BSM-SG Qubit Implementation

1. What do we know about nuclear spin according to the BSM-SG theory?

šŸ”¹ Nuclear spin is a fundamental property of atomic nuclei, related to the number of protons and neutrons.

šŸ”¹ Spin numbers have been determined empirically through nuclear magnetic resonance (NMR) and experiments on magnetic moments.

šŸ”¹ In the BSM-SG theory, the structure of the nucleus is formed by the Cosmic Lattice and Supergravitational forces, which suggests that nuclear spin can be determined through the internal structural characteristics of the nucleons.

2. Possibility to derive nuclear spin via BSM-SG

šŸ”¹ Using the internal geometry of the nucleons and their positions in the nucleus according to BSM-SG, it is possible to model the spin vector resulting from the coupling of all nuclear components.

šŸ”¹ This approach allows predicting nuclear spin based on theoretical principles instead of relying solely on empirical data.

3. What do we know about quantum spin?

šŸ”¹ Quantum spin is a fundamental property of elementary particles, manifesting as intrinsic angular momentum.

šŸ”¹ It is quantized and described using spin operators and Hilbert space formalism.

šŸ”¹ Spin is responsible for the magnetic moment of particles and plays a key role in quantum entanglement, statistics (Fermi-Dirac vs Bose-Einstein), and selection rules in atomic transitions.

4. Possibility of describing quantum spin from the perspective of BSM-SG theory

šŸ”¹ In BSM-SG, quantum spin arises from the internal dynamic structure of particles formed by twisted energy tubes and interactions with the Cosmic Lattice.

šŸ”¹ Spin is not an abstract quantum number but a manifestation of internal substructure and motion in space.

šŸ”¹ This description enables a physical understanding of spin orientation, polarization, and its influence on particle interactions.

5. Differences between classical and quantum spin

šŸ”¹ Classical spin corresponds to the rotation of a macroscopic object, described by vectors and moments of inertia.

šŸ”¹ Quantum spin has no classical analog; it is an intrinsic property with fixed values (e.g., 1/2, 1, 3/2).

šŸ”¹ Quantum spin exhibits phenomena such as superposition, entanglement, and quantum tunneling, which are not observed in classical systems.

6. How can we use the spin of a particle to simulate a quantum qubit?

šŸ”¹ A quantum qubit can be represented by the two spin states of a spin-1/2 particle: spin-up |ā†‘āŸ© and spin-down |ā†“āŸ©.

šŸ”¹ These states form the computational basis {|0āŸ©, |1āŸ©}, and any superposition Ī±|0āŸ© + Ī²|1āŸ© is a valid quantum state.

šŸ”¹ Spin qubits are controlled by magnetic or electric fields and measured through spin-dependent interactions (e.g., fluorescence or tunneling).

7. Applications of spin-based quantum simulation

šŸ”¹ Modeling quantum materials and magnetism.

šŸ”¹ Studying strongly correlated systems.

šŸ”¹ Quantum sensing with high spatial resolution (e.g., using NV centers in diamond).

šŸ”¹ Simulation of fundamental interactions (quantum chromodynamics models).

2025 Victor Pronchev