フック長の公式のソースを表示

{{翻訳中途|1=[https://en.wikipedia.org/w/index.php?title=Hook_length_formula&oldid=887586402 英語版 "Hook length formula" 15:49, 13 March 2019 (UTC)]|date=2019年4月}}
[[数学]]の[[組合せ論]]において、'''フック長の公式'''（フックちょうのこうしき、{{lang-en|Hook length formula}}）とは、与えられた[[ヤング図形]]の形をした[[ヤング図形#ヤング盤|標準盤]]を数える公式である。[[表現論]]や、[[確率論]]、[[アルゴリズム解析]]などの多種多様な分野に応用があり、{{仮リンク|最長増加部分列問題|en|Longest increasing subsequence}}などが例としてあげられる。
== Definitions and statement ==
Let <math>\lambda=(\lambda_1,\ldots,\lambda_m)</math> be a [[Partition (number theory)|partition]] of <math>n</math>. It is customary to interpret <math>\lambda</math> graphically as a [[Young diagram]], namely a left-justified array of square cells with <math>m</math> rows and <math>\lambda_i</math> cells in the <math>i</math>th row for each <math>1\le i\le m</math>. A [[Young tableau|standard Young tableau]] of shape <math>\lambda</math> is a Young diagram of shape <math>\lambda</math> in which each of the <math>n</math> cells contains a distinct integer between 1 and <math>n</math> (i.e., no repetition), such that each row and each column form increasing [[Sequence|sequences]]. For each cell of the Young diagram in coordinates <math>(i,j)</math> (that is, the cell in the <math>i</math>th row and <math>j</math>th column), the '''hook''' <math>H_\lambda(i,j)</math> is the [[Set (mathematics)|set]] of cells <math>(a,b)</math> such that <math>a=i</math> and <math>b \ge j</math> or <math>a \ge i</math> and <math>b=j</math>. The hook-length <math>h_\lambda(i,j)</math> is the number of cells in the hook <math>H_\lambda(i,j)</math>.

Then the hook-length formula expresses the number of standard Young tableaux of shape <math>\lambda</math>, sometimes denoted by <math>d_\lambda</math>, as

: <math> d_\lambda = \frac{n!}{\prod h_\lambda (i,j)} , </math>

where the product is over all cells <math>(i,j)</math> of <math>\lambda</math>.

== Example ==
[[ファイル:Hook-length_tableau_December_8_2013_3.jpg|右|サムネイル|A tableau listing the hook length of each cell in the Young diagram <math>(4, 3, 1, 1)</math>]]
The figure on the right shows hook-lengths for all cells in the [[Young diagram]] {{math|''λ''}} of the partition 

9 = 4 + 3 + 1 + 1. Then the number of standard [[Young tableaux]] <math>d_\lambda</math> for this Young diagram can be computed as

: <math>d_\lambda = \frac{9!}{7\cdot 5\cdot 4\cdot 3\cdot 2\cdot 2\cdot 1\cdot 1\cdot 1} = 216.</math>

== History ==
There are other formulas for <math>d_\lambda</math>, but the hook-length formula is particularly simple and elegant. The hook-length formula was discovered in 1954 by J. S. Frame, [[Gilbert de Beauregard Robinson|G. de B. Robinson]], and R. M. Thrall by improving a less convenient formula expressing <math>d_\lambda</math> in terms of a [[determinant]]. <ref>Frame, J. S., Robinson, G. de B. and Thrall, R. M. (1954). The hook graphs of the symmetric group. Can. J. Math. 6, 316–325.</ref> This earlier formula was deduced independently by [[Ferdinand Georg Frobenius|G. Frobenius]] and [[Alfred Young|A. Young]] in 1900 and 1902 respectively using algebraic methods. <ref>G. Frobenius. Uber die charaktere der symmetrischer gruppe, Preuss. &ad. Wk. sitz. (1900), 516–534.</ref> <ref>A. Young. Quantitative substitutional analysis II, Proc. London Math. Sot., Ser. 1, 35 (1902), 361–397.</ref> [[Percy Alexander MacMahon|P. A. MacMahon]] found an alternate proof for the Young–Frobenius formula in 1916 using difference methods. <ref>P. A. MacMahon. “Combinatory Analysis,” Cambridge Univ. Press, London/New York, 1916; reprinted by Chelsea, New York, 1960.</ref>

