Chapter 4.5

Analytical Methods Based on Laser Ablation Sampling

 

Matija Strlič1, Vid Simon Šelih2, Jana Kolar3

1 University College London, Centre for Sustainable Heritage, The Bartlett School of Graduate Studies, London, U.K.

2 University of Ljubljana, Faculty of Chemistry and Chemical Technology, Ljubljana, Slovenia

3 National and University Library, Ljubljana, Slovenia

 

Method

Non- / Micro-destructive

Information obtained

Chemical composition / trace analysis

Type of object

Any

Sample size/amount needed

Size: depending on the sampling chamber if used
Amount: ng 

Sampling type

Surface

Portable/transportable version available

No

 

Contents

4.5.1    Introduction
4.5.2    Basic Principles
    4.5.2.1    Sample Preparation and the Sampling Chamber
    4.5.2.2    Laser
    4.5.2.3    The Plasma
    4.5.2.4    Quadrupole Mass Spectrometer
4.5.3    Case Studies
    4.5.3.1    Case Study 1: Iron Gall Ink on Paper
    4.5.3.2    Case Study 2: Paint Layers
4.5.4    Conclusions
4.5.5    Acknowledgements
4.5.6    Supporting Information
    4.5.6.1    References
    4.5.6.2    Providers
    4.5.6.3    Useful Websites

4.5.7    Contact Information

   

4.5.1          Introduction

Some analytical methods utilize laser ablation (LA) as a “light chisel” in order to take a tiny amount of sample from the artefact surface for chemical analysis.

Most often, the sample is transported into an analyser consisting of inductively-coupled plasma and a mass spectrometer (ICP-MS). In this way, the elemental composition of the sampled spot is obtained. The information is useful for identification of pigments, metals, alloys, ceramics, glasses, and for trace analysis of organic materials, e.g. varnishes, paper, textiles etc. Occasionally, other types of analyzers are used, although ICP-MS is by far the most common one and will be described in more detail in this Chapter.

Scanning mode allows the information to be obtained along a line or any other path scanned by the laser. Since a minute amount of the artefact is removed, the method can be classified as micro-destructive. Whether the trace left by the laser is visible or not depends on the substrate material and laser parameters: materials such as stones, glass, and ceramics are less sensitive than organic materials.

LA-ICP-MS combines the micrometer-scale resolution of a laser probe with the speed, sensitivity and multi-elemental capability of ICP-MS, and rivals other micro-beam techniques such as the proton microprobe and secondary ion mass spectrometry (i.e. the "ion probe"). Compared to other micro-sampling analytical techniques, LA-ICP-MS has several advantages:

-          laser probing utilizes light rather than charged particles and can, therefore, analyze both conducting and non-conducting materials without the need for e.g., a conductive coating;

-          no vacuum is required in the sample chamber;

-          the analysis step is divided from the sampling step - therefore, both steps can be independently controlled and optimized;

However, quantification of data is difficult and requires well-defined standard samples. Also, the technique is not portable. The detection limit for most analytes (from Li on, excluding noble gasses, C, N, O, F, and Cl) is in the range of 0.01 - 0.1 µg/g.

For the more scientific reader, a review of LA-ICP-MS was recently published.1

4.5.2          Basic Principles

4.5.2.1       Sample Preparation and the Sampling Chamber

In order to collect and transport the ablated material, the sample is put in a chamber flushed with a carrier gas. There is no sample preparation needed. The sample surface is not necessarily flat. Fragments of frescoes, plasters, paint layers, already prepared in resin mounts for microscopic investigation can readily be used. The usual sample dimension is cca. 1-2 cm, the sampled area is limited by the laser beam diameter, which can be focussed down to a few micrometers, if necessary. Special samplers can be constructed allowing in-situ sampling of whole artworks.2

The principal components of the sampling part include a high-power laser, beam steering and focusing optics, an ablation chamber and interface connections that ensure an efficient transport of aerosol. A general block diagram of the LA setup is shown in Figure 4.5.1.

