Graduate HHL quantum algorithm and the phase estimation

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The HHL algorithm's controlled unitary, integral to the Hamiltonian simulation in Quantum Phase Estimation, is directly influenced by the coefficients of the Hermitian matrix. These coefficients define the system's Hamiltonian, which is essential for constructing the controlled unitary. The Hamiltonian facilitates the evolution of the state vector over time. This evolved state vector is crucial for estimating the eigenvalues of the Hamiltonian. Understanding this relationship is key to effectively implementing the HHL algorithm.
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In HHL algorithm, does the controlled unitary (Hamiltonian simulation part of Quantum phase estimation) depend on Hermitian matrix coefficients and how?
In HHL algorithm, does the controlled unitary (Hamiltonian simulation part of Quantum phase estimation) depend on Hermitian matrix coefficients and how?
 
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Yes, the controlled unitary used in the Hamiltonian simulation part of Quantum Phase Estimation depends on the Hermitian matrix coefficients. Specifically, the controlled unitary is constructed from the matrix coefficients of the Hermitian matrix that describes the system’s Hamiltonian. The Hamiltonian is then used to evolve the given state vector over a period of time, and the resulting state vector can be used to estimate the eigenvalues of the Hamiltonian.
 
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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