{i}|)\bigr)^{-1} ε ( 3 ( 1 + ∣ c i ∣ ) ) − 1 , and the least δ \delta δ of the three (claim 9 of Elementary Order Arithmetic in an Ordered Field ); by claims 4 and 5 of Properties of the Absolute Value in an Ordered Field the combination then varies by less than ε \varepsilon ε . Hence G G G is continuous and, by The Viscous Hamilton-Jacobi Operator with a Drift that is One-Sided Lipschitz on Sublevel Sets Satisfies the Operator Hypotheses of the Weighted-Penalty Comparison Principle , F F F satisfies Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables §continuity , Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables §strictly-proper with γ = λ \gamma=\lambda γ = λ , Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables §convex and Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables §structure . In particular F F F is degenerate elliptic, by claim 1 of Strictly Proper Second-Order Equation Operator .
Step 7 (comparison; claim 2). Apply Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables with D = W N D=W_{N} D = W N , the penalty P P P of Step 1, w = 1 w=1 w = 1 and γ = λ \gamma=\lambda γ = λ ; its hypotheses 1 to 4 hold by Step 6, and hypothesis 5 by Step 5. Since 1 ⋅ P = P 1\cdot P=P 1 ⋅ P = P , the growth assumptions of claim 2 are exactly those on u − w P u-wP u − wP and v − w P v-wP v − wP , so u ( x ) ≤ v ( x ) u(x)\le v(x) u ( x ) ≤ v ( x ) for every x ∈ W N x\in W_{N} x ∈ W N .
Step 8 (a viscosity subsolution of weight 1 1 1 ). Let m m m be as in Basic Properties of the Sublevel Sets of a Penalty §bounded-below , so m ≤ P m\le P m ≤ P . Let F = { s P − K s : s 0 ≤ s < 1 } \mathcal{F}=\{sP-K_{s}:s_{0}\le s<1\} F = { s P − K s : s 0 ≤ s < 1 } , a nonempty set. Each member is of class C 2 C^{2} C 2 and a classical subsolution (Step 5), hence a viscosity subsolution by claim 1 of Classical Sub- and Supersolutions of a Degenerate Elliptic Operator are Viscosity Sub- and Supersolutions , F F F being degenerate elliptic (Step 6). For s 0 ≤ s < 1 s_{0}\le s<1 s 0 ≤ s < 1 we have 0 < 1 − s ≤ 1 0<1-s\le1 0 < 1 − s ≤ 1 , so for y ∈ W N y\in W_{N} y ∈ W N
P ( y ) − ( s P ( y ) − K s ) = ( 1 − s ) P ( y ) + K s ≥ ( 1 − s ) m ≥ − ∣ m ∣ ; P(y)-\bigl(sP(y)-K_{s}\bigr)=(1-s)P(y)+K_{s}\ge(1-s)m\ge-|m| ; P ( y ) − ( s P ( y ) − K s ) = ( 1 − s ) P ( y ) + K s ≥ ( 1 − s ) m ≥ − ∣ m ∣ ;
thus every v ∈ F v\in\mathcal{F} v ∈ F satisfies v ≤ P + ∣ m ∣ v\le P+|m| v ≤ P + ∣ m ∣ . Fix x ∈ W N x\in W_{N} x ∈ W N . By Continuity of the Value, Gradient and Hessian Maps of a Differentiable Function §value , P P P is continuous at x x x , so there is δ > 0 \delta>0 δ > 0 with P ( y ) < P ( x ) + 1 P(y)<P(x)+1 P ( y ) < P ( x ) + 1 whenever d E ( x , y ) < δ d_{E}(x,y)<\delta d E ( x , y ) < δ ; with r = δ 2 r=\tfrac{\delta}{2} r = 2 δ , every v ∈ F v\in\mathcal{F} v ∈ F satisfies v ( y ) ≤ P ( x ) + 1 + ∣ m ∣ v(y)\le P(x)+1+|m| v ( y ) ≤ P ( x ) + 1 + ∣ m ∣ whenever d E ( y , x ) ≤ r d_{E}(y,x)\le r d E ( y , x ) ≤ r . So F \mathcal{F} F is locally uniformly bounded above, and since F F F is continuous (Step 6), The Upper Semicontinuous Envelope of a Supremum of Viscosity Subsolutions is a Viscosity Subsolution shows that u ‾ = u ~ ∗ \underline{u}=\widetilde{u}^{*} u = u ∗ , where u ~ ( x ) = sup { v ( x ) : v ∈ F } \widetilde{u}(x)=\sup\{v(x):v\in\mathcal{F}\} u ( x ) = sup { v ( x ) : v ∈ F } , is a viscosity subsolution of F F F on W N W_{N} W N .