Despite the simplicity of the hook-length formula, the Frame–Robinson–Thrall proof is uninsightful and does not provide an intuitive argument as to why hooks appear in the formula. The search for a short, intuitive explanation befitting such a simple result gave rise to many alternate proofs for the hook-length formula. <ref>Knuth, Donald (1973). The Art of Computer Programming, Volume 3: Sorting and Searching, 3rd Edition, Addison–Wesley, p. 63</ref> A. P. Hillman and R. M. Grassl gave the first proof that illuminates the role of hooks in 1976 by proving a special case of the [[Richard P. Stanley|Stanley]] hook-content formula, which is known to imply the hook-length formula. <ref>A. P. Hillman and R. M. Grassl. Reverse plane partitions and tableau hook numbers, J. Comb. Theory, Ser. A 21 (1976), 216–221.</ref> [[Curtis Greene|C. Greene]], [[Albert Nijenhuis|A. Nijenhuis]], and [[Herbert S. Wilf|H. S. Wilf]] found a probabilistic proof using the hook walk in which the hook lengths appear naturally in 1979. <ref name="#1">Greene, C., Nijenhuis, A. and Wilf, H. S. (1979). A probabilistic proof of a formula for the number of Young tableaux of a given shape. Adv. in Math. 31, 104–109.</ref> J. B. Remmel adapted the original Frame–Robinson–Thrall proof into the first bijective proof for the hook-length formula in 1982. <ref>J. B. Remmel. Bijective proofs of formulae for the number of standard Young tableaux, Linear and Multilinear Algebra 11 (1982), 45–100.</ref> A direct bijective proof was first discovered by D. S. Franzblau and [[Doron Zeilberger|D. Zeilberger]] in 1982. <ref>Franzblau, D. S. and Zeilberger, D. (1982). A bijective proof of the hook-length formula. J. Algorithms 3, 317–343.</ref> [[Doron Zeilberger|D. Zeilberger]] also converted the Greene–Nijenhuis–Wilf hook walk proof into a bijective proof in 1984. <ref>D. Zeilberger. A short hook-lengths bijection inspired by the Greene–Nijenhuis–Wilf proof, Discrete Math. 51 (1984), 101–108.</ref> A simpler direct bijective proof was announced by [[Igor Pak]] and Alexander V. Stoyanovskii in 1992, and its complete proof was presented by the pair and Jean-Christophe Novelli in 1997. <ref>Pak, I. M. and Stoyanovskii, A. V. (1992). A bijective proof of the hook-length formula. Funct. Anal. Appl. 24.</ref> <ref>Novelli, J.-C., Pak, I. M. and Stoyanovskii, A. V. (1997). A direct bijective proof of the hook-length formula. Discrete Mathematics and Theoretical Computer Science 1, 1997, 53–67.</ref>

Meanwhile, the hook-length formula has been generalized in several ways. R. M. Thrall found the analogue to the hook-length formula for shifted Young Tableaux in 1952. <ref>R. M. Thrall. A combinatorial problem, Michigan Math. J. 1 (1952), 81–88.</ref> [[Bruce Sagan|B. E. Sagan]] gave a shifted hook walk proof for the hook-length formula for shifted Young tableaux in 1980. <ref>Sagan, B. On selecting a random shifted Young tableau. J. Algorithms 1, 3 (1980), 213–234.</ref> B. E. Sagan and Y. N. Yeh proved the hook-length formula for binary trees using the hook walk in 1989. <ref>Sagan, B. E., and Yeh, Y. N. Probabilistic algorithms for trees. Fibonacci Quart. 27, 3 (1989), 201–208.</ref>

== Proofs ==

=== Knuth's heuristic argument ===
The hook-length formula can be understood intuitively using the following heuristic, but incorrect, argument suggested by [[Donald Knuth|D. E. Knuth]].<ref>{{citation|title=The Art of Computer Programming, Volume 3: Sorting and Searching, 3rd Edition|first=Donald|last=Knuth|publisher=Addison–Wesley|year=1973|isbn=0-201-03803-X|page=63}}.</ref> Given that each element of a tableau is the smallest in its hook and filling the tableau shape at random, the probability that cell <math>(i,j)</math> will contain the minimum element of the corresponding hook is the reciprocal of the hook length.  Multiplying these probabilities over all <math>i</math> and <math>j</math> gives the formula. This argument is fallacious since the events are not independent.

