Palaeomagnetism is the study of past magnetic fields recorded by geological or archaeological material, also spelled paleomagnetism. A measured direction or polarity can be compared with a dated regional or global magnetic sequence to constrain an event's age.
The magnetic component must belong to the event being dated: subsequent heating or chemical change can produce remagnetization. Laboratory separation of magnetic components and independent geological relationships are therefore part of the dating argument.[ref]
Rocks and Paleomagnetics Laboratory by United States Geological Survey. Research uses and separation of original and secondary magnetizations
magnetization retained as magnetic minerals cool through blocking temperatures in an ambient field. Subsequent alteration, reheating and remagnetization can change the record.
A measured magnetic field component or magnitude after subtraction of a reference field. Source geometry, magnetization direction and observation height affect its sign and amplitude; an anomaly is not a direct map of rock polarity.
A magnetic signal caused by the shape and distribution of magnetized terrain. Excavating a crater removes magnetic host rock, while its rim and remaining slopes redistribute magnetic masses. Unlike a gravity slab reduction, the effect depends on the vector magnetization, including remanence, so it has no universal density-only correction. Modelling the host and relief is necessary before attributing a crater anomaly to magnetic material in its infill.
The difference between a target region and the reference material it replaces. A weakly magnetic crater infill inside magnetic basalt can have a negative induced contrast, even though both materials have positive magnetic susceptibility. The sign and direction of this contrast, including remanent magnetization, determine a total-field magnetic anomaly together with geometry and the ambient field. Geophysical density contrast does not determine magnetic contrast.
The difference between measured scalar field strength and a specified background. For , it is approximately , not an arbitrary fixed Cartesian component.
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