ARCHAEOMETRY

Evaluation of Artifacts Produced by a Commercial Portable XRF Device and their Influence on the Analysis of Artworks

Borges, R. M. P. S.; Cavalcante, J. E.; Franzi, I. V. N. S.; Paula, A. G.; Azevedo, E.; Lopes, R. T.

DOI 10.5433/1679-0375.2025.v46.52708

Citation Semin., Ciênc. Exatas Tecnol. 2025, v. 46: e52708

Received: April 3, 2025 Received in revised for: June 25, 2025 Accepted: July 15, 2025 Available online: July 31, 2025

Abstract:

This study investigates the origin and impact of spectral interferences associated with the Bruker Tracer III portable X-ray fluorescence (pXRF) spectrometer, used by the authors for elemental characterization of cultural heritage objects. Systematic analyses were conducted on reference materials and on the sculpture Head of Apollo from the Eva Klabin House Museum, Rio de Janeiro, facilitating the detection of instrumental peaks and improving the accuracy of qualitative analyses by minimizing instrument-derived interferences. Measurements were carried out under controlled conditions, both with and without the spectrometer’s radiation protection shield, using fixed operational parameters (40 kV, 35 μA and 60 s). The resulting spectra revealed peaks attributable to the instrument’s structural components. With the shield in place, elements such as Ca, Ti, Fe, Ni, Cu, Zn, and Pb were detected. In the absence of the shield, the peaks corresponding to Ca, Zn, and Pb were suppressed, although interferences from the remaining elements persisted.

Keywords: portable X-ray fluorescence, instrumental characterization, spectral interferences, archaeometry

Introduction

X-ray fluorescence (XRF) has become a key non-destructive technique for the analysis of fragile or immovable artworks, such as paintings and sculptures, where invasive methods are not viable (Liss & Stout, 2017; Marguí et al., 2022; Osman, 2020). Its portability allows for in situ investigations in museums and archaeological sites, combining the preservation of cultural heritage with efficient data acquisition (Ferretti & Tirello, 2009; Franzi et al., 2024; Wang et al., 2022). Moreover, XRF’s capability to detect trace elements supports the study of historical production processes, restoration interventions, material degradation, and pigment provenance (Andrić et al., 2021; Franzi et al., 2024), establishing it as an essential tool in cultural heritage research (Felix & Pereira, 2021).

Despite these strengths, XRF’s analytical performance is affected by the heterogeneity of the material matrix. While homogeneous samples enable accurate quantification, layered or composite objects, such as multilayered paintings, limit the technique to qualitative or semi-quantitative interpretations due to compositional variability (Andrić et al., 2021; Felix & Pereira, 2021; Sitko & Zawisza, 2012). In the analysis of historical painted surfaces, XRF identifies elements associated with specific pigments, while trace elements can provide insights into the geographic origin of raw materials (Calza, 2013; Moioli & Seccaroni, 2000). However, spectral artifacts originating from the instrument itself can undermine the accuracy of results, especially when they coincide with elemental markers critical for provenance analysis (Gallhofer & Lottermoser, 2018; Laperche & Lemière, 2020).

This study investigates the origin and impact of spectral artifacts in the Bruker Tracer III portable spectrometer, an instrument widely employed in archaeometric research. Reference samples from the Nuclear Instrumentation Laboratory (UFRJ/Coppe/LIN) and the sculpture Head of Apollo from the Eva Klabin House Museum in Rio de Janeiro were analyzed. The sculpture, carved from marble (34.0 \(\times\) 27.0 \(\times\) 28.0 cm), is attributed to Greece and dates between the 3rd and 1st centuries BCE. It represents the head of a statue identified as Apollo, the deity associated with the sun, music, and reason. Greek marble sculptures were often polychrome and frequently integrated into architectural elements of temples. A fitting at the top of the skull suggests that this piece may have served as a support for a cornice or entablature (Casa, 2024).