Knuth's argument is however correct for the enumeration of labellings on trees satisfying monotonicity properties analogous to those of a Young tableau. In this case, the 'hook' events in question are in fact independent events.

=== フックウォークを用いた確率論的証明法 ===
これは1979年に、  [[Curtis Greene|C. Greene]], [[Albert Nijenhuis|A. Nijenhuis]] と [[Herbert S. Wilf|H. S. Wilf]] によって発見された、確率論的証明法である<ref name="#1"/>。証明の概略は、次のとおりである。

: <math>e_\lambda = \frac{n!}{\prod_{(i,j)\in Y(\lambda)}h_\lambda(i,j)}.</math>

を定義し、 <math>d_\lambda = e_\lambda</math>を証明する。 

<math>d_\lambda</math>は以下で与えられる。

: <math>d_\lambda = \sum_{\mu\uparrow\lambda}d_\mu, </math>

ここで、 <math>\mu\uparrow\lambda</math> は、<math>\mu</math>がヤング図形λから一つのコーナーセルを削除することで得られるヤングタブローであることを表している。

そのようなμの全体にわたって和をとる。ここで、慣習として <math>\phi</math>を空のダイアグラムとして、 <math>d_{\phi}=1</math>を用いる。

上の式に対する説明は、「ヤングタブローの最大項はそのコーナーセルで生じるものである」となる。

そのセルを削除することで、μの形のヤングタブローを得る。

μの形のヤングタブローの数が  <math>d_{\mu}</math>であり、それらμに関して和をとることでその式を得る。
[[ファイル:Corners_of_young.png|右|サムネイル|Corners of the Young diagram (5,3,2,1,1)]]
ここで、<math>e_{\phi}=1</math>であることにも注意されたい。それゆえ、次を示せば十分で、

: <math>e_\lambda = \sum_{\mu\uparrow\lambda}e_\mu,</math>

その結果、 <math>d_\lambda=e_\lambda</math> は帰納的に証明される。

上の式の和は、次のように式を書き換えることによって、確率の和と捉えることができる。

: <math> \sum_{\mu\uparrow\lambda}\frac{e_\mu}{e_\lambda}=1.</math>

われわれはこのようにして、 <math>\frac{e_\mu}{e_\lambda}</math>が、ヤング図形μの集合上の確率測度を定めている。（ここで <math>\mu\uparrow\lambda</math>）

これはフックウォークと呼ばれるランダムウォークを定義を用いた構成法によるものである。

フックウォークは、ヤング図形λの上で、ひとつのコーナーセルを選択する。

フックウォークは次のルールによって定義される。

(1)  <math>|\lambda|</math> 個のセルのなかから一様ランダムにひとつのセルを選び、そこからランダムウォークを始める。

(2) 現在の <math>(i,j)</math>セルの次のセルは、一様ランダムにフック <math>H_{\lambda}(i,j)\setminus \{(i,j)\}</math>から選ぶ。

(3) 一つのコーナーに到達するまでこれを続け、そのコーナーセルを<math>\textbf{c}</math>とする。

'''命題:''' λに属するすべてのコーナーセル <math>(a,b)</math>に対して、次が成り立つ。

: <math>\mathbb{P}\left(\textbf{c}=(a,b)\right)=\frac{e_\mu}{e_\lambda},</math>

ここで、 <math>\mu=\lambda\setminus\{(a,b)\}</math>.

