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Related Concept Videos

Propagation of Uncertainty from Random Error00:59

Propagation of Uncertainty from Random Error

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An experiment often consists of more than a single step. In this case, measurements at each step give rise to uncertainty. Because the measurements occur in successive steps, the uncertainty in one step necessarily contributes to that in the subsequent step. As we perform statistical analysis on these types of experiments, we must learn to account for the propagation of uncertainty from one step to the next. The propagation of uncertainty depends on the type of arithmetic operation performed on...
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Thermal Sigmatropic Reactions: Overview01:16

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Sigmatropic rearrangements are a class of pericyclic reactions in which a σ bond migrates from one part of a π system to another. These are intramolecular rearrangements where the total number of σ and π bonds remain unchanged.
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Free Energy Changes for Nonstandard States03:25

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The free energy change for a process taking place with reactants and products present under nonstandard conditions (pressures other than 1 bar; concentrations other than 1 M) is related to the standard free energy change according to this equation:
 
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The Quantum-Mechanical Model of an Atom02:45

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Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
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Consider the two thermodynamic processes involving an ideal gas that are represented by paths AC and ABC in Figure 1:
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Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
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Gradient Echo Quantum Memory in Warm Atomic Vapor
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Holographic deep thermalization for secure and efficient quantum random state generation.

Bingzhi Zhang1,2, Peng Xu3, Xiaohui Chen4

  • 1Ming Hsieh Department of Electrical and Computer Engineering, University of Southern California, Los Angeles, CA, 90089, USA. bingzhiz@usc.edu.

Nature Communications
|July 9, 2025
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Summary
This summary is machine-generated.

This study introduces holographic deep thermalization, a secure and hardware-efficient method for generating quantum random states. It significantly reduces resource requirements and enhances security for quantum applications.

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Area of Science:

  • Quantum Information Science
  • Quantum Computing
  • Quantum Cryptography

Background:

  • Genuine random pure states are crucial for quantum physics and applications like quantum device benchmarking.
  • Conventional deep thermalization methods for generating random states face scalability and security challenges.
  • Attacks can compromise the security of existing quantum random state generators.

Purpose of the Study:

  • To develop a secure and hardware-efficient quantum random state generator.
  • To overcome the limitations of conventional deep thermalization methods.
  • To enable reliable quantum advantage certification and benchmarking.

Main Methods:

  • Introduction of holographic deep thermalization, a novel approach for quantum random state generation.
  • Utilizing a sequence of scrambling-measure-reset processes to trade space with time.
  • Implementing a circuit-based approach on IBM Quantum devices.

Main Results:

  • Substantial reduction in the required ancilla size to a system-size-independent constant.
  • Guaranteed security by eliminating quantum correlations between the data system and potential attackers.
  • Successful generation of genuine 5-qubit random states using only 8 qubits on IBM Quantum devices.

Conclusions:

  • Holographic deep thermalization offers a secure and hardware-efficient solution for quantum random state generation.
  • The method significantly reduces resource overhead, making it more practical for real-world applications.
  • This advancement facilitates robust quantum device benchmarking and quantum advantage certification.