The marble used in the sculpture is a metamorphic rock composed primarily of calcite (\(\mathrm{CaCO_3}\)) or dolomite (\(\mathrm{CaMg(CO_3)_2}\)). It often contains trace elements and impurities that can aid in determining the quarry of origin. However, the compositional similarity between different marble sources necessitates the application of complementary analytical techniques for reliable provenance determination (Celik & Sert, 2020; Vaggelli et al., 2014).

In this context, XRF analysis was conducted on the Head of Apollo sculpture with two primary objectives:

The analysis was qualitative and exploratory, representing an initial survey designed to inform and support future, more comprehensive studies on the composition and provenance of the piece.

Material and methods

Thirteen reference samples, consisting of pure elements and compounds, were analyzed under two experimental conditions: with and without the radiation safety cap. Four of these samples were measured in both configurations to enable direct comparison. All measurements were carried out using the portable Tracer III XRF spectrometer (Bruker), operating at 40 kV and 35 \(\mu\)A, with an acquisition time of 60 seconds per spectrum. Data was processed using ARTAX (Bruker) and OriginPro 8.5 software. Figure 1 illustrates the experimental setup, including the measurement points on the Head of Apollo sculpture.

(a) (b)
image image
(c) (d)
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Figure 1 - Experimental setups with the Tracer III spectrometer: (a) measurement without the radiation safety cap, (b) measurement with the radiation safety cap, (c) analyzed points on the sculpture, (d) front view of the Head of Apollo sculpture.

Figure 1(a) shows the setup used for measurements without the safety cap. In this configuration, pressed pellets were placed on a sample table positioned at the instrument’s nose, providing a stable surface for analysis.

The sample table, visible in Figure 1(a) as a hexagonal accessory, was used to support the samples during acquisition. The distance between the X-ray window, located at the tip of the instrument’s nose, and the pellet surface was approximately 7.0 mm.

All pellet measurements were conducted using this same configuration, thereby maintaining a consistent distance between the X-ray window and the sample throughout the experiment. It is important to note that, for safety reasons, the instrument does not operate unless an object is placed in front of the X-ray window.

Figure 1(b) depicts the configuration with the safety cap in place. The safety cap is a black, hollow cylindrical accessory with a diameter of 8.0 cm and a height of 5.0 cm, featuring one open face that fits over the sample table. In this arrangement, the instrument can operate even without a sample. The spectrum of the safety cap itself was acquired using this setup, in the absence of any sample. For pellet measurements with the safety cap, the samples were positioned on the sample table, and the safety cap was fitted over them, maintaining the setup identical to that shown in Figure 1(b). Figures 1(c) and 1(d) indicate the locations selected for XRF analysis on the Head of Apollo sculpture.

Figure 2 presents the accessories of the portable instrument used in the experiment, the sample table and the safety cap, with selected dimensions indicated.

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Figure 2 - Tracer III accessories used in the experiment: the sample table is shown on the left and the safety cap on the right.

The samples, prepared as pressed pellets at the Nuclear Instrumentation Laboratory (LIN/UFRJ), have an average diameter of 25.5 mm and an average thickness of 0.7 mm and contain the following elements/compounds:

Boric acid was used as the binder in the pellet preparation. The pellets were pressed using a Schwing Siwa hydraulic press, applying a pressure of 12 tons for 15 minutes. Table 1 details the experimental measurement conditions for each pellet, specifying whether the safety cap was used, as well as identifying the pellets analyzed under both configurations, and also shows the compound or element name of each sample, total compound mass (Comp.), elemental mass fraction, elemental mass (M Elem.), final mass of the pellet (M Final), elemental concentration by weight (W%), and surface density (\(\sigma\)) in g/cm\(^2\).

