Minkowski's question mark function: Difference between revisions

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In [[mathematics]], the '''Jacobi triple product''' is the mathematical identity:
 
:<math>\prod_{m=1}^\infty
\left( 1 - x^{2m}\right)
\left( 1 + x^{2m-1} y^2\right)
\left( 1 + x^{2m-1} y^{-2}\right)
= \sum_{n=-\infty}^\infty x^{n^2} y^{2n},
</math>
for complex numbers ''x'' and ''y'', with |''x''| &lt; 1 and ''y'' ≠ 0.
 
It was introduced by {{harvs|txt|authorlink=Carl Gustav Jacob Jacobi|last=Jacobi|year=1829}} in his work ''[[Fundamenta Nova Theoriae Functionum Ellipticarum]]''.
 
The Jacobi triple product identity is the  [[Macdonald identity]] for the affine root system of type ''A''<sub>1</sub>, and is the [[Weyl denominator formula]] for the corresponding affine [[Kac–Moody algebra]].
 
== Properties ==
 
The basis of Jacobi's proof relies on Euler's [[pentagonal number theorem]], which is itself a specific case of the Jacobi Triple Product Identity.
 
Let <math>x=q^{3/2}</math> and <math>y^2=-\sqrt{q}</math>.  Then we have
:<math>\phi(q) = \prod_{m=1}^\infty \left(1-q^m \right) =
\sum_{n=-\infty}^\infty (-1)^n q^{(3n^2-n)/2}.\, </math>
 
The Jacobi Triple Product also allows the Jacobi [[theta function]] to be written as an infinite product as follows:
 
Let <math>x=e^{i\pi \tau}</math> and <math>y=e^{i\pi z}.</math>
 
Then the Jacobi theta function
 
:<math>
\vartheta(z; \tau) = \sum_{n=-\infty}^\infty \exp (\pi i n^2 \tau + 2 \pi i n z)
</math>
 
can be written in the form
 
:<math>\sum_{n=-\infty}^\infty y^{2n}x^{n^2}. </math>
 
Using the Jacobi Triple Product Identity we can then write the theta function as the product
 
:<math>\vartheta(z; \tau) = \prod_{m=1}^\infty
\left( 1 - \exp(2m \pi i \tau)\right)
\left( 1 + \exp((2m-1) \pi i \tau + 2 \pi i z)\right)
\left( 1 + \exp((2m-1) \pi i \tau -2 \pi i z)\right).
</math>
 
There are many different notations used to express the Jacobi triple product.  It  takes on a concise form when expressed in terms of [[q-Pochhammer symbol]]s:
 
:<math>\sum_{n=-\infty}^\infty q^{n(n+1)/2}z^n =
(q;q)_\infty \; (-1/z;q)_\infty \; (-zq;q)_\infty.</math>
 
Where <math>(a;q)_\infty</math> is the infinite ''q''-Pochhammer symbol.
 
It enjoys a particularly elegant form when expressed in terms of the [[Ramanujan theta function]]. For <math>|ab|<1.</math> it can be written as
 
:<math>\sum_{n=-\infty}^\infty a^{n(n+1)/2} \; b^{n(n-1)/2} = (-a; ab)_\infty \;(-b; ab)_\infty \;(ab;ab)_\infty.</math>
 
==Proof==
This proof uses a simplified model of the [[Dirac sea]] and follows the proof in Cameron (13.3) which is attributed to [[Richard Borcherds]]. It treats the case where the power series are formal. For the analytic case, see Apostol. The Jacobi triple product identity can be expressed as
 
:<math>\prod_{n>0}(1+q^{n-\frac{1}{2}}z)(1+q^{n-\frac{1}{2}}z^{-1})=\left(\sum_{l\in\mathbb{Z}}q^{l^2/2}z^l\right)\left(\prod_{n>0}(1-q^n)^{-1}\right).</math>
 
A ''level'' is a [[half-integer]]. The vacuum state is the set of all negative levels. A state is a set of levels whose symmetric difference with the vacuum state is finite. The ''energy'' of the state <math>S</math> is
 
:<math>\sum\{v\colon v > 0,v\in S\} - \sum\{v\colon v < 0, v\not\in S\}</math>
 
and the ''particle number'' of <math>S</math> is
 
:<math>|\{v\colon v>0,v\in S\}|-|\{v\colon v<0,v\not\in S\}|.</math>
 
An unordered choice of the presence of finitely many positive levels and the absence of finitely many negative levels (relative to the vacuum) corresponds to a state, so the generating function <math>\textstyle\sum_{m,l} s(m,l)q^mz^l</math> for the number <math>s(m,l)</math> of states of energy <math>m</math> with <math>l</math> particles can be expressed as
 
