Differential Geometry from Differential Equations
Differential Geometry from Differential Equations
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微分方程的微分几何
DOI:
10.1007/s002200100548
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发表时间:
2000
期刊:
影响因子:
--
通讯作者:
E. Newman
中科院分区:
文献类型:
--
作者:
S. Frittelli;C. Kozameh;E. Newman
We first show how, from the general 3rd order ODE of the form , one can construct a natural Lorentzian conformal metric on the four-dimensional space . When the function satisfies a special differential condition the conformal metric possesses a conformal Killing field, , which in turn, allows the conformal metric to be mapped into a three dimensional Lorentzian metric on the space ) or equivalently, on the space of solutions of the original differential equation. This construction is then generalized to the pair of differential equations,zss=S(z,zs,zt,zst,s,t) andztt=T(z,zs,zt,zst,s,t), withzsandztthe derivatives ofzwith respect tosandt. In this case, fromSandT, one can again, in a natural manner, construct a Lorentzian conformal metric on the six dimensional space (z,zs,zt,zst,s,t). When theSandTsatisfy differential conditions analogous to those of the 3rdorder ode, the 6-space then possesses a pair of conformal Killing fields, and which allows, via the mapping to the four-space of (z,zs,zt,zst) and a choice of conformal factor, the construction of a four-dimensional Lorentzian metric. In fact all four-dimensional Lorentzian metrics can be constructed in this manner. This construction, with further conditions onSandT, thus includes all (local) solutions of the Einstein equations.