Table 1 - Pellets and their characteristics used for calibration.
Z Pellet comp/elem. Comp. (g) Mass fraction M Elem. (g) M Final (g) W (%) \(\sigma\) (g/cm2)
19 K\(_2\)SO\(_4\) 0.1004 0.4487 0.0451 0.528 8.53 0.10424
25 Mn\(_2\)O\(_3\) 0.0497 0.6960 0.0346 0.473 7.31 0.09339
27 Co 0.0510 1.0000 0.0510 0.476 10.71 0.09398
37 RbNO\(_3\) 0.0501 0.5796 0.0290 0.476 6.10 0.09394
40 ZrO\(_2\) 0.0097 0.7403 0.0072 0.471 1.53 0.09293
51 Sb 0.0502 1.0000 0.0502 0.520 9.60 0.1030
59 Pr\(_6\)O\(_{11}\) 0.0503 0.8277 0.0416 0.510 8.10 0.1010
60 Nd\(_2\)O\(_3\) 0.0507 0.8574 0.0435 0.530 8.20 0.1050
62 Sm\(_2\)O\(_3\) 0.0504 0.8624 0.0435 0.510 8.50 0.1010
64 Gd\(_2\)O\(_3\) 0.0508 0.8676 0.0441 0.510 8.70 0.1000
66 Dy\(_2\)O\(_3\) 0.0505 0.8713 0.0440 0.500 8.80 0.0982
70 Yb\(_2\)O\(_3\) 0.0492 0.8782 0.0432 0.470 9.20 0.0925
74 W 0.0501 1.0000 0.0501 0.510 9.80 0.1000

Spectral overlaps were observed in some cases between peaks originating from compounds or elements present in the pellets and artifact peaks. Notable examples include the Fe K\(\alpha1\) line overlapping with the Dy L\(\alpha1\) line, and the Ca K\(\alpha1\) line overlapping with the Sb L\(\alpha1\) line (Xrayweb, 2025). In both instances, the energy difference between these lines is smaller than the energy resolution of the spectrometer’s semiconductor detector, making it impossible to adequately separate real peaks from instrumental artifacts, which can compromise spectral interpretation (Van Grieken & Markowicz, 2001). Additional cases of spectral overlap are detailed in the results section.

To evaluate the effect of the safety cap on the measurements, each reference sample was analyzed under different configurations: with the safety cap, without it, or in both conditions. Table 2 summarizes the experimental conditions applied to each compound or element during the measurements.

Table 2 - Experimental conditions used for each pressed reference pellet, indicating whether measurements were performed with, without, or in both safety cap configurations.
Pellet compound/element Experimental condition
K\(_2\)SO\(_4\) measured with the safety cap
Mn\(_2\)O\(_3\) measured without the safety cap
Co measured in both configurations
RbNO\(_3\) measured in both configurations
ZrO\(_2\) measured with the safety cap
Sb measured in both configurations
Pr\(_6\)O\(_{11}\) measured with the safety cap
Nd\(_2\)O\(_3\) measured with the safety cap
Sm\(_2\)O\(_3\) measured in both configurations
Gd\(_2\)O\(_3\) measured with the safety cap
Dy\(_2\)O\(_3\) measured with the safety cap
Yb\(_2\)O\(_3\) measured with the safety cap
W measured without the safety cap

The marble sculpture Head of Apollo was analyzed at five strategically chosen points, three on the hair, one on the face, and one on the neck, with the goal of maximizing the potential detection of pigment residues. Details can be seen in Figures 1(c) and 1(d).

Although no visible pictorial layers were observed, the possibility of surface traces could not be ruled out, thereby justifying the exploratory nature of the investigation.

The measurements were performed using the same acquisition parameters applied to the pressed pellets: \(40\ \text{kV}\), \(35\ \mu\text{A}\), and an acquisition time of \(60\) seconds per spectrum.

Results and Discussion

Reference samples

The analysis of the reference pellets allowed for the identification and characterization of artifact peaks generated by the Tracer III portable XRF spectrometer, distinguishing between interferences inherent to the instrument (Ti, Fe, Ni, Cu) and those associated with the radiation safety cap (Ca, Zn, Pb). The systematic approach involved acquiring spectra both with and without the safety cap, as well as analyzing the cap independently to determine its elemental composition.

Figures 3(a)–(f) show characteristic X-ray spectra of selected samples acquired with the safety cap, along with the spectrum of the cap alone, highlighting the impact of instrumental interferences on data interpretation. All spectra displayed peaks from Rh (the X-ray tube anode) and Ar (ambient atmosphere).

