Undergrad Difference Between T_{a}^{b} & T^{a}_{b}: (1,1) Tensors

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The discussion clarifies the distinction between the (1,1) tensors T_{a}^{b} and T^{a}_{b}, emphasizing that they are functions defined on different pairs of vector spaces. T_{a}^{b} takes a vector as its first argument and a dual vector as its second, while T^{a}_{b} does the opposite. Although both tensors can be related through the metric for index manipulation, they are generally not equivalent unless specific conditions, such as symmetry, are met. The geometric interpretation does not change between the two forms, but their functional roles differ significantly. Understanding these differences is crucial for proper tensor analysis in mathematical physics.
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What is the difference between ##{T{_{a}}^{b}}## and ##{T{^{a}}_{b}}## ? Both are (1,1) tensors that eat a vector and a dual to produce a scalar. I understand I could act on one with the metric to raise and lower indecies to arrive at the other but is there a geometric difference between the objects to which these are components?
 
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I don't think there's a geometric difference. The difference is that, where ##V## and ##V^*## are the underlying vector space and its dual, ##T_a{}^b## is a function from ##V\times V^*## to ##\mathbb R## and ##T^a{}_b## is a function from ##V^*\times V## to ##\mathbb R##. Or if we think of the tensor as being a function that takes two arguments, ##T_a{}^b## takes a vector as its first argument and ##T^a{}_b## takes a dual vector as its first argument.
 
Generally, they are different (1,1) tensors (you could imagine sidestepping #2 by defining the obvious equivalence between functions from ##V\times V^*## and functions from ##V^* \times V##). It is certainly not true that ##T^a_{\phantom ab} \omega_a V^b = T^{\phantom ba}_b \omega_a V^b## except in the case where ##T^a_{\phantom ab} g_{ac}## is symmetric.
 
##T_{\ \ \ \nu}^\mu=g_{\nu\xi}T^{\mu\xi}## and

##T^{\ \nu}_\mu=g_{\mu\xi}T^{\xi\nu}##

are different in general. Obviously when T is symmetric

##T^\mu_{\ \ \ \nu}=T^{\ \nu}_\mu## and they can be denoted as ##T^{\nu}_\mu##.
 
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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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