Can Quaternion and Pauli Matrix algebra be linked in EM course?

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Quaternion algebra can be linked to Pauli matrix algebra in the context of electromagnetism (EM) courses, particularly through the metric tensor of Minkowski space. The introduction of quaternions relates to Dirac's propositions regarding the Schrödinger equation, leading to the formulation of (4-4) matrices derived from (2-2) Pauli matrices. A key relationship is established where the product of these matrices satisfies a specific equation involving the metric tensor. Additionally, Hamilton multiplication rules differ from Pauli matrix rules by a factor of i, and using biquaternions can simplify the formulas of general relativity. The connection between Pauli quaternions and three-dimensional Clifford Algebra remains an intriguing area for further exploration.
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i am learning Quaternion now for my EM course. Can someone enlighten me on the correspondence between Quaternion and Pauli Matrix algebra?
 
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Not so easy to explain;
metric tensor of the Minkowski's space <=> introduction of the quaternions;
a proposition from Dirac to discuss the Schrödinger equation => introduction of (4-4) matrices built in fine with the (2-2) Pauli's matrices;
Let us call m(a) for a = 0, 1, 2, 3 the different (4-4) matrices; the discussion shows that following relation must hold: m(a). m(b) + m(b). m(a) = 2. g(ab)
where g(ab) is the metric tensor for a Minkowski’s space.

So: not a real good explanation (sorry) but a short exposé of the connections between the actors
 
From this site: http://home.pcisys.net/~bestwork.1/HamiltonQ/hamilton.htm

This quote:
The Hamilton multiplication rules differ from the Pauli matrix rules only by a factor of i. It is possible to formulate special relativity with Hamilton quaternions having complex coefficients(called biquaternions) and indeed it was first done that way(Silberstein). It turns out that the formulae of general relativity are simpler with the Pauli quaternions. There is also a very interesting (and possibly significant) relation between the Pauli quaternions and three dimensional Clifford Algebra
 
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still yet to figure out.. but the web link looks pretty informative. Thanks. Will see if i can make some sense out of it.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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