Increased success probability in Hardy's nonlocality: Theory and demonstration

Tran, Duc-Minh; Nguyen, Van-Duy; Ho, Le Bin; Nguyễn, Hồng Quang

doi:10.1103/physreva.107.042210

Cited by 13 publications

(34 citation statements)

References 54 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…This model improves the success probability in demonstrating nonlocality for

-particle HNT. Simulating this success prevents the vanishing of

grows compared to previous models of the same study [37] . Quantum tunneling for QFTh (QFTh-QT) [12 , 17] .…”

Section: Introductionmentioning

confidence: 92%

“… One-dimensional Gaussian (1DG), as a nearly optimized algorithm for generating a ground state (GS) of a free QFTh [18] that can correspond to a classical field of free particles, Section 3. Lattice quantum field theory (LQFT) [5 , 14 , 16] , Hardy's nonlocality theory (HNT) to predict entanglement by measuring EE for a particle pair interaction at a large distance [37] . This model improves the success probability in demonstrating nonlocality for

-particle HNT.…”

Section: Introductionmentioning

confidence: 99%

“…Hardy's nonlocality theory (HNT) to predict entanglement by measuring EE for a particle pair interaction at a large distance [37] . This model improves the success probability in demonstrating nonlocality for

-particle HNT.…”

Section: Introductionmentioning

confidence: 99%

“…Depending on how consistent the model under review is in producing the expected results describing the system, the

is evaluated relative to uncertainty measure and error rates. For instance, data loss and uncertainty increase are expected for a system’s state under decoherence [7] , [8] , [9] , 37 , 52] , e.g., an AQO program running on a D-Wave device [40] . However, the mitigation process to address data loss as a solution in reconstructing or retrieving data, can be satisfied by other models, such as QDF [7] , [8] , [9] and AQOpt [51 , 52] , which discuss this

.…”

Section: Introductionmentioning

confidence: 99%

“…Simulators from [12 , 37 , 40] for specific QFTh cases satisfy values of

. A QDF model as QF-LCA from [7] , [8] , [9] , [10] , [11] , satisfies values of

for any QFTh.…”

Section: Introductionmentioning

confidence: 99%

See 4 more Smart Citations

Quantum AI and hybrid simulators for a Universal Quantum Field Computation Model

Alipour,

Gulliver

2023

MethodsX

View full text Add to dashboard Cite

“…This model improves the success probability in demonstrating nonlocality for

-particle HNT. Simulating this success prevents the vanishing of

grows compared to previous models of the same study [37] . Quantum tunneling for QFTh (QFTh-QT) [12 , 17] .…”

Section: Introductionmentioning

confidence: 92%

-particle HNT.…”

Section: Introductionmentioning

confidence: 99%

-particle HNT.…”

Section: Introductionmentioning

confidence: 99%

“…Depending on how consistent the model under review is in producing the expected results describing the system, the

.…”

Section: Introductionmentioning

confidence: 99%

“…Simulators from [12 , 37 , 40] for specific QFTh cases satisfy values of

. A QDF model as QF-LCA from [7] , [8] , [9] , [10] , [11] , satisfies values of

for any QFTh.…”

Section: Introductionmentioning

confidence: 99%

See 3 more Smart Citations

Quantum AI and hybrid simulators for a Universal Quantum Field Computation Model

Alipour,

Gulliver

2023

MethodsX

View full text Add to dashboard Cite

The Imaginary Universe

Łukaszyk

2023

Preprint

View full text Add to dashboard Cite

Maxwell’s equations in vacuum provide the negative speed of light $-c$, which leads to imaginary Planck units. However, the second, negative fine-structure constant $\alpha_2^{-1} \approx -140.178$, present in the Fresnel coefficients for the normal incidence of electromagnetic radiation on monolayer graphene, establishes the different, negative speed of light in vacuum $c_2 \approx -3.06 \times 10^8~\text{[m/s]}$, which introduces imaginary Planck units different in magnitude from those parametrized with $c$. It follows that electric charges are the same in real and imaginary dimensions. We model neutron stars and white dwarfs, emitting perfect black-body radiation, as \textit{objects} having energy exceeding their mass-energy equivalence ratios. We define complex energies in terms of real and imaginary natural units. Their imaginary parts, inaccessible for direct observation, store the excess of these energies. It follows that black holes are fundamentally uncharged, masses of charged neutron stars and white dwarfs satisfy $M \lesssim 5.7275 \times 10^{-10}~[\text{kg}]$, and the radii of white dwarfs' cores are limited to $R_{\text{WD}} \lesssim 3.3967~R_{\text{BH}}$, where $R_{\text{BH}}$ is the Schwarzschild radius of a white dwarf mass. It is conjectured that the maximum atomic number $Z=238$. A black-body \textit{object} is in the equilibrium of complex energies if its radius $R_\text{eq} \approx 1.3833~R_{\text{BH}}$, which is close to the photon sphere radius $R_{\text{ps}}=1.5~R_{\text{BH}}$, and marginally greater than a locally negative energy density bound of $4/3~R_{\text{BH}}$. Complex Newton’s law of universal gravitation, based on complex energies, leads to the black-body object's surface gravity and the generalized Hawking radiation temperature, which includes its charge. The proposed model takes into account the value(s) of the fine-structure constant(s), which is/are otherwise neglected in general relativity, and explains the registered (GWOSC) high masses of neutron stars' mergers and the associated fast radio bursts (CHIME) without resorting to any hypothetical types of exotic stellar \textit{objects}.

show abstract

Assembly Theory of Binary Messages (How to Assemble a Black Hole and Use it to Assemble New Binary Information?)

Łukaszyk,

Bieniawski

2024

Preprint

View full text Add to dashboard Cite

Using assembly theory, we investigate assembly pathways of fixed-length binary strings formed by joining the individual bits present in the assembly pool and the strings that entered the pool as a result of previous joining operations. We show that the string assembly index is bounded from below and above. We derive the lower bound and conjecture the upper bound's form. We conjecture that a black hole surface is defined by a balanced distinct string that satisfies the upper bound of a distinct string assembly index. The results confirm that four Planck areas provide the minimum information capacity that provides a minimum thermodynamic (Bekenstein-Hawking) entropy. Knowing that the problem of determining the assembly index is at least NP-complete, we conjecture that the problem of determining the assembly index of a given binary string is NP-complete, while the problem of creating the string so that it would have a predetermined maximum assembly index is NP-hard. Therefore, once the new information is assembled by a dissipative structure or by a human, increasing the information entropy according to the second law of infodynamics, it is subject to the second law of thermodynamics, and nature seeks to optimize its assembly pathway.

show abstract

Increased success probability in Hardy's nonlocality: Theory and demonstration

Cited by 13 publications

References 54 publications

Quantum AI and hybrid simulators for a Universal Quantum Field Computation Model

Quantum AI and hybrid simulators for a Universal Quantum Field Computation Model

The Imaginary Universe

Assembly Theory of Binary Messages (How to Assemble a Black Hole and Use it to Assemble New Binary Information?)

Contact Info

Product

Resources

About