The function P + ∣ m ∣ P+|m| P + ∣ m ∣ is of class C 2 C^{2} C 2 by (c), hence continuous by Continuity of the Value, Gradient and Hessian Maps of a Differentiable Function §value , hence upper semicontinuous on W N W_{N} W N (claim 3 of Properties of the Absolute Value in an Ordered Field ). As u ~ ≤ P + ∣ m ∣ \widetilde{u}\le P+|m| u ≤ P + ∣ m ∣ , Properties of the Upper Semicontinuous Envelope §least gives u ‾ ≤ P + ∣ m ∣ \underline{u}\le P+|m| u ≤ P + ∣ m ∣ . Growth from above: for δ > 0 \delta>0 δ > 0 , δ P ≥ δ m ≥ − δ ∣ m ∣ \delta P\ge\delta m\ge-\delta|m| δ P ≥ δ m ≥ − δ ∣ m ∣ , so u ‾ − P ≤ ∣ m ∣ ≤ ( 1 + δ ) ∣ m ∣ + δ P \underline{u}-P\le|m|\le(1+\delta)|m|+\delta P u − P ≤ ∣ m ∣ ≤ ( 1 + δ ) ∣ m ∣ + δ P . Growth from below: by Properties of the Upper Semicontinuous Envelope §bounds , u ‾ ≥ u ~ ≥ s P − K s \underline{u}\ge\widetilde{u}\ge sP-K_{s} u ≥ u ≥ s P − K s for every s ∈ [ s 0 , 1 ) s\in[s_{0},1) s ∈ [ s 0 , 1 ) . If 0 < δ ≤ 1 − s 0 0<\delta\le1-s_{0} 0 < δ ≤ 1 − s 0 , take s = 1 − δ s=1-\delta s = 1 − δ : u ‾ − P ≥ − K 1 − δ − δ P \underline{u}-P\ge-K_{1-\delta}-\delta P u − P ≥ − K 1 − δ − δ P . If δ > δ 0 = 1 − s 0 \delta>\delta_{0}=1-s_{0} δ > δ 0 = 1 − s 0 , take s = s 0 s=s_{0} s = s 0 : u ‾ − P ≥ − K s 0 − δ 0 P = − K s 0 − δ P + ( δ − δ 0 ) P ≥ − ( K s 0 + ( δ − δ 0 ) ∣ m ∣ ) − δ P \underline{u}-P\ge-K_{s_{0}}-\delta_{0}P=-K_{s_{0}}-\delta P+(\delta-\delta_{0})P\ge-\bigl(K_{s_{0}}+(\delta-\delta_{0})|m|\bigr)-\delta P u − P ≥ − K s 0 − δ 0 P = − K s 0 − δ P + ( δ − δ 0 ) P ≥ − ( K s 0 + ( δ − δ 0 ) ∣ m ∣ ) − δ P . So u ‾ − P \underline{u}-P u − P has P P P -subordinate growth from above and from below .
Step 9 (a viscosity supersolution of weight 1 1 1 ). Let L = β n Π ( 2 θ ) − 1 > 0 L=\beta n_{\Pi}(2\theta)^{-1}>0 L = β n Π ( 2 θ ) − 1 > 0 , Λ = θ − 1 β n Π log 2 ≥ 0 \Lambda=\theta^{-1}\beta n_{\Pi}\log2\ge0 Λ = θ − 1 β n Π log 2 ≥ 0 (by (b4)),
K ′ = λ − 1 ( λ Λ + ( a + L ) β d N + κ ( a + L ) N R + M ) ≥ 0 , u ‾ = P + L l + K ′ . K'=\lambda^{-1}\bigl(\lambda\Lambda+(a+L)\beta d_{N}+\kappa(a+L)N_{\mathbb{R}}+M\bigr)\ge0,\qquad \overline{u}=P+L\,l+K' . K ′ = λ − 1 ( λ Λ + ( a + L ) β d N + κ ( a + L ) N R + M ) ≥ 0 , u = P + L l + K ′ .
