2021
DOI: 10.1002/qua.26853
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State preparation and evolution in quantum computing: A perspective from Hamiltonian moments

Abstract: Quantum algorithms on noisy intermediate-scale quantum (NISQ) devices are expected to soon simulate quantum systems that are classically intractable. However, the non-negligible gate error present on NISQ devices impedes the implementation of many purely quantum algorithms, necessitating the use of hybrid quantum-classical algorithms. One such hybrid quantum-classical algorithm, is based upon quantum computed Hamiltonian moments ϕj Ĥn jϕ D E n ¼ 1,2,ÁÁÁ ð Þ , with respect to quantum state j ϕi. In this tutoria… Show more

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Cited by 22 publications
(13 citation statements)
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“…ITE is an iterative computational method to solve the ground‐state of many‐body quantum systems. [ 51 ] Consider the time‐independent Schrödinger equation in imaginary time (tιt$t\rightarrow -\iota t$) |ϕ(t)t=scriptĤfalse|ϕ(t)false⟩$$\begin{align} \frac{\partial |\phi (t)\rangle }{\partial t}=-\hat{\mathcal {H}}|\phi (t)\rangle \end{align}$$where false|ϕfalse(tfalse)false⟩$|\phi (t)\rangle$ is a quantum state at time t and scriptĤ$\hat{\mathcal {H}}$ is the Hamiltonian. The formal solution of Equation (20) can be expressed as |ϕfalse(tfalse)=etrueĤt|ϕfalse(0false)$|\phi (t)\rangle =e^{-\hat{\mathcal {H}}t}|\phi (0)\rangle$, where false|ϕfalse(0false)false⟩$|\phi (0)\rangle$ is an initial state at time t=0$t=0$.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…ITE is an iterative computational method to solve the ground‐state of many‐body quantum systems. [ 51 ] Consider the time‐independent Schrödinger equation in imaginary time (tιt$t\rightarrow -\iota t$) |ϕ(t)t=scriptĤfalse|ϕ(t)false⟩$$\begin{align} \frac{\partial |\phi (t)\rangle }{\partial t}=-\hat{\mathcal {H}}|\phi (t)\rangle \end{align}$$where false|ϕfalse(tfalse)false⟩$|\phi (t)\rangle$ is a quantum state at time t and scriptĤ$\hat{\mathcal {H}}$ is the Hamiltonian. The formal solution of Equation (20) can be expressed as |ϕfalse(tfalse)=etrueĤt|ϕfalse(0false)$|\phi (t)\rangle =e^{-\hat{\mathcal {H}}t}|\phi (0)\rangle$, where false|ϕfalse(0false)false⟩$|\phi (0)\rangle$ is an initial state at time t=0$t=0$.…”
Section: Methodsmentioning
confidence: 99%
“…ITE is an iterative computational method to solve the groundstate of many-body quantum systems. [51] Consider the timeindependent Schrödinger equation in imaginary time (t → −𝜄t)…”
Section: The Selection Of the Learning Ratementioning
confidence: 99%
“…In a similar vein, quantum computers can be employed to prepare entangled states with sizable overlap with the true ground state and carry out the subsequent measurements in an efficient fashion. This can pave the way for widespread adoption of methodologies which estimate the ground state energy based on moments of the Hamiltonian [113][114][115][116][117], which share some commonalities with ITE [118], and real-time evolution on the grounds of Krylov basis ideas [66].…”
Section: Variational Quantum Eigensolver and Variantsmentioning
confidence: 99%
“…ITE is an iterative computational method to solve the ground-state of many-body quantum systems [51]. Consider the time-independent Schrödinger equation in imaginary time (t → −ιt),…”
Section: The Selection Of the Learning Ratementioning
confidence: 99%