(a)
Figure 3a
(b)
Figure 3b
(c)
Figure 3c
(d)
Figure 3d
(e)
Figure 3e
(f)
Figure 3f
Figure 3 - Characteristic X-ray spectra of selected samples measured with the safety cap compared to the spectrum of the radiation safety cap: (a) gadolinium oxide pellet, (b) potassium sulfate pellet, (c) neodymium oxide pellet, (d) rubidium nitrate pellet, (e) zirconium pellet, and (f) praseodymium oxide pellet.

Independent analysis of the safety cap revealed the presence of Ca, Ti, Fe, Ni, Cu, Zn, and Pb, which were subsequently confirmed through comparison with reference samples of known composition, Table 3.

The results obtained from the analysis of reference pellets without the protective safety cap are presented in Table 4.

Peaks corresponding to Ca, Zn, and Pb disappeared when the safety cap was removed, confirming their origin in the cap’s material. In contrast, Ti, Fe, Ni, and Cu peaks remained present under all measurement conditions, identifying them as intrinsic artifacts of the Tracer III instrument. It is important to note that, due to the limited thickness of the pellets ( 0.7 mm), the incident X-ray beam is partially attenuated, allowing it to reach the safety cap and generate interfering signals. In the case of infinitely thick samples (a few centimeters), this effect would be significantly reduced or even eliminated, as the beam would no longer reach the safety cap.

Table 3 - Analysis of reference pellets measured using the radiation safety cap using the Bruker Tracer III portable XRF spectrometer.
Compounds Detected Elements Remarks
Safety Cap Ca, Ti, Fe, Ni, Cu, Zn, Pb The elements Ca, Ti, Fe, Ni, Cu, Zn, and Pb are potential candidates for instrumental artifact peaks.
Overlap between Co K\(\beta_1\) line and Ni K\(\alpha_1\) line.
Dy\(_2\)O\(_3\) Ca, Ti, Dy, Cu, Pb Overlap between Dy L\(\alpha_1\) line and Fe K\(\alpha_1\) line; Dy L\(\beta_1\) line and Ni K\(\alpha_1\) line; and Dy L\(\gamma_2\) line and Zn K\(\alpha_1\) line.
Overlap between Gd L\(\gamma_2\) line and Cu K\(\alpha_1\) line.
K\(_2\)SO\(_4\) S, K, Ti, Fe, Ni, Cu, Zn, Pb Overlap between K K\(\beta_1\) line and Ca K\(\alpha_1\) line.
Nd\(_2\)O\(_3\) Ca, Ti, Nd, Fe, Ni, Cu, Zn, Pb Overlap between Nd L\(\ell\) line and Ti K\(\alpha_1\) line.
Pr\(_6\)O\(_{11}\) Ca, Pr, Ni, Cu, Zn, Pb Overlap between Pr L\(\ell\) line and Ti K\(\alpha_1\) line; Pr L\(\gamma_1\) line and Fe K\(\alpha_1\) line.
No overlaps. Sample is suitable for identifying all artifact peaks within a single spectrum. However, the analysis suggests Zn contamination in the sample.
Sb Ca, Ti, Fe, Ni, Cu, Zn, Pb Overlap is observed between the Sb L\(\alpha_1\) line and the Ca K\(\alpha_1\) line, as well as between the Sb L\(\gamma_1\) and L\(\gamma_2\) lines and the Ti K\(\alpha_1\) line.
Overlap between Sm L\(\beta_1\) line and Fe K\(\alpha_1\) line; Sm L\(\gamma_2\) line and Ni K\(\alpha_1\) line.
Overlap is observed between the Yb L\(\ell\) and Fe K\(\alpha_1\) lines, Yb L\(\alpha_1\) and Ni K\(\alpha_1\) lines, and Yb L\(\beta_2\) and L\(\beta_3\) lines with the Zn K\(\alpha_1\) line.
ZrO\(_2\) Ca, Ti, Fe, Ni, Cu, Zn, Pb, Zr Sample allows visualization of all instrumental and radiation safety cap artifact peaks.

