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Protein-protein Interfaces02:04

Protein-protein Interfaces

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Many proteins form complexes to carry out their functions, making protein-protein interactions (PPIs) essential for an organism's survival. Most PPIs are stabilized by numerous weak noncovalent chemical forces. The physical shape of the interfaces determines the way two proteins interact. Many globular proteins have closely-matching shapes on their surfaces, which form a large number of weak bonds. Additionally, many PPIs occur between two helices or between a surface cleft and a...
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Protein-Protein Interfaces02:04

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Factors Affecting Dissolution: Polymorphism, Amorphism and Pseudopolymorphism01:21

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Polymorphism refers to the existence of a drug substance in multiple crystalline forms, known as polymorphs. Recently, this term has been expanded to include solvates (forms containing a solvent), amorphous forms (non-crystalline forms), and desolvated solvates (forms from which the solvent has been removed).
Some polymorphic crystals possess lower aqueous solubility than their amorphous counterparts, leading to incomplete absorption. For instance, the oral suspension of Chloramphenicol, which...
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Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)

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Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
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Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)

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Vicinal or three-bond coupling is commonly observed between protons attached to adjacent carbons. Here, nuclear spin information is primarily transferred via electron spin interactions between adjacent C‑H bond orbitals. This generally favors the antiparallel arrangement of spins, so 3J values are usually positive.
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the involved orbitals. The...
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G-protein Coupled Receptors01:21

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G-protein coupled receptors are ligand binding receptors that indirectly affect changes in the cell. The actual receptor is a single polypeptide that transverses the cell membrane seven times creating intracellular and extracellular loops. The extracellular loops create a ligand specific pocket which binds to neurotransmitters or hormones. The intracellular loops holds onto the G-protein.
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Updated: Feb 16, 2026

P300-Based Brain-Computer Interface Speller Performance Estimation with Classifier-Based Latency Estimation
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P300-Based Brain-Computer Interface Speller Performance Estimation with Classifier-Based Latency Estimation

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Strongly coupled interface ferroelectricity and interface superconductivity in amorphous LaAlO3/KTaO3(111).

M D Dong1,2,3, X B Cheng1,2,3, M Zhang4

  • 1Department of Physics, School of Science, Westlake University, Hangzhou, 310024, China.

Nature Communications
|February 14, 2026
PubMed
Summary

We discovered ferroelectric order in amorphous LaAlO3/KTaO3 interfaces, where ferroelectricity and superconductivity coexist. This ferroelectric superconductivity allows non-volatile control of superconducting properties.

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Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Solid-State Chemistry

Background:

  • Interfaces between oxides exhibit emergent phenomena due to distinct charge, spin, and orbital orders.
  • Coexistence of ferroelectricity and superconductivity is rare due to their often-competing nature.

Purpose of the Study:

  • To investigate the presence of ferroelectric order at the amorphous LaAlO3/KTaO3(111) interface.
  • To explore the coupling between ferroelectricity and superconductivity in this system.
  • To demonstrate non-volatile control of superconductivity via ferroelectric polarization.

Main Methods:

  • Scanning Transmission Electron Microscopy (STEM) to observe atomic displacements.
  • Second Harmonic Generation (SHG) microscopy for ferroelectric confirmation.
  • Piezoelectric Force Microscopy (PFM) to probe and switch ferroelectric polarization.
  • Electrical transport measurements to assess conductivity and superconductivity.

Main Results:

  • Evidence of ferroelectric order confirmed by STEM, SHG, and PFM, showing K atom displacement facilitated by oxygen vacancies.
  • Switching ferroelectric polarization significantly reduced interfacial conductivity (>1000x) and suppressed superconductivity.
  • Ferroelectric hysteresis correlated with changes in conductivity and superconducting transition temperature (Tc), indicating strong coupling.

Conclusions:

  • Demonstrated coexistence of ferroelectricity and superconductivity at the amorphous LaAlO3/KTaO3 interface.
  • Established ferroelectric control over superconductivity, opening avenues for novel electronic devices.
  • Paved the way for ferroelectric superconductivity with broken inversion symmetry and non-volatile switching capabilities.