Practical XRD with Confidence

2: Quantitative XRD in Practice: From Phase Estimates to Defensible Results

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This is a written summary of a live webinar presented on May 20, 2026. The recording and resources are available on the recording page.

Presented by:

Akhilesh Tripathi

Akhilesh Tripathi

Applications Manager • XRD

Rigaku

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Webinar summary

In this webinar, the second in the series Practical XRD with Confidence, Akhilesh discusses quantitative X-ray diffraction, which is used to determine both the identity and relative abundance of crystalline phases in a material. A diffraction pattern contains several kinds of information at once: peak positions identify phases and reflect lattice parameters, peak intensities relate to atomic arrangement and phase amount, peak widths can reveal crystallite size or strain, and broad humps indicate amorphous content. A material may be fully crystalline, fully amorphous, or a mixture of ordered and disordered components, and the choice of analysis method depends heavily on that structural complexity.

Accurate quantification begins with careful sample preparation. The powder should be representative, homogeneous, evenly packed, and level with the sample holder. Particle size should generally be small enough to provide good averaging but not so fine that grinding introduces strain or excessive peak broadening. A practical range for many quantitative measurements is roughly 10 to 40 µm, with somewhat tighter control preferred for Rietveld refinement. The X-ray beam should remain fully on the sample, because spillover onto the holder increases background and can obscure weak peaks. Sample displacement, underfilling, overfilling, loose packing, or an uneven surface can shift peak positions and distort intensities, leading to incorrect identification or quantification.

The sample holder must also be chosen carefully. Aluminum holders are suitable for many inorganic powders, but weakly absorbing or low-density materials may allow the X-ray beam to penetrate through the sample and scatter from the holder. In those cases, deeper wells, glass holders, or zero-background holders may be more appropriate. The wrong holder can contribute unwanted peaks or background, especially when analyzing low-concentration phases or amorphous content.

Several methods are available for quantitative phase analysis. The relative intensity ratio method is a relatively simple semi-quantitative approach that uses database values comparing a phase’s strongest peak to a reference material such as corundum. It works best for simple mixtures with only a few phases, little peak overlap, and minimal preferred orientation. Its main weakness is dependence on selected peaks; if those peaks overlap or are affected by orientation, the results can be unreliable.

Calibration methods can provide high accuracy when suitable standards are available. External standard curves compare unknowns to prepared reference mixtures of known composition. Internal standard methods add a known amount of a reference material directly to the sample, which is especially useful for estimating amorphous content. Standard addition methods involve spiking the sample with known amounts of the phase of interest, then extrapolating back to the original concentration. These approaches are powerful but depend on matrix matching, instrument stability, good peak selection, and predictable intensity response. Matrix effects, microabsorption, preferred orientation, amorphous material, and peak overlap can all introduce error.

Rietveld refinement is the most powerful general-purpose method for complex mixtures. Rather than relying on one or two peaks, it models the entire diffraction pattern using known crystal structures. The calculated pattern is refined against the observed pattern by adjusting parameters such as scale factors, lattice constants, background, peak shapes, preferred orientation, and sometimes occupancies or thermal parameters. Because it uses the full pattern, Rietveld refinement is especially useful when phases overlap or when many phases are present.

Good Rietveld results require good data. A sufficiently broad 2θ range should be collected, especially for inorganic materials, minerals, clays, and cements. Organic and pharmaceutical materials often require a smaller angular range because their useful scattering typically decreases at higher angles. The step size should be fine enough to define peak shape, usually with several data points across each peak. Data should not be smoothed before refinement, because smoothing alters the counting statistics used for weighting. Background should normally be modeled during refinement rather than subtracted beforehand, because background can contain real contributions from amorphous material, holders, capillaries, Compton scattering, and detector effects.

Rietveld refinement depends on correct phase identification and appropriate structural models. If a phase lacks a known crystal structure, conventional Rietveld refinement cannot be performed for that phase, but profile-fitting methods such as Pawley or Le Bail fitting may still be used. This is useful for disordered materials such as some clays, where a full structural model may not exist. The quality of a refinement should be judged by both the visual fit and numerical indicators such as Rwp and goodness of fit. Difference plots are especially useful because unexplained residual peaks may indicate missing phases, poor background modeling, preferred orientation, or incorrect peak-shape parameters.