Table 4 - Analysis of reference pellets measured without the protective safety cap using the Bruker Tracer III portable XRF spectrometer.
Compounds Detected Elements Remarks
Co Ti, Fe, Co The absence of Ca, Zn, and Pb peaks confirms that these elements originate exclusively from the composition of the safety cap.
The presence of Zn and traces of Ca in the sample suggests contamination of the pellet with these elements. Additionally, overlap occurs between the Mn K\(\beta_1\) peak and the Fe K\(\alpha_1\) line.
RbNO\(_3\) Ti, Fe, Ni, Cu, Zn, Rb Confirms Ca and Pb as artifacts from the safety cap.
Sb Sb, Fe, Ni, Cu, Zn Confirms Ca and Pb as artifacts from the safety cap. The presence of Zn suggests contamination of the antimony pellet with this element.
Confirms Ca and Pb as artifacts from the safety cap. The presence of Zn suggests contamination of the antimony pellet with this element.
Confirms Ca and Pb as artifacts from the safety cap. Overlaps are observed between the following lines: W L\(\ell\) with Ni K\(\alpha_1\), W L\(\alpha_1\) with Cu K\(\alpha_1\), and W L\(\alpha_2\) with Zn K\(\alpha_1\). The analysis also suggests bismuth contamination in the sample.

Figure 4 illustrate different responses of elemental peaks to the presence or absence of the safety cap, comparing the spectra obtained from the RbNO\(_3\) and Co pellets, with and without the cap. In contrast, Figure 3 summarizes the cap’s influence on peak generation. These findings emphasize the importance of applying preliminary corrections to avoid false positives in qualitative analyses.

(a)
Figure 4a
(b)
Figure 4b
Figure 4 - Characteristic X-ray spectra samples measured with and without the protective safety cap: (a) cobalt pellet and (b) rubidium nitrate pellet.

A comparison of spectra acquired from samples measured with and without the safety cap, Figures 4(a) and 4(b), demonstrating significant variations in the counts of Rh and Ar peaks. These findings suggest that the safety cap induces scattering of radiation back toward the detector, thereby increasing the counts of these characteristic peaks. Additionally, the increase observed in the Ar peak may be attributed not only to direct excitation by the X-ray source but also to secondary excitation by characteristic radiation from lead. Since the characteristic energy of Pb is closer to the excitation energy of argon, Pb fluorescence may also probabilistically excite Ar atoms in the surrounding air along the return path to the detector, resulting in increased detection of Ar characteristic X-rays.

Head of Apollo

Following the identification and validation of artifact peaks generated by the XRF spectrometer in reference samples, the methodology was applied to analyze the Head of Apollo sculpture, incorporating corrections for the effects of these pre-characterized instrumental interferences.

The elemental analysis of the sculpture detected S, Ca, Ti, Mn, Fe, Cu, Zn, Pb and Sr, see Figure 5. The prominent calcium peak aligns with the carbonate composition of marble, while Mn, Fe, and Sr correspond to trace elements typically associated with distinct quarries. To accurately infer the material’s provenance, quantitative analyses are essential, as they would clarify whether the detected concentrations originate from ancient pigments, restoration patinas, or the geological matrix (Magrini et al., 2018).

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Figure 5 - Overlaid spectra from the five measurement points on the marble sculpture Head of Apollo.

The presence of Si and K may further contribute to determining the marble composition used in the Apollo sculpture. Additional chemical components, such as FeO, Fe\(_2\)O\(_3\), Al\(_2\)O\(_3\), SiO\(_2\), K\(_2\)O, and Na\(_2\)O, may occur in low concentrations and influence the marble’s mineralogy (Celik & Sert, 2020). Elements like Ti, Zn, and Pb are also consistent with trace signatures of marbles sourced from quarries supplying the Mediterranean during antiquity (Poretti et al., 2017). In the case of the Head of Apollo measurements, conducted without the radiation protective safety cap, the detection of Zn and Pb confirms their intrinsic origin in the sculpture. However, the interpretation of Ti remains ambiguous: although cited in the literature as a potential trace element in marbles, it was identified as an intrinsic artifact peak of the equipment.