この命題を得れば、すべての <math>\textbf{c}=(a,b)</math> に関して和をとることによって、 <math> \sum_{\mu\uparrow\lambda}\frac{e_{\mu}}{e_{\lambda}}=1</math>を得る。<!--
=== Other proofs ===

Mention that there are many different proofs, give references. Mention the bijective proofs of Franzblau–Zeilberger and Novelli–Pak–Stoyanovskii and explain why they are important.
-->

== Connection to representation theory ==
The hook-length formula is of great importance in the representation theory of the [[symmetric group]] <math>S_n</math>, where the number <math>d_\lambda</math> is known to be equal to the dimension of the complex irreducible representation <math>V_\lambda</math> associated to <math>\lambda</math>, and is frequently denoted by <math>\dim V_\lambda</math>, <math>\dim \lambda</math> or <math>f^\lambda</math>.

=== Detailed discussion ===
The complex irreducible representations <math> V_{\lambda} </math> of the symmetric group are indexed by partitions <math> \lambda </math> of <math> n </math> (for an explicit construction see [[Specht module]]) . Their characters are related to the theory of symmetric functions via the Hall inner product in the following formula

: <math> \chi^\lambda(w)=\langle s_\lambda, p_{\tau(w)}\rangle </math>

where <math> s_{\lambda} </math> is the [[Schur polynomial|Schur function]] associated to <math> \lambda </math> and <math> p_{\tau(w)} </math> is the power-sum symmetric function of the partition <math> \tau(w) </math> associated to the cycle decomposition of <math> w </math>. For example, if <math> w=(154)(238)(6)(79) </math> then <math> \tau(w) = (3,3,2,1) </math>.

Since the identity permutation <math>e</math> has the form <math> e=(1)(2)\cdots(n) </math> in cycle notation, <math> \tau(e) = 1+1+\cdots+1=1^{(n)} </math>. Then the formula says

: <math> \dim  V_\lambda =\chi^\lambda(e) = \langle s_\lambda, p_{1^{(n)}}\rangle </math>

Considering the expansion of Schur functions in terms of [[Monomial symmetric function|monomial symmetric functions]] using the [[Kostka number|Kostka numbers]]

: <math>  s_\lambda= \sum_\mu K_{\lambda\mu}m_\mu,</math>

the inner product with <math> p_{1^{(n)}} = h_{1^{(n)}} </math> is <math>  K_{\lambda 1^{(n)}} </math>, because <math>  \langle m_{\mu},h_{\nu} \rangle = \delta_{\mu\nu} </math>. Note that <math> K_{\lambda 1^{(n)}}  </math> is equal to <math> d_{\lambda} </math>. Hence

: <math> \dim V_\lambda = d_\lambda. </math>

An immediate consequence of this is

: <math> \sum_{\lambda\vdash n} \left(f^{\lambda}\right)^2 = n! </math>

The above equality is also a simple consequence of the [[Robinson–Schensted–Knuth correspondence]].

The computation also shows that:

: <math> (x_1+x_2+\cdots+x_k)^n = \sum_{\lambda\vdash n} s_\lambda f^\lambda. </math>

Which is the expansion of <math>  p_{1^{(n)}} </math> in terms of Schur functions using the coefficients given by the inner product, because <math> \langle s_{\mu},s_{\nu}\rangle = \delta_{\mu\nu}  </math>. The above equality can be proven also checking the coefficients of each monomial at both sides and using the [[Robinson–Schensted–Knuth correspondence]] or, more conceptually, looking at the decomposition of <math>V^{\otimes n} </math> by irreducible <math>  GL(V) </math> modules, and taking characters. See [[Schur–Weyl duality]].

=== Outline of the proof of the hook formula using Frobenius formula ===
By the above considerations

: <math> p_{1^{(n)}} =  \sum_{\lambda\vdash n} s_{\lambda}f^{\lambda} </math>

So that

: <math> \Delta(x)p_{1^{(n)}} = \sum_{\lambda\vdash n} \Delta(x)s_{\lambda}f^{\lambda} </math>

where <math>  \Delta(x) = \prod_{i<j} (x_i-x_j)</math> is the [[Vandermonde determinant]].

For a given partition <math> \lambda = (\lambda_1, \lambda_2, \cdots, \lambda_k) </math> define <math> l_i = \lambda_i+k-i </math> for <math> i=1,2,\cdots,k </math>. For the following we need at least as many variables as rows in the partition, so from now on we work with <math>n </math> variables <math>x_1,\cdots,x_n</math>.