Preferred orientation is a major source of error in quantitative XRD. Plate-like, needle-like, and layered crystals often align during sample preparation, making some peaks artificially strong and others too weak. RIR and calibration methods have limited ability to address this problem beyond avoiding affected peaks. Rietveld refinement can include preferred-orientation corrections, but it is still better to reduce orientation through careful preparation. Peak overlap is another common problem; when peaks from multiple phases occur at similar angles, single-peak methods become unreliable, while full-pattern methods are better able to separate contributions using the rest of the pattern.

Microstructure also affects quantification. Small crystallite size, strain, defects, and stress can broaden peaks and complicate analysis. Instrument broadening should be characterized with standards such as silicon or lanthanum hexaboride so that sample-related broadening can be interpreted more accurately. Overgrinding should be avoided because it may introduce strain or change the material itself.

The direct derivation method provides another option when conventional structure-based approaches are difficult. It uses the relationship between diffraction intensity, structure factors, electron density, and chemical composition. When a reasonable chemical formula is known, it can estimate phase quantities using reference profiles or extracted phase patterns. This method can be useful for materials lacking complete structural data, samples with texture or large crystallites, and mixtures containing amorphous or trace phases.

Amorphous content can be estimated in several ways. A simple crystallinity analysis compares the area of crystalline peaks with the total scattering area, including the amorphous hump. More advanced approaches can incorporate amorphous components into whole-pattern fitting or use internal standards to calculate how much non-crystalline material is present. Results should be interpreted realistically, since amorphous quantification is sensitive to background modeling, sample preparation, reference selection, and assumptions about composition.

The best quantitative method depends on the sample and the available information. RIR is appropriate for simple, clean mixtures. Calibration curves are best when high-quality standards and stable measurement conditions are available. Rietveld refinement is preferred for complex multiphase materials, overlapping peaks, and preferred-orientation correction. Direct derivation can be valuable when structural information is incomplete or amorphous material must be quantified. For routine or high-throughput work, clustering tools, templates, and macros can streamline analysis by grouping similar patterns and applying consistent refinement strategies across related samples.

Reliable quantitative XRD is not achieved by software alone. It requires representative sampling, careful specimen preparation, appropriate data collection, and a method matched to the material. Errors from poor preparation, peak overlap, preferred orientation, background treatment, matrix effects, and amorphous content can easily dominate the final numbers. When these factors are controlled, XRD becomes a powerful tool for measuring phase composition in materials ranging from minerals and cements to pharmaceuticals, clays, batteries, and complex industrial powders.

 

Frequently asked questions

An XRD pattern provides several types of information at the same time. The position of the diffraction peaks is used for phase identification and is related to lattice parameters. The intensity of the peaks is related to the arrangement of atoms in the crystal structure and, in quantitative work, to the amount of each phase present. Peak width, often measured as full width at half maximum, can provide information about crystallite size and strain. A broad hump in the pattern usually indicates amorphous content, while sharp peaks indicate crystalline material. A sample may contain only crystalline phases, only amorphous material, or a mixture of both.

Quantitative XRD depends on the assumption that the measured sample is representative of the material as a whole. If the sample is poorly prepared, the diffraction pattern may contain errors that lead to incorrect phase identification or inaccurate phase percentages. The powder should be spread evenly, packed firmly, and filled so that the surface is level with the edge of the holder. Underfilled or overfilled samples can cause peak-position errors, and uneven surfaces can distort intensities and peak shapes.

Particle size also matters. If particles are too large, the sample may not behave as a random powder and may show preferred orientation. If particles are too small, grinding can introduce strain broadening. A particle size range of roughly 10 to 40 µm is a practical target, with careful control being especially important for Rietveld refinement. The sample should also be homogeneously mixed, because a poorly mixed sample will not give reliable quantitative results.

The X-ray beam should remain fully on the sample. If the beam spills beyond the sample area, scattering from the holder, air, or nearby surfaces can increase the background and reduce the signal-to-noise ratio. Weak peaks may become difficult or impossible to detect, which can lead to missed minor phases or poor quantitative accuracy.

