赋权二叉树:修订间差异
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上述这些都跟ε(0)以下的tree相同 | 上述这些都跟ε(0)以下的tree相同 | ||
* [] = ε(0) | |||
* ([]) = ε(0)+1 | |||
* (([])) = ε(0)+2 | |||
* ([])() = ε(0)+ω | |||
* ([])([]) = ε(0)·2 | |||
* (([]))([]) = ε(0)·3 | |||
* (([])())([]) = ε(0)·ω | |||
* (([])([]))([]) = ε(0)^2 | |||
* (([]))(([])) = ε(0)^ω | |||
* (([])([]))(([])([])) = ε(0)^ε(0) | |||
* []() = ε(1) | |||
* [](()) = ε(2) | |||
* [](()()) = ε(ω) | |||
* []([]) = ε(ε(0)) | |||
* []([]([])) = ε(ε(ε(0))) | |||
* [()] = ζ(0) | |||
* ([()]) = ζ(0)+1 | |||
* ([()])([()]) = ζ(0)·2 | |||
* []([()]) = ε(ζ(0)+1) | |||
* [](([()])) = ε(ζ(0)+2) | |||
* []([]([()])) = ε(ε(ζ(0)+1)) | |||
* [()]() = ζ(1) | |||
* [()]([()]) = ζ(ζ(0)) | |||
* [(())] = ϑ(Ω·3) = φ(3,0) | |||
* []([(())]) = ϑ(Ω+ϑ(Ω·3)) | |||
* [()]([(())]) = ϑ(Ω·2+ϑ(Ω·3)) | |||
* [(())]() = ϑ(Ω·3+1) | |||
* [((()))] = ϑ(Ω·4) | |||
* [()()] = ϑ(Ω·ω) | |||
* [(()())] = ϑ(Ω·(ω+1)) | |||
* [(()())(()())] = ϑ(Ω·ω^ω^ω) | |||
* [([])] = ϑ(Ω·ϑ(Ω)) | |||
* [([])]() = ϑ(Ω·ϑ(Ω)+1) | |||
* [(([]))] = ϑ(Ω·(ϑ(Ω)+1)) | |||
* [([])([])] = ϑ(Ω·ϑ(Ω)·2) | |||
* [([]())] = ϑ(Ω·ϑ(Ω+1)) | |||
* [([()])] = ϑ(Ω·ϑ(Ω·2)) | |||
* [([([])])] = ϑ(Ω·ϑ(Ω·ϑ(Ω))) | |||
* [[]] = ϑ(Ω^2) = Γ(0) | |||
* []([[]]) = ϑ(Ω+ϑ(Ω^2)) | |||
* [()]([[]]) = ϑ(Ω·2+ϑ(Ω^2)) | |||
* [([[]])] = ϑ(Ω·ϑ(Ω^2)) | |||
* [([([[]])])] = ϑ(Ω·ϑ(Ω·ϑ(Ω^2))) | |||
* [[]]() = ϑ(Ω^2+1) | |||
* [[]]([[]]) = ϑ(Ω^2+ϑ(Ω^2)) | |||
* [[]()] = ϑ(Ω^2+Ω) | |||
* [[]([[]])] = ϑ(Ω^2+Ω·ϑ(Ω^2)) | |||
* <nowiki>[[()]]</nowiki>= ϑ(Ω^2·2) | |||
* [[([[]])]] = ϑ(Ω^2·ϑ(Ω^2)) | |||
* [[[]]] = ϑ(Ω^3) | |||
* [[[]]]() = ϑ(Ω^3+1) | |||
* [[[]]()] = ϑ(Ω^3+Ω) | |||
