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The '''Ozsváth–Schücking metric''', or the '''Ozsváth–Schücking solution''', is a [[vacuum solution (general relativity)|vacuum solution]] of the [[Einstein field equations]].  The metric was published by István Ozsváth and [[Engelbert Schücking]] in 1962.<ref>{{citation|first1=I.|last1=Ozsváth|first2=E.|last2=Schücking|title=An anti-Mach metric|journal=Recent Developments in General Relativity|pages=339–350|year=1962|url=http://web.mit.edu/jwk/www/docs/Ozsvath-Schucking%201962%20-%20Anti-Mach%20Metric.pdf}}</ref>  It is noteworthy among vacuum solutions for being the first known solution that is [[stationary spacetime|stationary]], globally defined, and singularity-free but nevertheless not isometric to the [[Minkowski metric]].  This stands in contradiction to a claimed strong Mach principle, which would forbid a vacuum solution from being anything but Minkowski without singularities, where the singularities are to be construed as mass as in the [[Schwarzschild metric]].<ref>{{citation|first1=F. A. E.|last1=Pirani|title=Invariant Formulation of Gravitational Radiation Theory|journal=Phys. Rev.|volume=105|pages=1089–1099|year=1957|doi=10.1103/PhysRev.105.1089|bibcode = 1957PhRv..105.1089P }}</ref>
 
With coordinates <math>\{x^0,x^1,x^2,x^3\}</math>, define the following [[tetrad (general relativity)|tetrad]]:
 
:<math>e_{(0)}=\frac{1}{\sqrt{2+(x^3)^2}}\left( x^3\partial_0-\partial_1+\partial_2\right)</math>
:<math>e_{(1)}=\frac{1}{\sqrt{4+2(x^3)^2}}\left[ \left(x^3-\sqrt{2+(x^3)^2}\right)\partial_0+\left(1+(x^3)^2-x^3\sqrt{2+(x^3)^2}\right)\partial_1+\partial_2\right]</math>
:<math>e_{(2)}=\frac{1}{\sqrt{4+2(x^3)^2}}\left[ \left(x^3+\sqrt{2+(x^3)^2}\right)\partial_0+\left(1+(x^3)^2+x^3\sqrt{2+(x^3)^2}\right)\partial_1+\partial_2\right]</math>
:<math>e_{(3)}=\partial_3</math>
 
It is straightforward to verify that e<sub>(0)</sub> is timelike, e<sub>(1)</sub>, e<sub>(2)</sub>, e<sub>(3)</sub> are spacelike, that they are all [[orthogonal]], and that there are no singularities. The corresponding proper time is
 
:<math>{d \tau}^{2} = -(dx^0)^2 +4(x^3)(dx^0)(dx^2)-2(dx^1)(dx^2)-2(x^3)(dx^2)^2-(dx^3)^2.</math>
 
The [[Riemann tensor]] has only one algebraically independent, nonzero component
 
:<math>R_{0202}=-1,</math>
 
which shows that the spacetime is [[Ricci flat]] but not [[conformally flat]].  That is sufficient to conclude that it is a vacuum solution distinct from Minkowski spacetime.  Under a suitable coordinate transformation, the metric can be rewritten as
 
:<math>
d\tau^2 = [(x^2 - y^2) \cos (2u) + 2xy \sin(2u)] du^2 - 2dudv - dx^2 - dy^2
</math>
 
and is therefore an example of a [[pp-wave spacetime]].
 
==References==
<references/>
 
{{DEFAULTSORT:Ozsvath-Schucking metric}}
[[Category:Exact solutions in general relativity]]
 
 
{{relativity-stub}}

Revision as of 12:21, 9 May 2013

The Ozsváth–Schücking metric, or the Ozsváth–Schücking solution, is a vacuum solution of the Einstein field equations. The metric was published by István Ozsváth and Engelbert Schücking in 1962.[1] It is noteworthy among vacuum solutions for being the first known solution that is stationary, globally defined, and singularity-free but nevertheless not isometric to the Minkowski metric. This stands in contradiction to a claimed strong Mach principle, which would forbid a vacuum solution from being anything but Minkowski without singularities, where the singularities are to be construed as mass as in the Schwarzschild metric.[2]

With coordinates {x0,x1,x2,x3}, define the following tetrad:

e(0)=12+(x3)2(x301+2)
e(1)=14+2(x3)2[(x32+(x3)2)0+(1+(x3)2x32+(x3)2)1+2]
e(2)=14+2(x3)2[(x3+2+(x3)2)0+(1+(x3)2+x32+(x3)2)1+2]
e(3)=3

It is straightforward to verify that e(0) is timelike, e(1), e(2), e(3) are spacelike, that they are all orthogonal, and that there are no singularities. The corresponding proper time is

dτ2=(dx0)2+4(x3)(dx0)(dx2)2(dx1)(dx2)2(x3)(dx2)2(dx3)2.

The Riemann tensor has only one algebraically independent, nonzero component

R0202=1,

which shows that the spacetime is Ricci flat but not conformally flat. That is sufficient to conclude that it is a vacuum solution distinct from Minkowski spacetime. Under a suitable coordinate transformation, the metric can be rewritten as

dτ2=[(x2y2)cos(2u)+2xysin(2u)]du22dudvdx2dy2

and is therefore an example of a pp-wave spacetime.

References

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    Naturally, you will have to pay a safety deposit and that is usually one month rent for annually of the settlement. That is the place your good religion deposit will likely be taken into account and will kind part or all of your security deposit. Anticipate to have a proportionate amount deducted out of your deposit if something is discovered to be damaged if you move out. It's best to you'll want to test the inventory drawn up by the owner, which can detail all objects in the property and their condition. If you happen to fail to notice any harm not already mentioned within the inventory before transferring in, you danger having to pay for it yourself.

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