Schwarz reflection principle: Difference between revisions
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In [[mathematics]], the '''Hausdorff moment problem''', named after [[Felix Hausdorff]], asks for necessary and sufficient conditions that a given sequence { ''m''<sub>''n''</sub> : ''n'' = 0, 1, 2, ... } | |||
be the sequence of [[moment (mathematics)|moments]] | |||
:<math>m_n = \int_0^1 x^n\,d\mu(x)\,</math> | |||
of some [[Borel measure]] ''μ'' [[support (measure theory)|supported]] on the closed unit interval [0, 1]. In the case ''m''<sub>0</sub> = 1, this is equivalent to the existence of a [[random variable]] ''X'' supported on [0, 1], such that '''E''' ''X''<sup>n</sup> = ''m''<sub>''n''</sub>. | |||
The essential difference between this and other well-known moment problems is that this is on a bounded interval, whereas in the [[Stieltjes moment problem]] one considers a half-line [0, ∞), and in the [[Hamburger moment problem]] one considers the whole line (−∞, ∞). | |||
In 1921, Hausdorff showed that { ''m''<sub>''n''</sub> : ''n'' = 0, 1, 2, ... } is such a moment sequence if and only if the sequence is '''completely monotonic''', i.e., its difference sequences satisfy the equation | |||
:<math>(-1)^k(\Delta^k m)_n \geq 0</math> | |||
for all ''n'',''k'' ≥ 0. Here, Δ is the [[difference operator]] given by | |||
:<math>(\Delta m)_n = m_{n+1} - m_n.</math> | |||
The necessity of this condition is easily seen by the identity | |||
:<math>(-1)^k(\Delta^k m)_n = \int_0^1 x^n (1-x)^k d\mu(x),</math> | |||
which is ''≥ 0'', being the integral of an almost sure non-negative function. | |||
For example, it is necessary to have | |||
:<math>\Delta^4 m_6 = m_6 - 4m_7 + 6m_8 - 4m_9 + m_{10} = \int x^6 (1-x)^4 d\mu(x) \geq 0.</math> | |||
==See also== | |||
* [[Total monotonicity]] | |||
==References== | |||
* Hausdorff, F. "Summationsmethoden und Momentfolgen. I." ''Mathematische Zeitschrift'' 9, 74-109, 1921. | |||
* Hausdorff, F. "Summationsmethoden und Momentfolgen. II." ''Mathematische Zeitschrift'' 9, 280-299, 1921. | |||
* Feller, W. "An Introduction to Probability Theory and Its Applications", volume II, John Wiley & Sons, 1971. | |||
* [[James Alexander Shohat|Shohat, J.A]].; [[Jacob Tamarkin|Tamarkin, J. D.]] ''The Problem of Moments'', American mathematical society, New York, 1943. | |||
==External links== | |||
* [http://mathworld.wolfram.com/MomentProblem.html Moment Problem, on Mathworld] | |||
[[Category:Probability theory]] | |||
[[Category:Theory of probability distributions]] | |||
[[Category:Mathematical problems]] |
Revision as of 04:07, 22 May 2013
In mathematics, the Hausdorff moment problem, named after Felix Hausdorff, asks for necessary and sufficient conditions that a given sequence { mn : n = 0, 1, 2, ... } be the sequence of moments
of some Borel measure μ supported on the closed unit interval [0, 1]. In the case m0 = 1, this is equivalent to the existence of a random variable X supported on [0, 1], such that E Xn = mn.
The essential difference between this and other well-known moment problems is that this is on a bounded interval, whereas in the Stieltjes moment problem one considers a half-line [0, ∞), and in the Hamburger moment problem one considers the whole line (−∞, ∞).
In 1921, Hausdorff showed that { mn : n = 0, 1, 2, ... } is such a moment sequence if and only if the sequence is completely monotonic, i.e., its difference sequences satisfy the equation
for all n,k ≥ 0. Here, Δ is the difference operator given by
The necessity of this condition is easily seen by the identity
which is ≥ 0, being the integral of an almost sure non-negative function. For example, it is necessary to have
See also
References
- Hausdorff, F. "Summationsmethoden und Momentfolgen. I." Mathematische Zeitschrift 9, 74-109, 1921.
- Hausdorff, F. "Summationsmethoden und Momentfolgen. II." Mathematische Zeitschrift 9, 280-299, 1921.
- Feller, W. "An Introduction to Probability Theory and Its Applications", volume II, John Wiley & Sons, 1971.
- Shohat, J.A.; Tamarkin, J. D. The Problem of Moments, American mathematical society, New York, 1943.