Micro-Thermal Analysis: Techniques and Applications

Micro-Thermal Analysis: Techniques and Applications

INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS D: APPLIED PHYSICS J. Phys. D: Appl. Phys. 34 (2001) R23–R53 www.iop.org/Journals/jd PII: S0022-3727(01)07217-5 TOPICAL REVIEW Micro-thermal analysis: techniques and applications H M Pollock and A Hammiche Department of Physics, Lancaster University, Lancaster LA1 4YB, UK E-mail: [email protected] Received 21 December 2000 Abstract The terms micro-thermal analysis and micro-spectroscopic analysis are used to include any form of localized characterization or analysis combined with microscopy that uses a near-field thermal probe to exploit the benefits of using thermal excitation. Individual regions of a solid sample are selected by means of surface or sub-surface imaging (atomic force microscopy and/or scanning thermal microscopy), so as to add spatial discrimination to four well-established methods of chemical fingerprinting, namely thermomechanometry, calorimetry, spectroscopy and analytical pyrolysis. We begin by describing the state of the art of scanning microscopy that uses resistive thermal probes, followed by an account of the various techniques of micro-thermal analysis. Modern materials technology is increasingly concerned with the control of materials at the mesoscale. The ability to add an extra dimension of, say, chemical composition information to high-resolution microscopy, or microscopic information to spectroscopy, plays an increasingly useful part in applied research. Micro-thermal analysis is now being used commercially to visualize the spatial distribution of phases, components and contaminants in polymers, pharmaceuticals, foods, biological materials and electronic materials. This review outlines various applications that have been described in the literature to date, the topics ranging from multi-layer packaging materials and interphase regions in composites, to the use of the technique as a means of surface treatment. Contents 1. Introduction 23 2. Scanning thermal microscopy 24 2.1. Thermal microscopy using resistive probes 25 2.2. Use of temperature modulation 28 2.3. Scanning thermal expansion microscopy 31 2.4. Measurement of the absolute thermal properties of materials on a sub-µm scale 32 3. Variants of micro-thermal and micro-spectroscopic analysis 34 3.1. Localized thermomechanometry 34 3.2. Localized calorimetry 35 3.3. Dynamic localized thermomechanical analysis 36 3.4. Localized thermo-rheometry 36 3.5. Localized gas chromatography-mass spectrometry 38 3.6. Near-field photothermal infrared spectroscopy 38 4. Applications 40 4.1. Distinguishing different constituents of a heterogeneous material: various examples 40 4.2. Polymorphic forms of polymers: thermal history 45 4.3. Identification of a contaminant or surface film 46 4.4. Biological applications 46 4.5. Microelectronics applications 47 4.6. Interfaces and interphases 47 5. Concluding remarks 49 0022-3727/01/090023+31$30.00 © 2001 IOP Publishing Ltd Printed in the UK R23 Topical review List of acronyms as used here, it includes any form of localized characterization or analysis combined with microscopy, that uses a near- AFM atomic force microscopy field thermal probe. Micro-thermal analysis was launched BLE best linear estimate commercially in March 1998 (µTA ™ Micro-Thermal Analyser CVD chemical vapour deposited (T A Instruments, New Castle, USA)), and two aspects of its DSC differential scanning calorimetry development encourage the development of future variants. FFT fast Fourier transform (FT)-IR (Fourier transform)-infrared (a) As in other forms of scanning probe microscopy, (GC)-MS (gas chromatography)-mass spectrometry ‘near-field’ imaging1 is achieved (‘scanning thermal L-CA localized calorimetric analysis microscopy’ (SThM)). We shall see that thermal imaging (L)-DMA (localized)-dynamic mechanical analysis contrast is used to reveal spatial variations in the thermal (L)-DTA (localized)-differential thermal analysis conductivity and diffusivity of the sample, and that a (L)-TA (localized)-thermal analysis particular advantage of SThM is its ability to detect sub- (L)-TMA (localized)-thermomechanical analysis surface structure. OPG optical parametric generator (b) Localized thermal/spectroscopic analysis builds upon this SThEM scanning thermal expansion microscopy near-field thermal imaging technique, in order to add SThM scanning thermal microscopy spatial discrimination to four well-established methods TASM tomographic analysis for scanning microscopy of chemical fingerprinting, namely thermomechanometry, Tg glass transition temperature calorimetry, spectroscopy and analytical pyrolysis. The same probe may be used in each version of the technique 1. Introduction so that, as we shall describe, in principle it is possible to combine, in one