Lucas Oriens Kim

[Deep Dive] Superconducting Hydride Mg2RhH6 Experimentally Achieved at Lower Pressure

Deep-Dive

[Deep Dive] Superconducting Hydride Mg2RhH6 Experimentally Achieved at Lower Pressure

🔬 DEEP DIVE ANALYSIS Superconducting Hydride Mg2RhH6 Experimentally Achieved at Lower Pressure Superconductivity • August 18, 2026 Reading time: ~12 minutes 📑 Contents 1. Executive Summary 2. Technical Deep Dive 3. Market Landscape 4. Timeline & Milestones 5. Investment Perspective 6. Key Takeaways 📊 Executive Summary Hydride superconductivity has spent a decade trading temperature

By Lucas Oriens Kim

Superconductor-Lab

[Superconductor Lab | Week 25 Day 5] Li₂(Mg₁₋ₓSrₓ)BeH₁₆ and Li₂(Mg₁₋ₓBaₓ)BeH₁₆, plus decompression-recovery screening of all Week-25 leads - AI Simulator Activation

[Week 25 Day 5] Li₂(Mg₁₋ₓSrₓ)BeH₁₆ and Li₂(Mg₁₋ₓBaₓ)BeH₁₆, plus decompression-recovery screening of all Week-25 leads Superconductor Lab — AI Simulator Activation 2026 🔬 Computational Research Note This analysis is based on computational modeling and theoretical predictions. As with all computational materials science, experimental validation is needed to

By Lucas Oriens Kim

Superconductor-Lab

[Superconductor Lab | Week 25 Day 4] (Li₂₋ᵢNaᵢ)(Mg₁₋ₓCaₓ)BeH₁₆ and (Li₂₋ᵢKᵢ)(Mg₁₋ₓCaₓ)BeH₁₆, i = 0.0–1.0 - AI Simulator Activation

[Week 25 Day 4] (Li₂₋ᵢNaᵢ)(Mg₁₋ₓCaₓ)BeH₁₆ and (Li₂₋ᵢKᵢ)(Mg₁₋ₓCaₓ)BeH₁₆, i = 0.0–1.0 Superconductor Lab — AI Simulator Activation 2026 🔬 Computational Research Note This analysis is based on computational modeling and theoretical predictions. As with all computational materials science, experimental validation is needed to

By Lucas Oriens Kim

Superconductor-Lab

[Superconductor Lab | Week 25 Day 3] Li₂(Mg₁₋ₓCaₓ)(Be₁₋ᵧBᵧ)H₁₆ pressure-descent study, y = 0.05–0.30, P = 80–200 GPa - AI Simulator Activation

[Week 25 Day 3] Li₂(Mg₁₋ₓCaₓ)(Be₁₋ᵧBᵧ)H₁₆ pressure-descent study, y = 0.05–0.30, P = 80–200 GPa Superconductor Lab — AI Simulator Activation 2026 🔬 Computational Research Note This analysis is based on computational modeling and theoretical predictions. As with all computational materials science, experimental validation is needed

By Lucas Oriens Kim

Superconductor-Lab

[Superconductor Lab | Week 25 Day 2] Li₂(Mg₀.₅₅Ca₀.₄₅₋ₓREₓ)BeH₁₆ with RE = Y, La, Sc, Ce at dilute x = 0.02–0.15 - AI Simulator Activation

[Week 25 Day 2] Li₂(Mg₀.₅₅Ca₀.₄₅₋ₓREₓ)BeH₁₆ with RE = Y, La, Sc, Ce at dilute x = 0.02–0.15 Superconductor Lab — AI Simulator Activation 2026 🔬 Computational Research Note This analysis is based on computational modeling and theoretical predictions. As with all computational materials science, experimental validation is

By Lucas Oriens Kim
[Deep Dive] Thermal Hall tomography of chiral superconductivity in rhombohedral graphene

Deep-Dive

[Deep Dive] Thermal Hall tomography of chiral superconductivity in rhombohedral graphene

🔬 DEEP DIVE ANALYSIS Thermal Hall tomography of chiral superconductivity in rhombohedral graphene Superconductivity • August 15, 2026 Reading time: ~12 minutes 📑 Contents 1. Executive Summary 2. Technical Deep Dive 3. Market Landscape 4. Timeline & Milestones 5. Investment Perspective 6. Key Takeaways 📊 Executive Summary Rhombohedral graphene has become the first platform

By Lucas Oriens Kim

Superconductor-Lab

[Superconductor Lab | Week 25 Day 1] Li₂(Mg₁₋ₓCaₓ)BeH₁₆ (fine composition grid, x = 0.00–1.00 in Δx = 0.02) with explicit anharmonic phonon validation - AI Simulator Activation

[Week 25 Day 1] Li₂(Mg₁₋ₓCaₓ)BeH₁₆ (fine composition grid, x = 0.00–1.00 in Δx = 0.02) with explicit anharmonic phonon validation Superconductor Lab — AI Simulator Activation 2026 🔬 Computational Research Note This analysis is based on computational modeling and theoretical predictions. As with all computational materials science,

By Lucas Oriens Kim