* [[[]()]] = ϑ(Ω^3+Ω^2) | |||
* [[[()]]] = ϑ(Ω^3·2) | |||
* [[[[]]]] = ϑ(Ω^4) | |||
* [][] = ϑ(Ω^ω) | |||
* ([][]) = ϑ(Ω^ω)+1 | |||
* []([][]) = ϑ(Ω+ϑ(Ω^ω)) | |||
* [([][])] = ϑ(Ω·ϑ(Ω^ω)) | |||
* [[([][])]] = ϑ(Ω^2·ϑ(Ω^ω)) | |||
* [[][]] = ϑ(Ω^ω+1) | |||
* [[][]]() = ϑ(Ω^ω+2) | |||
* [[][]]([][]) = ϑ(Ω^ω+ϑ(Ω^ω)) | |||
* [[[][]]] = ϑ(Ω^ω+Ω) | |||
* [[[][]]]() = ϑ(Ω^ω+Ω+1) | |||
* [[[][]]()] = ϑ(Ω^ω+Ω·2) | |||
* [[[[][]]]] = ϑ(Ω^ω+Ω^2) | |||
* [[[[[][]]]]] = ϑ(Ω^ω+Ω^3) | |||
* [()][] = ϑ(Ω^ω·2) | |||
* [[()][]] = ϑ(Ω^ω·2+1) | |||
* [[[()][]]] = ϑ(Ω^ω·2+Ω) | |||
* [[[[()][]]]] = ϑ(Ω^ω·2+Ω^2) | |||
* [(())][] = ϑ(Ω^ω·3) | |||
* [([][])][] = ϑ(Ω^ω·ϑ(Ω^ω)) | |||
* [[]][] = ϑ(Ω^(ω+1)) | |||
* [[[]]][] = ϑ(Ω^(ω+2)) | |||
* [[][]][] = ϑ(Ω^(ω·2)) | |||
* [[[][]][]] = ϑ(Ω^(ω·2)+1) | |||
* [[[[][]][]]] = ϑ(Ω^(ω·2)+Ω) | |||
* [[[][]]][] = ϑ(Ω^(ω·2)+Ω^ω) | |||
* [[[][]]()][] = ϑ(Ω^(ω·2)+Ω^ω·2) | |||
* [[[[][]]]][] = ϑ(Ω^(ω·2)+Ω^(ω+1)) | |||
* [[()][]][] = ϑ(Ω^(ω·2)·2) | |||
* [[[]][]][] = ϑ(Ω^(ω·2+1)) | |||
* [[[][]][]][] = ϑ(Ω^(ω·3)) | |||
* [[[[][]][]][]][] = ϑ(Ω^(ω·4)) | |||
* [()][()] = ϑ(Ω^ω^2) | |||
* [[()][()]] = ϑ(Ω^ω^2+1) | |||
* [[[()][()]][]] = ϑ(Ω^ω^2+Ω^ω) | |||
* [(())][()] = ϑ(Ω^ω^2·2) | |||
* [[]][()] = ϑ(Ω^(ω^2+1)) | |||
* [[()][()]][()] = ϑ(Ω^(ω^2·2)) | |||
* [(())][(())] = ϑ(Ω^ω^3) | |||
* [([])][([])] = ϑ(Ω^ϑ(Ω)) | |||
* [[]][[]] = ϑ(Ω^Ω) = LVO | |||
看上去[]可以作为Ω的角色了,这样只使用权重1~2就能达到至少BHO的序型 | 看上去[]可以作为Ω的角色了,这样只使用权重1~2就能达到至少BHO的序型 | ||
2026年2月21日 (六) 16:11的版本
赋权二叉树(Weighted Binary Tree)是FataliS1024提出的大数函数。
定义
对于有根二叉树,令其每条边都有一个正整数权值,即得到赋权二叉树,记作wb
对于两个wb A和B,如果A能通过以下操作得到B,就称B嵌入A,A容纳B,A大于B,B小于A:
- 删掉一个度为1的顶点和它连接的边
- 删掉一个度为2的非根顶点和它连接的两条边,并将它原本连接的两个顶点连起来,权值等于min(原来两条边的权值)