Derivatives of l l l . The set V = ( 0 , ∞ ) V=(0,\infty) V = ( 0 , ∞ ) is open in R 1 \mathbb{R}^{1} R 1 and q ( x ) ∈ V q(x)\in V q ( x ) ∈ V for x ∈ W N x\in W_{N} x ∈ W N . By The Natural Logarithm , log \log log is smooth on V V V with derivative ρ ( t ) = t − 1 \rho(t)=t^{-1} ρ ( t ) = t − 1 ; ρ = ∂ 1 log \rho=\partial_{1}\log ρ = ∂ 1 log is smooth on V V V by claim 3 of Coordinate Functions, the C k C^k C k Hierarchy, and Partial Derivatives of a Smooth Map , and ∂ 1 ρ ( t ) = − ( t − 1 ) 2 \partial_{1}\rho(t)=-(t^{-1})^{2} ∂ 1 ρ ( t ) = − ( t − 1 ) 2 by claim 2 of Reciprocal Rule for One-Dimensional Derivatives (for a function of one variable on an open interval, the limit defining the partial derivative in Partial Derivative on a Euclidean Open Set is the one defining the derivative in Derivative at an Interior Point ). By claims 1 and 2 of A Composition of C k C^k C k Maps Between Euclidean Open Sets is of Class C k C^k C k (smooth maps being of class C k C^{k} C k for every k k k by Smooth Map on a Euclidean Open Set ) and Step 0(d), l = log ∘ q l=\log\circ q l = log ∘ q is of class C 2 C^{2} C 2 on W N W_{N} W N with ∂ i l = ( ρ ∘ q ) ∂ i q \partial_{i}l=(\rho\circ q)\,\partial_{i}q ∂ i l = ( ρ ∘ q ) ∂ i q , i.e. D l ( x ) = 2 q ( x ) − 1 x Dl(x)=2q(x)^{-1}x D l ( x ) = 2 q ( x ) − 1 x ; and ρ ∘ q \rho\circ q ρ ∘ q is of class C 1 C^{1} C 1 with ∂ i ( ρ ∘ q ) ( x ) = − q ( x ) − 2 2 x i \partial_{i}(\rho\circ q)(x)=-q(x)^{-2}\,2x_{i} ∂ i ( ρ ∘ q ) ( x ) = − q ( x ) − 2 2 x i . By the product rule (claim 1 of Constants, Coordinate Functions, Sums and Products of C k C^k C k Functions on a Euclidean Open Set ) and ∂ i ∂ i q = 2 \partial_{i}\partial_{i}q=2 ∂ i ∂ i q = 2 (Step 0(d), Hessian Matrix of a C^2 Function , Identity Matrix ),
∂ i ∂ i l ( x ) = 2 q ( x ) − 1 − 4 q ( x ) − 2 x i 2 , tr ( D 2 l ( x ) ) = 2 q ( x ) − 1 N R − 4 q ( x ) − 2 ∥ x ∥ 2 ≤ 2 N R , \partial_{i}\partial_{i}l(x)=2q(x)^{-1}-4q(x)^{-2}x_{i}^{2},\qquad \operatorname{tr}\bigl(D^{2}l(x)\bigr)=2q(x)^{-1}N_{\mathbb{R}}-4q(x)^{-2}\lVert x\rVert^{2}\le2N_{\mathbb{R}}, ∂ i ∂ i l ( x ) = 2 q ( x ) − 1 − 4 q ( x ) − 2 x i 2 , tr ( D 2 l ( x ) ) = 2 q ( x ) − 1 N R − 4 q ( x ) − 2 ∥ x ∥ 2 ≤ 2 N R ,
by Trace of a Real Square Matrix , claims 2 and 3 of Properties of Finite Sums , claim 1 of Elementary Properties of the Euclidean Norm on R n \mathbb{R}^n R n and Step 0(a).