Each term <math> \Delta(x)s_{\lambda}  </math> is equal to

: <math> a_{(\lambda_1+k-1, \lambda_2+k-2, \dots , \lambda_k)} (x_1, x_2, \dots , x_k) =
\det \left[ \begin{matrix} x_1^{l_1} & x_2^{l_1} & \dots & x_k^{l_1} \\
x_1^{l_2} & x_2^{l_2} & \dots & x_k^{l_2} \\
\vdots & \vdots & \ddots & \vdots \\
x_1^{l_k} & x_2^{l_k} & \dots & x_k^{l_k} \end{matrix} \right]
</math>

See [[Schur polynomial|Schur function]]. Since the vector <math> (l_1,l_2,\cdots, l_k) </math> is different for each partition, this means that the coefficient of <math>  x_1^{l_1}\cdots x_k^{l_k} </math> in <math>\Delta(x)p_{1^{(n)}}</math>, denoted <math>\left[\Delta(x)p_{1^{(n)}}\right]_{l_1,\cdots,l_k}</math>, is equal to <math> f^{\lambda} </math>. This is known as the [[Frobenius formula|Frobenius Character Formula]], which gives one of the earliest proofs.<ref>W. Fulton, J. Harris. Representation Theory: A First Course Springer-Verlag , New York, 1991</ref> All that remains is tracking that coefficient with a mixture of cleverness and brute force: Multiplying

: <math> \Delta(x) = \sum_{w\in S_n}  \sgn(w) x_1^{w(1)-1}x_2^{w(2)-1}\cdots x_k^{w(k)-1} </math>

and

: <math> p_{1^{(n)}} = (x_1+x_2+\cdots+x_k)^n = \sum \frac{n!}{d_1!d_2!\cdots d_k!} x_1^{d_1}x_2^{d_2}\cdots x_k^{d_k} </math>

we conclude that the coefficient that we are looking for is

: <math> \sum_{w\in S_n} \sgn(w)\frac{n!}{(l_1-w(1)+1)!(l_2-w(2)+1)!\cdots (l_k-w(k)+1)!} </math>

which can be written as

: <math> \frac{n!}{l_1!l_2!\cdots l_k!} \sum_{w\in S_n} \sgn(w)\left[(l_1)(l_1-1)\cdots(l_1-w(1)+2)\right] \left[(l_2)(l_2-1)\cdots(l_2-w(2)+2)\right]\left[(l_k)(l_k-1)\cdots(l_k-w(k)+2)\right] </math>

The latter sum is equal to the following determinant

: <math> \det \left[ \begin{matrix} 1 & l_1 & l_1(l_1-1) & \dots & \prod_{i=0}^{k-2} (l_1-i) \\
1 & l_2 & l_2(l_2-1) & \dots & \prod_{i=0}^{k-2} (l_2-i)\\
\vdots & \vdots & \vdots& \ddots & \vdots \\
1 & l_k & l_k(l_k-1) & \dots & \prod_{i=0}^{k-2} (l_k-i) \end{matrix} \right] </math>

which column reduces to the Vandermonde determinant, and we obtain the formula

: <math> d_\lambda = \frac{n!}{l_1!l_2!\cdots l_k!} \prod_{i<j} (l_i-l_j) </math>

Note that <math> l_i </math> is the hook length of the first box in each row of the Young Diagram. Transforming this expression into the form <math> \frac{n!}{\prod h_\lambda (i,j)} </math> claimed by the hook-length formula is a fairly simple exercise in combinatorics: For any given <math> i = 1, 2, \ldots, k </math>, one has to argue that <math> l_i! = \left(\prod_{j > i} (l_i - l_j)\right) \cdot \prod_c h_\lambda(c) </math>, where the latter product ranges over all cells <math>c</math> in the <math>i</math>-row of the Young diagram of <math>\lambda</math>.

