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IBM Q Experience as a versatile experimental testbed for simulating open quantum systems
Quantum Physics · Submitted 17 Jun 2019
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Our main result is to prove the great versatility of the IBM Q Experience processors.
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The abstract, sentence by sentence
The advent of Noisy Intermediate-Scale Quantum (NISQ) technology is changing rapidly the landscape and modality of research in quantum physics. NISQ devices, such as the IBM Q Experience, have very recently proven their capability as experimental platforms accessible to everyone around the globe. Until now, IBM Q Experience processors have mostly been used for quantum computation and simulation of closed systems. Here we show that these devices are also able to implement a great variety of paradigmatic open quantum systems models, hence providing a robust and flexible testbed for open quantum systems theory. During the last decade an increasing number of experiments have successfully tackled the task of simulating open quantum systems in different platforms, from linear optics to trapped ions, from Nuclear Magnetic Resonance (NMR) to Cavity Quantum Electrodynamics. Generally, each individual experiment demonstrates a specific open quantum system model, or at most a specific class. Our main result is to prove the great versatility of the IBM Q Experience processors. Indeed, we experimentally implement one and two-qubit open quantum systems, both unital and non-unital dynamics, Markovian and non-Markovian evolutions. Moreover, we realise proof-of-principle reservoir engineering for entangled state generation, demonstrate collisional models, and verify revivals of quantum channel capacity and extractable work, caused by memory effects. All these results are obtained using IBM Q Experience processors publicly available and remotely accessible online.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The advent of Noisy Intermediate-Scale Quantum (NISQ) technology is changing rapidly the landscape and modality of research in quantum physics. | background 1.00 | 0.04 | 0.02 | asserted 1.00 |
| s1 | NISQ devices, such as the IBM Q Experience, have very recently proven their capability as experimental platforms accessible to everyone around the globe. | background 1.00 | 0.08 | 0.02 | asserted 1.00 |
| s2 | Until now, IBM Q Experience processors have mostly been used for quantum computation and simulation of closed systems. | gap 0.70 | 0.07 | 0.02 | asserted 0.98 |
| s3 | Here we show that these devices are also able to implement a great variety of paradigmatic open quantum systems models, hence providing a robust and flexible testbed for open quantum systems theory. | contribution 0.95 | 0.92 | 0.72 | asserted 1.00 |
| s4 | During the last decade an increasing number of experiments have successfully tackled the task of simulating open quantum systems in different platforms, from linear optics to trapped ions, from Nuclear Magnetic Resonance (NMR) to Cavity Quantum Electrodynamics. | background 1.00 | 0.03 | 0.02 | asserted 1.00 |
| s5 | Generally, each individual experiment demonstrates a specific open quantum system model, or at most a specific class. | gap 0.51 | 0.04 | 0.02 | asserted 0.94 |
| s6 | Our main result is to prove the great versatility of the IBM Q Experience processors. | result 0.56 | 0.84 | 0.95 | asserted 1.00 |
| s7 | Indeed, we experimentally implement one and two-qubit open quantum systems, both unital and non-unital dynamics, Markovian and non-Markovian evolutions. | result 0.57 | 0.96 | 0.15 | asserted 1.00 |
| s8 | Moreover, we realise proof-of-principle reservoir engineering for entangled state generation, demonstrate collisional models, and verify revivals of quantum channel capacity and extractable work, caused by memory effects. | result 0.66 | 0.96 | 0.07 | asserted 1.00 |
| s9 | All these results are obtained using IBM Q Experience processors publicly available and remotely accessible online. | method 0.90 | 0.74 | 0.05 | asserted 1.00 |
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The paper
Original abstract
The advent of Noisy Intermediate-Scale Quantum (NISQ) technology is changing rapidly the landscape and modality of research in quantum physics. NISQ devices, such as the IBM Q Experience, have very recently proven their capability as experimental platforms accessible to everyone around the globe. Until now, IBM Q Experience processors have mostly been used for quantum computation and simulation of closed systems. Here we show that these devices are also able to implement a great variety of paradigmatic open quantum systems models, hence providing a robust and flexible testbed for open quantum systems theory. During the last decade an increasing number of experiments have successfully tackled the task of simulating open quantum systems in different platforms, from linear optics to trapped ions, from Nuclear Magnetic Resonance (NMR) to Cavity Quantum Electrodynamics. Generally, each individual experiment demonstrates a specific open quantum system model, or at most a specific class. Our main result is to prove the great versatility of the IBM Q Experience processors. Indeed, we experimentally implement one and two-qubit open quantum systems, both unital and non-unital dynamics, Markovian and non-Markovian evolutions. Moreover, we realise proof-of-principle reservoir engineering for entangled state generation, demonstrate collisional models, and verify revivals of quantum channel capacity and extractable work, caused by memory effects. All these results are obtained using IBM Q Experience processors publicly available and remotely accessible online.
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References
How later papers used it
70 later papers cite it
1 later paper by other authors is listed below: 1 used its method or tool.
Uses its method or tool 1 of 8 papers with this label
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For this, we consider the Amplitude damping channel (AD) with the angle $θ$ defined as [ref] : [equation] where $p_AD(t)$ is given by [equation] where $r=√(2γ_s-γ_s^2)$ and $γ_s$ correspond to the SPEs damping rate as in Eq. [ref], and the dephasing is not included here explicitly since it appears as an intrinsic noise of the quantum simulator.
Generation of phonon quantum states and quantum correlations among single photon emitters in hexagonal boron nitride (2023) · Quantum circuit for the IBM Quantum Simulator · 0.85
How the literature uses it
6 arXiv papers cite this in 6 sentences
Papers citing it · 4 sentences without a confident label
Cites it as background 2 papers
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In addition, the emergence of quantum computing opens new opportunities and challenges for the simulation of OQS [ref] .
Unitary Dynamics for Open Quantum Systems with Density-Matrix Purification · Introduction · 0.88
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The amplitude damping channel can be written in terms of the Kraus operators $K_1 = [ 1 0; 0 Γ ]$ and $K_2 = [ 0 √(1-|Γ|^2); 0 0 ]$, which arise e.g. from the Jaynes-Cummings model of a qubit system interacting with a quantized bosonic field [ref] .
Compressive gate set tomography · Gate set and measurement structure · 0.85
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