Supersolution. By (c), u ‾ \overline{u} u is of class C 2 C^{2} C 2 with D u ‾ = D P + L D l D\overline{u}=DP+L\,Dl D u = D P + L D l and D 2 u ‾ = D 2 P + L D 2 l D^{2}\overline{u}=D^{2}P+L\,D^{2}l D 2 u = D 2 P + L D 2 l . Expanding ∥ D P + L D l ∥ 2 \lVert DP+L\,Dl\rVert^{2} ∥ D P + L D l ∥ 2 by (c) and using Step 3 with s = 1 s=1 s = 1 , k = K ′ k=K' k = K ′ and e ( 1 ) = f ( 1 ) = 0 e(1)=f(1)=0 e ( 1 ) = f ( 1 ) = 0 ,
F [ u ‾ ] ( x ) = λ θ − 1 H − a β d N − κ a N R + λ K ′ − g + λ L l + θ L D P ⋅ D l + θ 2 L 2 ∥ D l ∥ 2 − κ 2 L tr ( D 2 l ) , F[\overline{u}](x)=\lambda\theta^{-1}H-a\beta d_{N}-\kappa aN_{\mathbb{R}}+\lambda K'-g+\lambda L\,l+\theta L\,DP\cdot Dl+\tfrac{\theta}{2}L^{2}\lVert Dl\rVert^{2}-\tfrac{\kappa}{2}L\operatorname{tr}(D^{2}l), F [ u ] ( x ) = λ θ − 1 H − a β d N − κa N R + λ K ′ − g + λ L l + θ L D P ⋅ D l + 2 θ L 2 ∥ D l ∥ 2 − 2 κ L tr ( D 2 l ) ,
all functions evaluated at x x x . By (L), θ − 1 H ≥ − Λ − L l \theta^{-1}H\ge-\Lambda-L\,l θ − 1 H ≥ − Λ − L l , so λ θ − 1 H + λ L l ≥ − λ Λ \lambda\theta^{-1}H+\lambda L\,l\ge-\lambda\Lambda λ θ − 1 H + λ L l ≥ − λ Λ . By Step 2, Bilinearity and Symmetry of the Dot Product on R n \mathbb{R}^n R n and The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §euler ,
D P ⋅ D l = 2 q − 1 θ − 1 D H ⋅ x + 4 a q − 1 ∥ x ∥ 2 = − q − 1 θ − 1 β d N + 4 a q − 1 ∥ x ∥ 2 ≥ − θ − 1 β d N , DP\cdot Dl=2q^{-1}\theta^{-1}DH\cdot x+4aq^{-1}\lVert x\rVert^{2}=-q^{-1}\theta^{-1}\beta d_{N}+4aq^{-1}\lVert x\rVert^{2}\ge-\theta^{-1}\beta d_{N}, D P ⋅ D l = 2 q − 1 θ − 1 DH ⋅ x + 4 a q − 1 ∥ x ∥ 2 = − q − 1 θ − 1 β d N + 4 a q − 1 ∥ x ∥ 2 ≥ − θ − 1 β d N ,
since 0 < q − 1 ≤ 1 0<q^{-1}\le1 0 < q − 1 ≤ 1 and 0 ≤ d N 0\le d_{N} 0 ≤ d N ; so θ L D P ⋅ D l ≥ − L β d N \theta L\,DP\cdot Dl\ge-L\beta d_{N} θ L D P ⋅ D l ≥ − L β d N . Also θ 2 L 2 ∥ D l ∥ 2 ≥ 0 \tfrac{\theta}{2}L^{2}\lVert Dl\rVert^{2}\ge0 2 θ L 2 ∥ D l ∥ 2 ≥ 0 , − κ 2 L tr ( D 2 l ) ≥ − κ L N R -\tfrac{\kappa}{2}L\operatorname{tr}(D^{2}l)\ge-\kappa LN_{\mathbb{R}} − 2 κ L tr ( D 2 l ) ≥ − κ L N R and − g ≥ − M -g\ge-M − g ≥ − M . Therefore
F [ u ‾ ] ( x ) ≥ − λ Λ − ( a + L ) β d N − κ ( a + L ) N R − M + λ K ′ = 0 , F[\overline{u}](x)\ge-\lambda\Lambda-(a+L)\beta d_{N}-\kappa(a+L)N_{\mathbb{R}}-M+\lambda K'=0 , F [ u ] ( x ) ≥ − λ Λ − ( a + L ) β d N − κ ( a + L ) N R − M + λ K ′ = 0 ,
so u ‾ \overline{u} u is a classical supersolution, hence a viscosity supersolution by claim 2 of Classical Sub- and Supersolutions of a Degenerate Elliptic Operator are Viscosity Sub- and Supersolutions .