== Connection to longest increasing subsequences ==
The hook length formula also has important applications to the analysis of [[Longest increasing subsequence|longest increasing subsequences]] in random permutations. If <math>\sigma_n</math> denotes a uniformly random permutation of order <math>n</math>, <math>L(\sigma_n)</math> denotes the maximal length of an increasing subsequence of <math>\sigma_n</math>, and <math>\ell_n</math> denotes the expected (average) value of <math>L(\sigma_n)</math>, Anatoly Vershik and Sergei Kerov <ref>Vershik, A. M.; Kerov, C. V. (1977), "Asymptotics of the Plancheral measure of the symmetric group and a limiting form for Young tableaux", Dokl. Akad. Nauk SSSR 233: 1024–1027</ref> and independently Benjamin F. Logan and Lawrence A. Shepp <ref>B. F. Logan and L. A. Shepp, A variational problem for random Young tableaux, Advances in Math. 26 (1977), no. 2, 206–222.</ref> showed that when <math>n</math> is large, <math>\ell_n</math> is approximately equal to <math>2 \sqrt{n}</math>. This answers a question originally posed by [[Stanislaw Ulam]]. The proof is based on translating the question via the [[Robinson–Schensted correspondence]] to a problem about the limiting shape of a random Young tableau chosen according to [[Plancherel measure]]. Since the definition of Plancherel measure involves the quantity <math>d_\lambda</math>, the hook length formula can then be used to perform an asymptotic analysis of the limit shape and thereby also answer the original question.

The ideas of Vershik–Kerov and Logan–Shepp were later refined by Jinho Baik, Percy Deift and Kurt Johansson, who were able to achieve a much more precise analysis of the limiting behavior of the maximal increasing subsequence length, proving an important result now known as the Baik–Deift–Johansson theorem. Their analysis again makes crucial use of the fact that <math>d_\lambda</math> has a number of good formulas, although instead of the hook length formula it made use of one of the determinantal expressions.

== Related formulas ==
The formula for the number of Young tableau of a given shape was originally derived from the [[Frobenius determinant theorem|Frobenius determinant formula]] in connection to representation theory.<ref>{{citation|last1=Knuth|first1=Donald|publisher=Addison–Wesley|year=1973|authorlink=Donald Ervin Knuth|edition=1|title=[[The Art of Computer Programming]]|volume=3|pages=61–62}}</ref>  If the shape of a Young diagram is given by the row lengths <math>n_1,\dots,n_m</math>, then the number of tableau with that shape is given by

: <math> f(n_1,n_2,\ldots,n_m) = \frac{n! \,\Delta(n_m,n_{m-1}+1,\ldots,n_1 + m - 1)}{n_m ! (n_{m-1} + 1)! \cdots (n_1 + m - 1)!}</math>

Hook lengths can also be used to give a product representation to the generating function for the number of reverse plane partitions of a given shape.<ref>{{Citation|authorlink=Richard P. Stanley|last1=Stanley|first1=Richard P.|title=Theory and applications of plane partitions, 2|year=1971|journal=[[Studies in Applied Mathematics]]|volume=50|pages=259–279}}</ref>  If {{mvar|''λ''}} is a partition of some integer {{mvar|''p''}}, a reverse plane partition of {{mvar|''n''}} with shape {{mvar|''λ''}} is obtained by filling in the boxes in the Young diagram with non-negative integers such that the entries add to {{mvar|''n''}} and are non-decreasing along each row and down each column.  The hook lengths <math> h_1,\dots,h_p </math> can be defined as with Young tableau.  If {{math|''π''<sub>''n''</sub>}} denotes the number of reverse plane partitions of {{mvar|''n''}} with shape {{mvar|''λ''}}, then the generating function can be written as

: <math> \sum_{n=0}^\infty \pi_n x^n = \prod_{k=1}^p (1-x^{h_k})^{-1} </math>

Stanley discovered another formula for the same generating function.<ref>R.P. Stanley, "Ordered Structures and Partitions" PhD Thesis, Harvard University, 1971</ref> In general, if <math> A </math> is any poset with <math> n </math> elements, the generating function for reverse <math> A </math>-partitions is

: <math> \frac{P(x)}{(1-x)(1-x^2)\cdots(1-x^n)} </math>

where <math> P(x)  </math> is a polynomial such that <math>P(1)</math> is the number of natural labelings of <math> A </math>.