The sample size must be adapted to the sample chamber, which is equipped with a quartz glass lid transparent to laser light (Figure 4.5.2). A stream of carrier gas enters the sample cell and picks up fine sample particles produced by the ablation process and transports them into the analyser (ICP-MS). The carrier gas can be Ar or He.

The sample cell is mounted on a stage that allows the sample to be moved relative to the laser beam in all three directions. The laser is focused and the ablation process can be observed on a monitor showing the images captured by a video camera.


4.5.2.2       Laser

The lasers initially used for the purpose were ruby lasers. Other lasers also in use were carbon dioxide and nitrogen lasers and recently also excimer lasers. The most common type of laser is the Q-switched (pulsed) Nd-YAG laser. The fundamental wavelength of this laser is 1064 nm, however, since UV laser light interacts more efficiently with most solids, the Nd-YAG lasers in LA-ICP-MS instruments commonly use the fourth harmonic (266 nm) or even fifth harmonic (213 nm). The interaction between UV laser light and most solids tends to involve photochemical phenomena (bond scission) and physical ablation, whereas IR laser light often causes unwanted sample heating and melting.

The basic requirement for the laser is to deliver energies of sufficiently high power densities (typically 1-20 J/cm2, 10-20 Hz, ~5 ns) at the lens focus to ablate and vaporise diverse sample matrices. The laser ablation instrument requires an accurate optical system of lenses, prisms and mirrors that conducts and focuses the laser beam onto the sample. The optical system may also include a system of apertures of different diameters that can be used to vary the beam diameter and/or shape.

The laser beam can be thought of as a "light chisel" which interacts with the solid sample to generate very fine solid particles leaving behind a minute ablation crater (in the order of tens of µm in diameter).

4.5.2.3       The Plasma

Inductively coupled plasma - mass spectrometry requires the sample to be introduced into a high temperature argon plasma (approx. 8000 °C), which dissociates molecules and ionizes atoms. The positive ions are passed into vacuum via an interface, where electrostatic lenses focus and accelerate the ion beam into a mass spectrometer. Here, the ions are sorted by mass and detected using an ion detector, usually an electron multiplier.

The plasma torch consists of an assembly of three concentric quartz tubes, providing flow path for plasma, sample and outer Ar gas. At the end of the torch, Ar plasma is formed and sustained with constant delivery of high power, high frequency RF energy via the load coil (1 to 2 kW, 27 MHz). The energy is transferred by interaction of ionized argon with the electromagnetic field of the induction coil. Both positive argon ions and electrons are accelerated by the high-frequency field of the coil. Due to constant movement and friction, particles are heated to very high temperatures.

4.5.2.4       Quadrupole Mass Spectrometer

A quadrupole mass spectrometer consists of four hyperbolically shaped parallel metal rods, onto which a potential is applied (Figure 4.5.3). The applied voltages affect the ions travelling down the flight path centred between the four rods. For given applied voltages, only ions of a certain mass-to-charge ratio pass through such a quadrupole filter while all other ions are thrown out, not reaching the detector. A mass spectrum is obtained by monitoring the ions passing through the quadrupole filter as the voltages on the rods are varied. Other types of mass spectrometers are also in use, with the same aim, to separate and detect ions on the basis of their mass-to-charge ratio.

 

4.5.3          Case Studies

There are a number of interesting examples of the use of laser ablation methods described in the literature. The aim of the following paragraphs is not to provide a literature review but rather to highlight some interesting applications on different materials.

An interesting approach without the use of ICP-MS was applied by Colombini et al.3 The group used sampled micro-amounts of mainly organic materials from thin layers of painting using a pulsed Er:YAG laser system operating at 2.94 μm assisted by water/ethanol mixtures. The ablated materials condensed on glass coverslips and were characterised by Fourier transformed infrared spectrometry (FT-IR) and gas chromatography mass spectrometry (GC-MS). In this way, a 17th century canvas copy of Caravaggio’s “Christ crowned with thorns” and a 13th century panel “Virgin with Child” by Anonymous were examined and the presence of overpainting consisting of egg and Venice turpentine in one case, and of “beverone” over a varnish (linseed oil and Venice turpentine) in the other one was highlighted.