Elements such as Pb, Cu, Ni, and Zn may derive from sulfide or oxide inclusions, often present in marbles as submicroscopically distributed impurities with dimensions of a few micrometers (Poretti et al., 2017). This hypothesis explains the consistent detection of S across all spectra.

The interpretation of Ti, Cu and Ni, however, remains uncertain. While Ti is referenced as a trace element in marbles (Poretti et al., 2017), its low spectral intensity and similarity to instrumental artifacts complicates definitive attribution. Similarly, Cu and Ni, which also appears as equipment-derived interference, cannot be conclusively assigned to either natural or instrumental sources. In contrast Fe exhibited peak intensities exceeding those recorded in pellet measurements suggesting its probable presence either as residue from pictorial layers or as a naturally occurring trace element within the marble matrix.

Figure 6 presents a comparison between the X-ray spectrum acquired from measurement point 1, on the Head of Apollo, see Figure 1(c), and that of an RbNO\(_3\) pellet measured without the safety cap.

image

Figure 6 - X-ray spectrum acquired from measurement point 1 on the Head of Apollo, compared with the spectrum of an RbNO\(_3\) pellet measured without the safety cap.

The experimental conditions for the sculpture and the pellet measurements, both conducted without the safety cap, are comparable. Based on this comparison, it is qualitatively evident that, although the Fe signal includes a contribution from the instrument itself, iron is indeed present in the analyzed area of the sculpture.

Conclusions

The results confirmed the generation of artifact peaks by the portable XRF Tracer III spectrometer, with Ti, Fe, Ni, and Cu identified as intrinsic equipment interferences, while Ca, Zn, and Pb were linked to the safety cap. Distinguishing these artifacts from the samples’ true composition proved critical to avoiding misinterpretations, particularly in analyses of artworks and archaeological materials, where trace elements are pivotal for inferring provenance or identifying pigments.

In the application to the Head of Apollo sculpture, elements such as Ca, Fe, Mn, and Sr aligned with the marble’s composition, whereas Zn and Pb suggested natural impurities or historical residues. However, the presence of Ti, Ni, and Cu as artifacts introduced ambiguities, necessitating spectral corrections to prevent data distortions. Qualitative analysis could not conclusively determine whether Zn and Pb originated from the geological matrix, pigments, or conservation interventions, underscoring the need for complementary methodologies.

While this study characterized the Tracer III’s artifact peaks, unresolved gaps require further investigation. These include the determination of the instrument’s sensitivity curve and limits of detection (LOD); the verification of detector linearity; the use of certified reference samples to refine analytical accuracy; the comparison of data with spectra from different pXRF spectrometer models to assess equipment-specific biases; the validation of reproducibility across multiple units of the same equipment to confirm intrinsic variations and the implementation of quantitative analyses to measure the relative contribution of artifacts in in situ measurements.

For the Head of Apollo, integrating XRF with techniques such as X-ray diffraction (XRD) and Raman spectroscopy could resolve spectral overlaps and corroborate hypotheses regarding marble provenance or pigment residues. Finally, identifying these instrumental interferences optimizes XRF spectral interpretation in archaeometry, ensuring higher precision in assessing the chemical composition of historical objects.

Acknowledgments

This study was supported by the Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq), INCT INAIS (grant 406303/2022-3), and was partially funded by the Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES) – Finance Code 001. The authors would also like to thank the Fundação de Amparo à Pesquisa do Estado do Rio de Janeiro (FAPERJ) for their financial support.

Author Contributions

R. M. de P. S. Borges participated in: conceptualization, data curation, formal analysis, investigation, methodology, visualization, and writing – original draft. J. E. Cavalcante, I. V. N. da S. Franzi, and A. G. de Paula participated in: investigation. E. Azevedo and R. T. Lopes participated in: resources and funding. D. F. Oliveira participated in: validation, resources, supervision, and writing – review and editing.

Conflicts of Interest

The authors declare no conflict of interest.

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