In the case of a partition <math> \lambda </math>, we are considering the poset in its cells given by the relation

: <math> (i,j) \leq (i',j') \iff i\leq i' \qquad \textrm{and} \qquad j\leq j'</math>.

So a natural labeling is simply a standard Young tableau, i.e. <math> P(1) = f^{\lambda} </math>

=== Yet another proof of the hook length formula ===
Combining the two formulas for the generating functions we have

: <math> \frac{P(x)}{(1-x)(1-x^2)\cdots(1-x^n)}  = \prod_{(i,j)\in \lambda} (1-x^{h_{(i,j)}})^{-1} </math>

Both sides converge inside the disk of radius one and the following expression makes sense for <math> |x| < 1 </math>

: <math> P(x) = \frac{\prod_{k=1}^n (1-x^k)}{\prod_{(i,j)\in \lambda} (1-x^{h_{(i,j)}})}. </math>

It would be violent to plug in 1, but the right hand side is a continuous function inside the unit disk and a polynomial is continuous everywhere so at least we can say

: <math> P(1) = \lim_{x\to 1} \frac{\prod_{k=1}^n (1-x^k)}{\prod_{(i,j)\in \lambda} (1-x^{h_{(i,j)}})}.   </math>

Finally, applying L'Hopital's rule <math> n </math> times yields the hook length formula

: <math> P(1) = \frac{n!}{\prod_{(i,j)\in \lambda}h_{(i,j)}}. </math>

== Specialization of Schur functions ==
Specializing the schur functions to the variables <math> 1,t,t^2,t^3, \cdots </math> there is the formula

: <math> s_{\lambda}(1,t,t^2,\cdots) = \frac{t^{n\left( \lambda\right)}}{\prod_{(i,j)\in Y(\lambda)}(1-t^{h_{\lambda}(i,j)})}  </math>

The number <math> n(\lambda) </math> is defined as

: <math> n(\lambda) = \sum_i (i-1)\lambda_i = \sum_i \binom{\lambda_i'}{2} </math>

where <math> \lambda' </math> is the conjugate partition

=== Skew shape formula ===
There is a generalization of this formula for skew shapes, <ref>Morales, A. H., Pak, I., and Panova, G. Hook formulas for skew shapes, arXiv:1512.08348.</ref>

: <math> s_{\lambda/\mu}(1,t,t^2,\cdots) = \sum_{S \in E(\lambda/\mu)} \prod_{(i,j) \in \lambda\setminus S} \frac{t^{\lambda_j'-i}}{1-t^{h(i,j)}}  </math>

where the sum is taken over ''excited diagrams'' of shape <math>\lambda</math> and boxes distributed according to <math>\mu</math>.

== A formula for the Catalan numbers ==
The [[Catalan number|Catalan numbers]] are ubiquitous in [[enumerative combinatorics]]. Not surprisingly, they are also part of this story:

: <math> C_n = f^{(n,n)} </math>

Lets briefly mention why.  When doing a Dyck path we may go up (U) or down (D). So for any Dyck path of length <math> n </math> consider the tableaux of shape <math> (n,n) </math> such that the first row is given by the numbers <math> i </math> such that the <math> i </math>-th step was up and in the second row given by the positions in which it goes down. For example, UUDDUD correspond to the tableaux with rows 125 and 346.

The hook formula gives another way of getting a closed formula for the Catalan numbers

: <math> C_n = \frac{(2n)!}{(n+1)(n)\cdots(3)(2)(n)(n-1)\cdots(2)(1)} = \frac{(2n)!}{(n+1)!n!} = \frac{1}{n+1}\binom{2n}{n}</math>

== 脚注 ==
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== 関連項目 ==

* [[ヤング図形]]
* [[シューア多項式]]

== 外部リンク ==

* A [http://www.math.ucdavis.edu/~romik/book/ published book on longest increasing subsequences] by Dan Romik (PDF copy available for download). Contains discussions of the hook length formula and several of its variants, with applications to the mathematics of longest increasing subsequences.

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[[Category:組合せ論]]
[[Category:数学に関する記事]]