A very similar approach was used by Feely et al,4 who studied health risks associated with the use of Nd:YAG lasers for the removal of black sulphation crusts. The ablated material was collected on glass plates and analysed using scanning electron microscopy (SEM) with energy dispersive X-ray spectroscopy (EDS).  The presence of Al, Si, Fe in addition to Ca, S, and O was indicated.

Research on marble crusts by Ulens et al.5 using LA-ICP-MS showed that this technique can be used in authentication studies. The depth profiles of Mg, Al, Mn, Fe, Zn, Sr, Ba, La and Pb in weathered marble crusts were obtained.

Hogan et al.6 used laser ablation mass spectrometry (without the ICP part) to characterize the surface composition of a daguerreotype. Using their instrument, consisting of an Nd:YAG laser and a home-built mass spectrometer, they were able to determine the elemental composition of the surface. By ablating and analyzing the ablated material, they were able to follow the process of laser cleaning. On a tarnished nineteenth century daguerreotype, they found Na+, Ca2+, Hg2+, Agn+, and AgnS+ ions. The analyses of the daguerreotype after laser cleaning showed that silver sulphide was greatly reduced or eliminated.

LA-ICP-MS was applied also for the characterization of historical glass samples.7 Iridescent Art Nouveau lead crystal glass samples were analyzed and it was proven that the material of single layers originated from different glass sources. The analysis of glass fragments from the archaeological site in Ephesos, Turkey, showed only a low concentration of Pb.

A very interesting application was developed to recognize art forgeries.2 The authors applied LA-ICP-MS to the analysis of artist paints from different manufacturers to identify variation in the elemental composition. In this way, a comparison of the paints to assist provenancing was facilitated. Preliminary trials of a prototype sample collection device designed to reduce damage and allow for in-situ sampling of artworks were also undertaken. The device allowed direct laser-based sampling of a complete painting.

Devos et al. investigated early-medieval archaeological iron finds.8 The analysis of elemental impurities in the iron provided useful archaeometallurgical information on the production process and the provenance of the iron. Preliminary results from the analysis of archaeological iron samples from several excavations in Switzerland were given.

Roman mints were analysed by Ponting et al.9 using Pb isotope analysis. They showed that Pb isotope compositions gave isotope fingerprints despite the likely reworking of the metal during coin production.

The analysis of gold coins issued from the 7th to the 12th century AD in the Arab Empire by Gondonneau and Guerra10 using LA-ICP-MS showed that several different supplying sources were used, according to the region and to the period.

The identification of different gold ores by means of characteristic trace elements indicated recycling of the ancient coinage and, after AD 750, the minting in the entire Arab Empire of different new gold ores: Egyptian type, North Eastern type and West African type.

Islamic glazed ceramic ware were analysed by Hill et al.11 In a survey of 175 artefacts from Sasanian and Early Islamic period sites located on the Deh Luran Plain in south-western Iran were examined to identify the constituents of the ceramic glazes. The results of the analyses revealed that alkaline-based glazed ceramics have paste compositions that are distinct from contemporary and later ceramics decorated with alkaline-low-lead and lead-based glazes.

Non-conservation oriented applications of the LA-ICP-MS technique include other materials of conservation interest, e.g. wood12, corals13 etc.

Two case studies are presented here carried out at the University of Ljubljana, using the instrumental set-up consisting of the New Wave Research UP-213 Deep UV YAG laser ablation workstation with the standard sample cell, He carrier gas, coupled with Agilent 7500ce ICP-MS instrument, 1500 W Ar plasma.

4.5.3.1       Case Study 1: Iron Gall Ink on Paper

The LA-ICP-MS technique could be useful for determination of metals in the paper material, however, it can also provide valuable information on the composition of various inks deposited on its surface. The infamous iron gall inks, for instance, usually contain an appreciable amount of transition metals, such as iron, copper, manganese etc.,14 and reports on the use of LA-ICP-MS are already available in the literature.15

Here, we present an LA-ICP-MS scan of an iron-gall ink fragment (Figure 4.5.5a). The laser light wavelength used was 213 nm, pulse length 4 ns, beam diameter 25 μm.

