Question on orthogonal eigenfunctions

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The discussion centers on finding normalized linear combinations of two eigenfunctions, φ1 and φ2, that are orthogonal to specified functions. The integral condition provided, ∫φ1*φ2 dτ = d, indicates a non-zero overlap between the eigenfunctions. To achieve orthogonality, two equations are established: L.L = 1 for normalization and L.φ1 = 0 for the first case, and L.(φ1 + φ2) = 0 for the second. The solution involves solving these equations simultaneously for the coefficients c1 and c2. Understanding this process requires a grasp of linear algebra concepts, particularly regarding eigenfunctions and orthogonality.
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in this book I have by G.L Squires. One of the questions is:

if \phi1 and \phi2 are normalized eigenfunctions corresponding to the same eigenvalue. If:
\int\phi1*\phi2 d\tau = d

where d is real, find normalized linear combinations of \phi1 and
\phi 2 that are orthogonal to a) \phi 1 b) \phi1 + \phi2the part I'm having trouble with is finding a linear combination. The book gives: c1phi1 + c2phi2 (to shorten it) as the linear combo but yeah, what's the deal with that. they give a solution for a but yeah what is going on there. what's the process involved. yes, I am basically asking for a "tutor" so to speak, so I am n0t asking for any old person to help me but someone who is willing to explain it without becoming angry that I know not of such things.
thanks in advance!
 
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Let L be the linear combination (depends on c1 and c2). In both cases you have one (of two) equation L.L=1.
(. means dot product, which is the integral you described).

For a) the other equation is L.φ1=0.
For b) the other equation is L.(φ12)=0

You wil have in both cases two equations in two unknowns (c1 and c2).
 
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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