What Do Upper and Lower Indices in Tensor Notation Signify?

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Upper and lower indices in tensor notation signify different types of quantities: upper indices represent contravariant vectors, while lower indices denote covariant vectors or covectors. In the context of manifolds, covectors correspond to differential forms that can be integrated without a metric, whereas vectors require a metric for their definition. The distinction is crucial for understanding tensor manipulation in general relativity, where both types of indices can coexist in a single tensor. This relationship allows for a one-to-one correspondence between covectors and vectors when a metric is present. Clarifying this conceptual difference is essential for further comprehension of tensor calculus in physics.
taylrl3
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Hi,

I am very new to general relativity and have only just started to learn how to do some very basic manipulation of tensors. I can understand the methods I am using and have some idea of what a tensor is but am not sure what the difference between upper and lower indices signifies. I can identify that one is covariant and another contravariant but what is the difference between the two and what about when a tensor has both indices? I feel I need to clear this conceptual issue up before I can understand things further. Thanks :-)

Taylrl
 
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Usually one of them is associated to "covectors" and the other to "vectors". Both are vectors in the linear algebra sense, but on a manifold, the former correspond to "forms" which are things that can be integrated even without a metric. In the presence of a metric, as in general relativity, there is one-to-one correspondence between covectors and vectors. http://www.math.ucla.edu/~tao/preprints/forms.pdf

A perhaps more physical explanation goes something like https://www.physicsforums.com/showpost.php?p=3361102&postcount=14.
 
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MOVING CLOCKS In this section, we show that clocks moving at high speeds run slowly. We construct a clock, called a light clock, using a stick of proper lenght ##L_0##, and two mirrors. The two mirrors face each other, and a pulse of light bounces back and forth betweem them. Each time the light pulse strikes one of the mirrors, say the lower mirror, the clock is said to tick. Between successive ticks the light pulse travels a distance ##2L_0## in the proper reference of frame of the clock...

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