LS coupling and calculating the total angular momentum

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The discussion focuses on calculating total angular momentum (J) in many-electron atoms using LS coupling. Given L=2 (orbital angular momentum) and S=1 (spin angular momentum), the possible configurations for J can be derived using the quantum mechanical rule J=L+S, L+S-1, ..., |L-S|. This results in potential values of J being 3, 2, and 1. Participants seek clarification on how to apply this rule to determine specific configurations and their corresponding total angular momentum values. Understanding these calculations is essential for grasping the behavior of electrons in multi-electron systems.
cooper607
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hi all, these days i m going through Arther Beiser's modern physics book where i read about the total angular momentum in many electron atoms..now i could understand the LS coupling and spin orbit effect how they combine to form total angular momentum but if i m given the magnitude of L=2 (orbital angular momentum ) and S=1 (spin angular momentum)

then how can i calculate the configurations they can have and also how can i calculate the J(total angular momentum ) for each configuration ...please help me anyone... i m referring from BESISER'S "PERSPECTIVE OF MODERN PHYSICS "
 
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The general rule for addition of angular momenta in quantum mechanics is, for ##J=L+S##,
$$
J = L+S, L+S-1, \ldots, \left| L - S \right|
$$
 
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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