Weight. u ‾ − P = L l + K ′ \overline{u}-P=L\,l+K' u − P = L l + K ′ . From below: for δ > 0 \delta>0 δ > 0 , − δ ∣ m ∣ − δ P ≤ 0 ≤ L l + K ′ -\delta|m|-\delta P\le0\le L\,l+K' − δ ∣ m ∣ − δ P ≤ 0 ≤ L l + K ′ by (b3). From above: fix δ > 0 \delta>0 δ > 0 and let η = δ a ( ( 1 + δ ) L ) − 1 > 0 \eta=\delta a\bigl((1+\delta)L\bigr)^{-1}>0 η = δ a ( ( 1 + δ ) L ) − 1 > 0 . The upper bound of (b) at η q ( x ) \eta q(x) η q ( x ) gives log η + l ( x ) ≤ η q ( x ) − 1 \log\eta+l(x)\le\eta q(x)-1 log η + l ( x ) ≤ η q ( x ) − 1 , hence
( 1 + δ ) L l ( x ) ≤ δ a ∥ x ∥ 2 + δ a + ( 1 + δ ) L ∣ 1 + log η ∣ . (1+\delta)L\,l(x)\le\delta a\lVert x\rVert^{2}+\delta a+(1+\delta)L\,|1+\log\eta| . ( 1 + δ ) L l ( x ) ≤ δ a ∥ x ∥ 2 + δ a + ( 1 + δ ) L ∣1 + log η ∣.
By (L), a ∥ x ∥ 2 = P ( x ) − θ − 1 H ( x ) ≤ P ( x ) + Λ + L l ( x ) a\lVert x\rVert^{2}=P(x)-\theta^{-1}H(x)\le P(x)+\Lambda+L\,l(x) a ∥ x ∥ 2 = P ( x ) − θ − 1 H ( x ) ≤ P ( x ) + Λ + L l ( x ) , so δ a ∥ x ∥ 2 ≤ δ P ( x ) + δ Λ + δ L l ( x ) \delta a\lVert x\rVert^{2}\le\delta P(x)+\delta\Lambda+\delta L\,l(x) δ a ∥ x ∥ 2 ≤ δ P ( x ) + δ Λ + δ L l ( x ) . Combining and subtracting δ L l ( x ) \delta L\,l(x) δ L l ( x ) ,
u ‾ ( x ) − P ( x ) ≤ ( δ Λ + δ a + ( 1 + δ ) L ∣ 1 + log η ∣ + K ′ ) + δ P ( x ) . \overline{u}(x)-P(x)\le\bigl(\delta\Lambda+\delta a+(1+\delta)L|1+\log\eta|+K'\bigr)+\delta P(x). u ( x ) − P ( x ) ≤ ( δ Λ + δ a + ( 1 + δ ) L ∣1 + log η ∣ + K ′ ) + δ P ( x ) .
So u ‾ − P \overline{u}-P u − P has P P P -subordinate growth from above and from below.
Step 10 (existence and uniqueness; claim 3). Apply Perron's Method with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables: Existence and Uniqueness of a Viscosity Solution of Given Weight with D = W N D=W_{N} D = W N (open and nonempty), the penalty P P P , w = 1 w=1 w = 1 and γ = λ \gamma=\lambda γ = λ : its operator hypotheses hold by Step 6 and its barrier by Step 5 (s 0 < 1 s_{0}<1 s 0 < 1 ). Since 1 ⋅ P = P 1\cdot P=P 1 ⋅ P = P , a function f f f is of weight 1 1 1 in the sense of that theorem exactly when f − P f-P f − P has P P P -subordinate growth from above and from below; so u ‾ \underline{u} u (Step 8) and u ‾ \overline{u} u (Step 9) are a viscosity subsolution and a viscosity supersolution of weight 1 1 1 . By Perron's Method with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables: Existence and Uniqueness of a Viscosity Solution of Given Weight §existence there is a function u u u with the properties of claim 3, by Perron's Method with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables: Existence and Uniqueness of a Viscosity Solution of Given Weight §uniqueness any two such functions are equal, and by Perron's Method with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables: Existence and Uniqueness of a Viscosity Solution of Given Weight §continuity it is continuous on W N W_{N} W N . This proves claim 3.