- 将任意一个大于1的权值-1
符合以下条件的最长的有序wb列的长度记作wbtree(n):
- 第k个wb最多有k+1个顶点
- 所有wb的边权值不超过n
- 前面的wb不小于后面的wb
分析
用()表示权值1的边与它的子节点(远离根的一端)。用[]表示权值2。{}表示权值3.根节点不写
以下提供了wbtree中的一个序型分析
- 单根=0
- () = 1
- (()) = 2
- ()() = ω
上述这些都跟ε(0)以下的tree相同
- [] = ε(0)
- ([]) = ε(0)+1
- (([])) = ε(0)+2
- ([])() = ε(0)+ω
- ([])([]) = ε(0)·2
- (([]))([]) = ε(0)·3
- (([])())([]) = ε(0)·ω
- (([])([]))([]) = ε(0)^2
- (([]))(([])) = ε(0)^ω
- (([])([]))(([])([])) = ε(0)^ε(0)
- []() = ε(1)
- [](()) = ε(2)
- [](()()) = ε(ω)
- []([]) = ε(ε(0))
- []([]([])) = ε(ε(ε(0)))
- [()] = ζ(0)
- ([()]) = ζ(0)+1
- ([()])([()]) = ζ(0)·2
- []([()]) = ε(ζ(0)+1)
- [](([()])) = ε(ζ(0)+2)
- []([]([()])) = ε(ε(ζ(0)+1))
- [()]() = ζ(1)
- [()]([()]) = ζ(ζ(0))
- [(())] = ϑ(Ω·3) = φ(3,0)
- []([(())]) = ϑ(Ω+ϑ(Ω·3))
- [()]([(())]) = ϑ(Ω·2+ϑ(Ω·3))
- [(())]() = ϑ(Ω·3+1)
- [((()))] = ϑ(Ω·4)
- [()()] = ϑ(Ω·ω)
- [(()())] = ϑ(Ω·(ω+1))
- [(()())(()())] = ϑ(Ω·ω^ω^ω)
- [([])] = ϑ(Ω·ϑ(Ω))
- [([])]() = ϑ(Ω·ϑ(Ω)+1)
- [(([]))] = ϑ(Ω·(ϑ(Ω)+1))
- [([])([])] = ϑ(Ω·ϑ(Ω)·2)
- [([]())] = ϑ(Ω·ϑ(Ω+1))
- [([()])] = ϑ(Ω·ϑ(Ω·2))
- [([([])])] = ϑ(Ω·ϑ(Ω·ϑ(Ω)))
- [[]] = ϑ(Ω^2) = Γ(0)
- []([[]]) = ϑ(Ω+ϑ(Ω^2))
- [()]([[]]) = ϑ(Ω·2+ϑ(Ω^2))
- [([[]])] = ϑ(Ω·ϑ(Ω^2))
- [([([[]])])] = ϑ(Ω·ϑ(Ω·ϑ(Ω^2)))
- [[]]() = ϑ(Ω^2+1)
- [[]]([[]]) = ϑ(Ω^2+ϑ(Ω^2))
- [[]()] = ϑ(Ω^2+Ω)
- [[]([[]])] = ϑ(Ω^2+Ω·ϑ(Ω^2))
- [[()]]= ϑ(Ω^2·2)
- [[([[]])]] = ϑ(Ω^2·ϑ(Ω^2))
- [[[]]] = ϑ(Ω^3)
- [[[]]]() = ϑ(Ω^3+1)
- [[[]]()] = ϑ(Ω^3+Ω)
- [[[]()]] = ϑ(Ω^3+Ω^2)
- [[[()]]] = ϑ(Ω^3·2)
- [[[[]]]] = ϑ(Ω^4)
- [][] = ϑ(Ω^ω)
- ([][]) = ϑ(Ω^ω)+1
- []([][]) = ϑ(Ω+ϑ(Ω^ω))
- [([][])] = ϑ(Ω·ϑ(Ω^ω))
- [[([][])]] = ϑ(Ω^2·ϑ(Ω^ω))
- [[][]] = ϑ(Ω^ω+1)
