Unitary and linear operator in quantum mechanics

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In quantum mechanics, a transformation U that satisfies the invariance of the scalar product, <ψ'|ψ'> = <ψ|ψ>, indicates that U is either linear and unitary or antilinear and antiunitary. To prove this for a linear and unitary U, one can show that <Uψ|Uψ> simplifies to <ψ|ψ> using properties of inner products and the adjoint operator. The proof can be streamlined by demonstrating that <Uφ|Uψ> equals <φ|ψ> without needing to reference a specific basis. The discussion confirms that the initial approach to proving U's properties is correct, emphasizing the importance of linearity in the transformation. Understanding these properties is crucial for the mathematical foundation of quantum mechanics.
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Given a transformation ##U## such that ##|\psi'>=U|\psi>##, the invariance ##<\psi'|\psi'>=<\psi|\psi>## of the scalar product under the transformation ##U## means that ##U## is either linear and unitary, or antilinear and antiunitary.

How do I prove this?

##<\psi'|\psi'>##
##= <U\psi|U\psi>##

For ##U## unitary and linear, we have
##<U\psi|U\psi>##
##<U(\alpha\psi_{a}+\beta\psi_{\beta})|U(\alpha\psi_{a}+\beta\psi_{\beta})>##
##<(\alpha U\psi_{a}+\beta U\psi_{\beta})|(\alpha U\psi_{a}+\beta U\psi_{\beta})>##
##=(<\psi_{a}|(U^{\dagger})\alpha^{*}+<\psi_{b}|(U^{\dagger})\beta^{*})(\alpha U|\psi_{a}>+\beta U|\psi_{\beta}>)##
##=|\alpha|^{2}(<\psi_{a}|(U^{\dagger})(U)|\psi_{a}>+|\beta|^{2}(<\psi_{b}|(U^{\dagger})(U)|\beta>##
##=|\alpha|^{2}+|\beta|^{2}##

Is this how the proof should go for ##U## linear and unitary?
 
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But you don't need to go into a basis: ##\langle U\phi|U\psi\rangle =\langle \phi|U^*U\psi\rangle=\langle \phi|\psi\rangle## is enough.
 
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I wanted to show the property of linearity.
 
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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