:<math>\prod_{n>0}(1+q^{n-\frac{1}{2}}z)(1+q^{n-\frac{1}{2}}z^{-1}).</math>
 
On the other hand, any state with <math>l</math> particles can be obtained from the lowest energy <math>l-</math>particle state, <math>\{v\colon v<l\}</math>, by rearranging particles: take a partition <math>\lambda_1\geq\lambda_2\geq\cdots\geq\lambda_j</math> of <math>m'</math> and move the top particle up by <math>\lambda_1</math> levels, the next highest particle up by <math>\lambda_2</math> levels, etc.... The resulting state has energy <math>m'+\frac{l^2}{2}</math>, so the generating function can also be written as
 
:<math>\left(\sum_{l\in\mathbb{Z}}q^{l^2/2}z^l\right)\left(\sum_{n\geq0}p(n)q^n\right)=\left(\sum_{l\in\mathbb{Z}}q^{l^2/2}z^l\right)\left(\prod_{n>0}(1-q^n)^{-1}\right)</math>
 
where <math>p(n)</math> is the [[Partition function (number theory)|partition function]]. [http://arxiv.org/abs/math-ph/0309015 The uses of random partitions] by [[Andrei Okounkov]] contains a picture of a partition exciting the vacuum.
 
== Notes ==
<references/>
 
==References==
* See chapter 14, theorem 14.6 of {{Apostol IANT}}
* Peter J. Cameron, ''Combinatorics: Topics, Techniques, Algorithms'', (1994) Cambridge University Press, ISBN 0-521-45761-0
*{{Citation | last1=Jacobi | first1=C. G. J. | title=Fundamenta nova theoriae functionum ellipticarum | url=http://archive.org/details/fundamentanovat00jacogoog | publisher=Borntraeger|place=Königsberg | language=Latin | isbn=978-1-108-05200-9 | id=Reprinted by Cambridge University Press 2012 | year=1829}}
 
[[Category:Elliptic functions]]
[[Category:Theta functions]]
[[Category:Mathematical identities]]
[[Category:Number theory]]

Revision as of 16:59, 1 November 2013

In mathematics, the Jacobi triple product is the mathematical identity:

for complex numbers x and y, with |x| < 1 and y ≠ 0.

It was introduced by Template:Harvs in his work Fundamenta Nova Theoriae Functionum Ellipticarum.

The Jacobi triple product identity is the Macdonald identity for the affine root system of type A1, and is the Weyl denominator formula for the corresponding affine Kac–Moody algebra.

Properties

The basis of Jacobi's proof relies on Euler's pentagonal number theorem, which is itself a specific case of the Jacobi Triple Product Identity.

Let and . Then we have

The Jacobi Triple Product also allows the Jacobi theta function to be written as an infinite product as follows:

Let and

Then the Jacobi theta function

can be written in the form

Using the Jacobi Triple Product Identity we can then write the theta function as the product

There are many different notations used to express the Jacobi triple product. It takes on a concise form when expressed in terms of q-Pochhammer symbols:

Where is the infinite q-Pochhammer symbol.

It enjoys a particularly elegant form when expressed in terms of the Ramanujan theta function. For it can be written as

Proof

This proof uses a simplified model of the Dirac sea and follows the proof in Cameron (13.3) which is attributed to Richard Borcherds. It treats the case where the power series are formal. For the analytic case, see Apostol. The Jacobi triple product identity can be expressed as

A level is a half-integer. The vacuum state is the set of all negative levels. A state is a set of levels whose symmetric difference with the vacuum state is finite. The energy of the state is

and the particle number of is

An unordered choice of the presence of finitely many positive levels and the absence of finitely many negative levels (relative to the vacuum) corresponds to a state, so the generating function for the number of states of energy with particles can be expressed as

On the other hand, any state with particles can be obtained from the lowest energy particle state, , by rearranging particles: take a partition of and move the top particle up by levels, the next highest particle up by levels, etc.... The resulting state has energy , so the generating function can also be written as

where is the partition function. The uses of random partitions by Andrei Okounkov contains a picture of a partition exciting the vacuum.

Notes


References

  • See chapter 14, theorem 14.6 of Template:Apostol IANT
  • Peter J. Cameron, Combinatorics: Topics, Techniques, Algorithms, (1994) Cambridge University Press, ISBN 0-521-45761-0
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