 

Without proper calibration, the results can be given on a relative scale, meaning that we know only the distribution of a particular element (Figure 4.5.5b), and not its actual content. Nevertheless, the distributions are of enormous interest if we want to evaluate, e.g. migration processes during a particular conservation treatment.

4.5.3.2       Case Study 2: Paint Layers

Paint layers or façade fragments can readily be studied even after inclusion into a resin for routine microscopic investigations (Figure 4.5.6b). Here, we present an LA-ICP-MS scan of a paint fragment taken from an 18th-century statue of St. Zacharias from the Kamnik Museum in Slovenia (Figure 4.5.6a). The laser light wavelength used was 213 nm, energy density 14.8 J/cm2, pulse length 4 ns.

  

The results (Figure 4.5.6c) clearly indicate the calcium-rich ground layer, onto which lead-rich pigment layer was painted, probably lead white (2PbCO3·Pb(OH)2). This is a face fragment, the pink colouration was obtained using a mercury-rich pigment, e.g. vermillion (HgS) possibly mixed with the red minium (Pb3O4). The top layer contains some barium-containing pigment – this could well be a consequence of a later conservation intervention.

4.5.4          Conclusions

Laser ablation (LA) sampling is a simple and often micro-destructive technique for sampling of artefacts. Following the sampling, analysis can proceed using a variety of analytical techniques, e.g. IR spectroscopy, gas chromatography or X-ray spectroscopy. By far the most often used analytical techniques associated with laser ablation sampling is inductively coupled plasma with mass spectrometry (ICP-MS).

Using the latter technique, which is not available as a portable instrument, multielemental analysis can be performed, however, the sample has to be introduced into a sample compartment, thus limiting its size. There are new developments in this area, promising in-situ sampling of whole artefacts.

Studies of artefacts include metals, glass, ceramics, paintings, daguerrotypes, paper, stone, providing information on authenticity, provenance, or composition of pigment, patina and crust. In comparison to other techniques, LA-ICP-MS offers trace analysis of samples (elements from Li on, excluding noble gasses, C, N, O, F, and Cl) at atmospheric pressure with the spatial resolution of a few μm, at a moderate cost.

4.5.5          Acknowledgements

The authors acknowledge the financial support of the Ministry of Higher education, science and technology of the Republic of Slovenia (Programme no. P1-0153) and of the COST G7 action. The authors thank Mr. I. Nemec from the Restoration Centre, Ljubljana, Slovenia for supplying the pigment fragment.

4.5.6          Supporting Information

4.5.6.1          References

1      J. S. Becker: “Applications of inductively coupled plasma mass spectrometry and laser ablation inductively coupled plasma mass spectrometry in materials science”, Spectrochim. Acta B 57 (2002) 1805–1820.

2      K. Smith, K. Horton, R. J. Watling, N. Scoullar: “Detecting art forgeries using LA-ICP-MS incorporating the in situ application of laser-based collection technology”, Talanta 67 (2005) 402-413.

3      M. P. Colombini, A. Andreotti, G. Lanterna, M. Rizzi: “A novel approach for high selective micro-sampling of organic painting materials by Er:YAG laser ablation”, J. Cult. Herit. 4 (2003) 355s–361s.

4      J. Feely, S. Williams, P. S. Fowles: “An initial study into the particulates emitted during the laser ablation of sulphation crusts”, J. Cult. Herit. 1(2000) S65–S70.

5      K. Ulens, L. Moens, R. Dams, S. Vanwinckel, L. Vandevelde: “Study of element distribution in weathered marble crusts using laser-ablation inductively-coupled plasma-mass spectrometry”, J. Anal. Atom. Spectr. 9 (1994) 1243-1248.

6      D. L. Hogan, V. V. Golovlev, M. J. Gresalfi, J. A. Chaney, C. S. Feigerle, J. C. Miller, G. Romer, P. Messier: “Laser ablation mass spectroscopy of nineteenth century daguerreotypes”, Appl. Spectrosc. 53 (1999) 1161–1168; V. V. Golovlev, M. J. Gresalfi, J. C. Miller, G. Romer, P. Messier: “Laser characterization and cleaning of nineteenth century Daguerreotypes”, J. Cult. Herit. 1 (2000) S139–S144.