instrument, a number of different modes In a wide variety of new forms of analytical instrumentation of analysis—as well as surface topographic imaging by we see one common feature: quantitative analysis or physical atomic force microscopy (AFM). The source of thermal characterization is combined with the ability to record excitation may be the near-field thermal probe itself, microscope images, and thus to choose individual regions of an used both as a heater and as a thermometer (‘active’ inhomogeneous sample for analysis. To give just one example, thermal probe), for localized application of temperature the rapidly expanding use of Raman microscopy arises from programmes. For micro-thermal analysis, the resistive its ease of use, even with opaque or aqueous samples, as well probe has proved to be the most useful device, and our as its ability to complement other analytical techniques such technical descriptions concentrate on this type of detector. as Fourier transform infrared (FT-IR) spectroscopy. We then give examples of SThM that use resistive probes, The benefits of using thermal excitation have been followed by brief descriptions of the various techniques exploited by several popular methods for the non-destructive of micro-thermal analysis. Much of the published work characterization of solids at the macroscale. Any local has involved more than one such technique in combination disturbance of the structure, that results in a change in density, and, for this reason, examples of the applications of micro- specific heat or thermal conductivity, may be detected by some thermal analysis are described separately, in section 4 of type of thermal probe—often with higher sensitivity than by this review. the use of optical, x-ray or electron-microscopical methods. Until recently, most materials technology has involved 2. Scanning thermal microscopy optimization of materials at the atomic scale (alloying) or at the macroscale (grain structure). In contrast, the development A scanning thermal microscope, as generally employed, of nanocomposites is an example of how modern materials incorporates some or all of the following features: technology is also concerned with the control of materials at the mesoscale. Most microanalytical techniques lack the • the probe as a near-field temperature detector; spatial resolution to operate in this regime. Consider the • a source of heat—this may be external (e.g. incident glass transition temperature (Tg) of an amorphous polymer, electromagnetic radiation), internal to the sample (a buried one of the most important parameters in polymer technology. hot region inside a chip) or, as mentioned above, may At temperatures above Tg, the behaviour of a non-crystalline consist of the probe itself; polymer material is either rubbery or viscous, depending on the • a force transducer in the form of a cantilever, whose molecular weight and by how much the temperature exceeds deflection senses the force that acts between the (thermal) Tg. Below Tg, the polymer is glassy. The extent to which Tg probe and the sample; may be affected by the confinement of the polymer matrix at • one or more feedback systems, in particular, force a surface or interface is a topic of much current interest [1]. feedback and thermal feedback—accordingly, a scanning Likewise, the properties of blends and other inhomogeneous thermal microscope generally acts also as an atomic force polymer materials may depend strongly on localized variations microscope; • in crystallinity or Tg. The possibility of exploring such effects the remaining components that are needed in the was one of the chief motives for the development of micro- construction and operation of an atomic force microscope. thermal analysis. The functions involved include actuators for spatial Micro-thermal analysis, the subject of this article, was 1 As opposed to traditional variants of microscopy in which the spatial originally the name given to the combination of localized resolution depends on wavelength, as determined by the relevant far-field thermal analysis with near-field microscopy. In its wider sense optics. R24 Topical review scanning, a system to measure cantilever deflection, display and analysis software, etc. As with a standard atomic force microscope, the height of the probe above the surface being scanned is generally controlled by a feedback system that maintains constant the force between probe and surface; the probe height is used to create topographic image contrast, quite independently of the process of temperature measurement. At the same time, the temperature signal from the same probe is used to generate a thermal image. This contains information that will depend upon a number of factors, including the nature of the heat source employed. A variety of types of thermal

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