The sample holder must also be appropriate for the material. Aluminum holders are generally suitable for many inorganic samples, such as minerals, clays, and cement-related materials. However, for low-absorbing materials, especially materials rich in light elements such as carbon-based organic compounds, X-rays can penetrate through the sample and scatter from the holder. In those cases, a deeper sample well, glass holder, or zero-background holder may be more suitable, depending on the sample amount and the type of analysis being performed.

The relative intensity ratio method is a relatively simple semi-quantitative approach that uses database values to estimate phase amounts from peak intensities. It is best suited for simple mixtures containing only a few phases, especially when peaks are well separated and preferred orientation is not a major issue. For example, a two-phase mixture with clearly distinguishable peaks can often be estimated effectively using RIR values.

Its main limitation is that it relies heavily on selected peaks. If the strongest peak of one phase overlaps with a peak from another phase, the result can be inaccurate. Another peak can sometimes be selected, but the method does not offer the same level of correction or modeling available in full-pattern methods. As mixtures become more complex, or as peak overlap increases, RIR becomes less reliable.

Rietveld refinement uses the entire diffraction pattern rather than relying on one or two individual peaks. A calculated pattern is generated from known crystal structures, and the model is refined until it matches the measured pattern as closely as possible. This allows the method to handle complex mixtures, overlapping peaks, background contributions, peak-shape effects, lattice-parameter changes, and preferred orientation more effectively than simpler approaches.

The method is especially useful when several phases are present. Even if some peaks overlap, other parts of the pattern may still contain enough information to distinguish the phases and refine their relative amounts. Rietveld refinement can also include corrections for preferred orientation and peak broadening, although the best results still require good sample preparation and high-quality data.

Good Rietveld refinement requires properly collected raw data. A sufficiently broad 2θ range should be measured, particularly for inorganic materials, minerals, clays, and cements. A range extending to about 90° or 100° 2θ can be useful because low-angle data help determine lattice parameters, while higher-angle data help refine structural and thermal parameters. For organic and pharmaceutical materials, the useful scattering often drops off at higher angles, so the upper range may not need to be as high.

The step size should be small enough to define the peak shape properly. A good practical guideline is to collect enough points across each peak, often at least five to seven points across the full width at half maximum. Step sizes around 0.01° or 0.02° are commonly appropriate for sharp crystalline materials. Data should not be smoothed before refinement because smoothing changes the counting statistics and affects the weighting used by the refinement algorithm. Background should also generally be modeled during refinement rather than removed beforehand, because background may contain real contributions from amorphous material, sample holders, capillaries, Compton scattering, or detector effects.

Amorphous content appears as a broad hump rather than sharp diffraction peaks. One simple approach is to compare the integrated area of crystalline peaks with the total scattering area, including the amorphous hump, to estimate percent crystallinity. This can provide a practical measure of how much of the material is crystalline versus amorphous.

More advanced approaches use an internal standard or whole-pattern methods. In an internal standard method, a known amount of a crystalline reference material is added to the sample. The reduction in the apparent crystalline phase amounts can then be used to estimate how much amorphous material is present. Whole-pattern methods can also model amorphous contributions if an appropriate profile or approximate structural representation is available. Amorphous quantification must be treated carefully because it depends strongly on background modeling, standard selection, sample preparation, and assumptions about composition.

The best method depends on the sample complexity, the available reference information, and the required accuracy. RIR is useful for simple mixtures with only a few phases and minimal overlap. Calibration-curve methods can be very accurate when suitable standards are available and the unknown samples closely match the standards in matrix, crystallinity, and particle behavior. Internal standards are especially useful for amorphous quantification, while standard addition can help measure a low-level phase when the pure phase is available for spiking.

Rietveld refinement is usually the preferred method for complex multiphase samples, especially when peaks overlap or when preferred orientation must be corrected. Direct derivation can be useful when complete crystal-structure information is unavailable but chemical formulas or reasonable composition estimates are known. In all cases, the method should be matched to the real limitations of the sample. Preferred orientation, microabsorption, peak overlap, amorphous content, instrument drift, and poor sample preparation can all dominate the error if they are not controlled.

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