7      G. Schultheis, T. Prohaska, G. Stingeder, K. Dietrich, D. Jembrih-Simburger, M. Schreiner: “Characterisation of ancient and art nouveau glass samples by Pb isotopic analysis using laser ablation coupled to a magnetic sector field inductively coupled plasma mass spectrometer (LA-ICP-SF-MS)”, J. Anal. Atom. Spectrom. 19 (2004) 838-843.

8      W. Devos, M. Senn-Luder, C. Moor, C. Salter: “Laser ablation inductively coupled plasma mass spectrometry (LA-ICP-MS) for spatially resolved trace analysis of early-medieval archaeological iron finds”, Fresen. J. Anal. Chem. 366 (2000) 873-880.

9      M. Ponting, J. A. Evans, V. Pashley: “Fingerprinting of Roman mints using laser-ablation MC-ICP-MS lead isotope analysis”, Archaeometry 45 (2003) 591-597.

10   A. Gondonneau, M. F. Guerra: “The circulation of precious metals in the Arab Empire: the case of the near and the Middle East”, Archaeometry, 44 (2002) 573-599.

11   D. V. Hill, R. J. Speakman, M. Glascock: “Chemical and mineralogical characterization of Sasanian and Early Islamic glazed ceramics from the Deh Luran Plain, southwestern Iran”, Archaeometry 46 (2004) 585-605.

12   T. Prohaska, C. Stadlbauer, R. Wimmer, G. Stingeder, C. Latkoczy, E. Hoffmann, H. Stephanowitz: “Investigation of element variability in tree rings of young Norway spruce by laser-ablation-ICPMS”, Sci. Tot. Environ. 219 (1998) 29-39.

13   D. J. Sinclair, L. P. J. Kinsley, M. T. McCulloch: “High resolution analysis of trace elements in corals by laser ablation ICP-MS”, Geochem. Cosmochem. Acta, 62 (1998) 1889-1901.

14   J. Kolar, M. Strlic (Eds.): “Iron Gall Inks: On the Manufacture, Characterisation, Degradation and Stabilisation”, National and University Library, Ljubljana, 2006.

15   B. Wagner, S. Garbos, E. Bulska, A. Hulanicki: “Determination of iron and copper in old manuscripts by slurry sampling graphite furnace atomic absorption spectrometry and laser ablation inductively coupled plasma mass spectrometry”, Spectrochim. Acta B 54 (1999) 797-804.

4.5.6.2          Providers

Laser ablation solid sampling

http://www.new-wave.com/1nwrProducts/LaserAblation.htm

http://www.cetac.com/prods/laser/laser_overview.html

http://www.tuilaser.com/markets/science/ablation.htm

ICP-MS

http://www.chem.agilent.com/Scripts/PCol.asp?lPage=513

http://www.thermo.com/com/cda/product/detail/1,1055,15265,00.html

http://las.perkinelmer.com/Catalog/default.htm?CategoryID=ICP+Mass+Spectrometry+%5bICP-MS%5d

4.5.6.3          Useful Websites

More on LA-ICP-MS

http://www.agu.org/revgeophys/neal00/node11.html

30-min guide to ICP-MS

http://las.perkinelmer.com/Content/RelatedMaterials/D-6355A-30Min.pdf

4.5.7          Contact Information

Matija Strlič
University College London
Centre for Sustainable Heritage
The Bartlett School of Graduate Studies
Gower Street (Torrington Place Site)
London WC1E 6BT
United Kingdom
E: m.strlic@ucl.ac.uk
W: http://www.ucl.ac.uk/sustainableheritage/

Vid Simon Šelih
Faculty of Chemistry and
Chemical Technology
University
of Ljubljana
Askerceva 5
SI-1000
Ljubljana
Slovenia
E: 
vid-simon.selih@fkkt.uni-lj.si
W: http://www.fkkt.uni-lj.si/

Jana Kolar
National and University Library
Turjaška 1
SI-1000 Ljubljana
Slovenia
E: jana.kolar@nuk.uni-lj.si
W: http://www.nuk.uni-lj.si