FeSe Superconducting Film Epitaxy and FeTe Protection

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Solution Overview

Problem

Iron-based high-temperature superconducting films often have inhomogeneous structures and many impurities, which affect the study of superconductivity mechanisms and hinder the understanding of superconducting properties.

Innovation Solution

A high-temperature superconducting film is created using a SrTiO3 substrate with a single crystalline FeSe layer epitaxially grown on it, and a protective FeTe layer is added to prevent oxidation and impurity adsorption, resulting in atomically smooth interfaces and enhanced superconducting properties.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Manufacturing precision

If iron-based high-temperature superconducting films are prepared by Pulsed Laser Deposition (PLD), then the films can be synthesized, but they comprise inhomogeneous structure and many impurities

Engineering Contradiction:
Improvestructural homogeneityVSAvoidfilm quality
Core Design Contradiction:
Manufacturing precisionVSReliability

Solution Approach 1:

The patent employs molecular beam epitaxy (MBE) instead of PLD, fundamentally changing the deposition parameters and method. MBE allows for precise control of deposition rates, temperature, and vacuum conditions, enabling the growth of homogeneous single-crystalline FeSe films without the inhomogeneities and impurities associated with PLD

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent introduces a protective FeTe layer specifically at the surface of the FeSe film to prevent oxidation and impurity adsorption. This local protective measure addresses the quality issue without affecting the bulk properties of the superconducting FeSe layer

Inventive Principle:
Principle #3Local quality

2Reliability

If protective layer is added to prevent oxidation and impurity adsorption, then superconducting properties are preserved, but device complexity increases

Engineering Contradiction:
Improvesuperconducting property stabilityVSAvoidfilm structure complexity
Core Design Contradiction:
ReliabilityVSDevice complexity

Solution Approach 1:

The patent creates a composite structure by combining FeSe and FeTe layers. The FeTe layer serves as a protective coating that prevents oxidation and impurity adsorption on the FeSe surface, while maintaining the superconducting properties of the underlying FeSe layer. This composite approach solves the protection need without requiring complex external environments

Inventive Principle:
Principle #40Composite materials

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

The approach results in a high-quality, single crystalline FeSe film with a superconducting transition temperature of at least 54.5 K and a critical current density of 106 A/cm² at 12 K, minimizing external influences and preserving superconductivity.

Implementation Method 1

a single crystalline FeSe layer epitaxially grown on it

Methodology Applied
Scientific EffectEpitaxial growth: Epitaxy

Implementation Method 2

a protective FeTe layer is added to prevent oxidation and impurity adsorption

Methodology Applied
Scientific EffectAdsorption prevention: Adsorption

Implementation Method 3

a superconducting transition temperature of at least 54.5 K

Methodology Applied
Scientific EffectSuperconductivity: Superconductivity

Data Source

PatentUS9461233B2High-temperature superconducting film
Publication Date: 2016.10.04 TSINGHUA UNIVERSITY
  • US9461233B2 patent drawing
  • US9461233B2 patent drawing
  • US9461233B2 patent drawing

AI summary

A high-temperature superconducting film includes a SrTiO3 substrate, a single crystalline FeSe layer, and a protective layer with a layered crystal structure. The single crystalline FeSe layer is sandwiched between the SrTiO3 substrate and the protective layer via a layer-by-layer mode. An onset temperature of superconducting transition of the high-temperature superconducting film is greater than or equal to 54 K, and a critical current density of the high-temperature superconducting film is about 106 A/cm2 at 12 K.