Photo-thermal Chemical Imaging via Scanning Probe Microscopy

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Solution Overview

Problem

Current chemical imaging techniques lack the necessary spatial resolution, are often destructive, require extensive sample preparation, and are not suitable for a wide range of samples, particularly microfabricated devices and organic compounds, with existing methods like FTIR, Raman, and photo-thermal spectroscopy having limitations in resolution and practicality.

Innovation Solution

A non-destructive, non-contact photo-thermal chemical imaging method using IR lasers or focused electron/ion beams to achieve high spatial resolution (1-50 nm) without sample preparation, allowing for molecular information mapping with improved resolution and rapid scan rates, capable of handling samples with surface roughness and fluorescence.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If FTIR micro-spectroscopy is used to achieve chemical composition mapping, then spatial resolution is improved to about 20 μm, but the resolution is still insufficient for nanoscale imaging

Engineering Contradiction:
Improvespatial resolutionVSAvoidspatial resolution limit
Core Design Contradiction:
Measurement precisionVSManufacturing precision

Solution Approach 1:

The patent replaces conventional optical FTIR micro-spectroscopy with a scanning probe microscopy-based photo-thermal technique. The mechanical scanning probe system enables sub-100 nm spatial resolution by using a physical probe to detect local thermal changes, bypassing the diffraction limit of optical methods while maintaining chemical specificity through photo-thermal spectroscopy.

Inventive Principle:
Principle #28Mechanics substitution (Replace mechanical system)

Solution Approach 2:

The patent changes the detection parameter from direct IR absorption measurement to photo-thermal signal measurement. By monitoring thermal changes induced by localized IR heating, the system achieves enhanced spatial resolution beyond the optical diffraction limit, as thermal diffusion lengths can be controlled to be much smaller than the IR wavelength.

Inventive Principle:
Principle #35Parameter changes

2Measurement precision

If Raman micro-spectroscopy is used to achieve adequate spatial resolution (∼1 μm), then the process becomes inefficient with extremely low signal response levels, necessitating long integration times and expensive detectors

Engineering Contradiction:
Improvespatial resolutionVSAvoidscan time
Core Design Contradiction:
Measurement precisionVSProductivity

Solution Approach 1:

The patent converts the typically harmful thermal effects (which cause sample damage or require complex cooling) into a beneficial signal. By using photo-thermal spectroscopy, the localized heating induced by the IR laser is detected as a positive signal through thermal lensing or thermal expansion, providing strong contrast without requiring expensive cryogenic detectors or long integration times.

Inventive Principle:
Principle #22Blessing in disguise (Convert harm into benefit)

Solution Approach 2:

The patent exploits thermal phase transitions and thermal expansion of the sample material as the detection mechanism. The localized heating causes measurable changes in refractive index, physical dimensions, or thermal conductivity, which are detected by the scanning probe, providing a strong signal that enables rapid scanning without long integration times.

Inventive Principle:
Principle #36Phase transitions

3Measurement precision

If atomic force microscopy with photo-thermal effect is used to achieve chemical imaging with 0.1 μm resolution, then specialized sample preparation is required including microtoming to 10 μm thin and physical contact with prism substrate and scanning probe tip

Engineering Contradiction:
Improvespatial resolutionVSAvoidsample preparation
Core Design Contradiction:
Measurement precisionVSEase of manufacture

Solution Approach 1:

The patent creates a universal imaging technique that can analyze diverse sample types (solids, liquids, gases, powders) without requiring specialized preparation. The scanning probe photo-thermal method works on bulk samples, thin films, and heterogeneous materials alike, eliminating the need for microtoming or specific substrate mounting required by conventional AFM-photo-thermal techniques.

Inventive Principle:
Principle #6Universality (Multi-functionality)

Solution Approach 2:

The patent extracts and eliminates the restrictive sample preparation steps from the imaging process. By using a scanning probe that can detect photo-thermal signals from the sample surface or near-surface region, the technique removes the requirement for thin sectioning and specialized mounting, allowing direct analysis of samples in their native state.

Inventive Principle:
Principle #2Taking out (Extraction)

4Quantity of substance

If PT-IRIS with quantum cascade lasers is used to map chemical composition, then the spatial resolution is diffraction limited by the long wavelength of the heating source and thermal emission

Engineering Contradiction:
Improvechemical composition mappingVSAvoidspatial resolution
Core Design Contradiction:
Quantity of substanceVSMeasurement precision

Solution Approach 1:

The patent introduces a scanning probe as an intermediary between the IR heating source and the detection system. The probe locally senses the photo-thermal effects with sub-diffraction precision, acting as a spatial filter that confines the measurement volume to a small region around the probe tip, thereby achieving spatial resolution much better than the IR wavelength would otherwise permit.

Inventive Principle:
Principle #24Intermediary (Mediator)

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 method provides over an order of magnitude improvement in spatial resolution compared to FTIR micro-spectroscopy, enabling detailed chemical imaging of microfabricated structures and organic compounds with simultaneous acquisition of confocal microscopy images and thermal properties, while being independent of sample form and surface roughness.

Implementation Method 1

a sample undergoes photo-thermal heating using an IR laser and the resulting increase in thermal emissions is measured

Methodology Applied
Scientific EffectPhoto-thermal heating: Absorption (EM radiation)

Implementation Method 2

the resulting increase in thermal emissions is measured with either an IR detector or a laser probe

Methodology Applied
Scientific EffectThermal radiation: Thermal Radiation

Implementation Method 3

the infrared laser is replaced with a focused electron or ion source while the thermal emission is collected

Methodology Applied
Scientific EffectElectron beam heating: Electron Beam

Implementation Method 4

the infrared laser is replaced with a focused electron or ion source while the thermal emission is collected

Methodology Applied
Scientific EffectIon beam heating: Ion Beam

Implementation Method 5

a laser probe having a visible laser reflected from the sample

Methodology Applied
Scientific EffectLight reflection: Reflection

Data Source

PatentUS9841324B2Chemical mapping using thermal microscopy at the micro and nano scales
Publication Date: 2017.12.12 THE UNITED STATES OF AMERICA AS REPRESENTED BY THE SECRETARY OF THE NAVY
  • US9841324B2 patent drawing
  • US9841324B2 patent drawing
  • US9841324B2 patent drawing

AI summary

A non-destructive method for chemical imaging with ˜1 nm to 10 μm spatial resolution (depending on the type of heat source) without sample preparation and in a non-contact manner. In one embodiment, a sample undergoes photo-thermal heating using an IR laser and the resulting increase in thermal emissions is measured with either an IR detector or a laser probe having a visible laser reflected from the sample. In another embodiment, the infrared laser is replaced with a focused electron or ion source while the thermal emission is collected in the same manner as with the infrared heating. The achievable spatial resolution of this embodiment is in the 1-50 nm range.