- [[][]]() = ϑ(Ω^ω+2)
- [[][]]([][]) = ϑ(Ω^ω+ϑ(Ω^ω))
- [[[][]]] = ϑ(Ω^ω+Ω)
- [[[][]]]() = ϑ(Ω^ω+Ω+1)
- [[[][]]()] = ϑ(Ω^ω+Ω·2)
- [[[[][]]]] = ϑ(Ω^ω+Ω^2)
- [[[[[][]]]]] = ϑ(Ω^ω+Ω^3)
- [()][] = ϑ(Ω^ω·2)
- [[()][]] = ϑ(Ω^ω·2+1)
- [[[()][]]] = ϑ(Ω^ω·2+Ω)
- [[[[()][]]]] = ϑ(Ω^ω·2+Ω^2)
- [(())][] = ϑ(Ω^ω·3)
- [([][])][] = ϑ(Ω^ω·ϑ(Ω^ω))
- [[]][] = ϑ(Ω^(ω+1))
- [[[]]][] = ϑ(Ω^(ω+2))
- [[][]][] = ϑ(Ω^(ω·2))
- [[[][]][]] = ϑ(Ω^(ω·2)+1)
- [[[[][]][]]] = ϑ(Ω^(ω·2)+Ω)
- [[[][]]][] = ϑ(Ω^(ω·2)+Ω^ω)
- [[[][]]()][] = ϑ(Ω^(ω·2)+Ω^ω·2)
- [[[[][]]]][] = ϑ(Ω^(ω·2)+Ω^(ω+1))
- [[()][]][] = ϑ(Ω^(ω·2)·2)
- [[[]][]][] = ϑ(Ω^(ω·2+1))
- [[[][]][]][] = ϑ(Ω^(ω·3))
- [[[[][]][]][]][] = ϑ(Ω^(ω·4))
- [()][()] = ϑ(Ω^ω^2)
- [[()][()]] = ϑ(Ω^ω^2+1)
- [[[()][()]][]] = ϑ(Ω^ω^2+Ω^ω)
- [(())][()] = ϑ(Ω^ω^2·2)
- [[]][()] = ϑ(Ω^(ω^2+1))
- [[()][()]][()] = ϑ(Ω^(ω^2·2))
- [(())][(())] = ϑ(Ω^ω^3)
- [([])][([])] = ϑ(Ω^ϑ(Ω))
- [[]][[]] = ϑ(Ω^Ω) = LVO
看上去[]可以作为Ω的角色了,这样只使用权重1~2就能达到至少BHO的序型
- ψ(Ω₂)={}
- ψ(Ω₂+Ω)=[{}]
- ψ(Ω₂+Ω^Ω^ω)=[{}][]
- ψ(Ω₂+ψ₁(Ω₂))=[{}][{}]
- ψ(Ω₂+ψ₁(Ω₂)+Ω)=[{}][[{}]]
- ψ(Ω₂+ψ₁(Ω₂)×2)=[{}][[{}][{}]]
- ψ(Ω₂+ψ₁(Ω₂)×3)=[{}][[{}][[{}][{}]]]
- ψ(Ω₂+ψ₁(Ω₂+1))=[[{}]][[{}]]
- ψ(Ω₂+ψ₁(Ω₂+2))=[[[{}]]][[[{}]]]
- ψ(Ω₂+ψ₁(Ω₂+ω))=[[{}]()][[{}]()]
- ψ(Ω₂+ψ₁(Ω₂+Ω))=[[{}][]][[{}][]]
- ψ(Ω₂+ψ₁(Ω₂+ψ₁(Ω₂)))=[[{}][{}]][[{}][{}]]
- ψ(Ω₂+ψ₁(Ω₂+ψ₁(Ω₂+ψ₁(Ω₂))))=[[[{}][{}]][[{}][{}]]][[[{}][{}]][[{}][{}]]]
- ψ(Ω₂×2)={}()
- ψ(Ω₂×ω)={}(()())
- ψ(Ω₂×Ω)={}[]
- ψ(Ω₂×ψ₁(Ω₂))={}[{}]
- ψ(Ω₂×ψ₁(Ω₂×ψ₁(Ω₂)))={}[{}[{}]]
- ψ(Ω₂²)={()}
- ψ(Ω₂^ω)={()()}
- ψ(Ω₂^Ω)={[]}
- ψ(Ω₂^Ω₂)={{}}
- ψ(Ω₂^Ω₂³)={{{{}}}}
- ψ(Ω₂^Ω₂^ω)={}{}
- ψ(Ω₂^Ω₂^Ω)={[]}{[]}
- ψ(Ω₂^Ω₂^Ω₂)={{}}{{}}
- ψ(Ω₂^Ω₂^Ω₂^ω)={{}{}}{{}{}}
于是得到ψ(Ω_ω)=极限