Removing foxing stains from old paper at 157 nm 3 E. Sarantopouloua,*, Z. Samardzijb, S. Kobeb, Z. Kolliaa, A.C. Cefalasa 4 5 a 6 7 8 Theoretical and Physical Chemistry Institute, National Hellenic Research Foundation, 48 Vassileos Constantinou Avenue, Athens 11635, Greece b Jozef Stefan Institute, Jamova 39, 1001 Ljubljana, Slovenia TE Abstract Using a molecular fluorine laser at 157 nm foxing stains were removed successfully from a 16th century old paper. Laser cleaning of stains and foxing from old paper manuscripts is far more effective at 157 nm in comparison to different wavelengths without leaving any yellowish after-effect on the paper. This is because at 157 nm illumination of old paper, complete bond breaking of all the organic molecules of the paper is taking place. Mass spectroscopy at 157 nm and for moderate laser intensities up to 1 mJ/cm2 of old paper suffering from foxing indicate organic matter disintegration to small photofragments atomic, diatomic or triatomic, which are flying apart with supersonic speed. In addition high spatial resolution energy dispersive X-ray system (EDXS) analysis over the effected areas indicate the presence of iron, suggesting that biological activity is taking place preferentially in paper areas containing iron. # 2002 Published by Elsevier Science B.V. EC 9 10 11 12 13 14 15 16 17 18 19 20 21 Keywords: Energy dispersive X-ray system; Foxing stains; Mass spectroscopy 24 1. Introduction 25 The rusty red irregular shaped areas in old manuscripts dated from the 16th to the 19th century are known as foxing. They may vary in size from just visible spots to large areas covering most of the page. Foxing is a serious problem because the stains might migrate through successive pages and causing thus irreversible damage of old paper and manuscripts. It was long thought to have been the result of rust, from tiny fragments of iron metal, which were worn off papermaking machinery. However it is now known that initial cause of foxing was a group of conidia, which had been 30 31 32 33 34 35 CO 28 29 * UN 27 RR 22 23 26 Corresponding author. Tel.: þ30-10-7273840; fax: þ30-10-7273842. E-mail address: [email protected] (E. Sarantopoulou). 1 2 DP RO OF Applied Surface Science 9611 (2002) 1–6 deposited on the surface of the paper and germinated in situ [1]. Possible cause of foxing is the contamination by the auto-oxidization of lipids from conidia. The color in the foxed areas is due to an alkaline-soluble rusty red material and an insoluble straw-colored stain in the paper fibers. Therefore foxing could be spread all over the paper volume, devaluating manuscript appearance and destroying unique evidences of human history. Preventing action therefore should be taken for foxing, and besides treatment by conventional dry and yet methods laser techniques have been applied before at various wavelengths on paper parchment and paintings [2–5]. Immediate and long-term effects on paper treatment using lasers were assessed by Kolar et al. [6], by determining the degree of polymerization of cellulose. They found a strong and immediate cellulose degradation after laser treatment at 308 nm while laser irradia- 0169-4332/02/$ – see front matter # 2002 Published by Elsevier Science B.V. doi:10.1016/S0169-4332(02)01379-X 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 2. Experimental 96 The experimental apparatus consists mainly of the F2 laser source and the vacuum chamber, where the 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 97 CO 57 UN 55 56 quadrupole mass spectrometer and the Ptolemaic map were placed. The map was placed 1 mm apart from the quadrupole mass spectrometer (Baltzers QMG 311) at right angle to its axis (Fig. 1). The all stainless steel 316 vacuum chamber was evacuated to 106 mbar using a turbomolecular pump. The laser head at 157 nm delivers 10 1 mJ per pulse, and the pulse duration was 12 ns at FWHM. The laser beam was focused on the old paper map, using a quartz lens of 40 cm focal length. Following photodissociation of the parent molecule, the molecular photofragments were ionized using an electron gun inside an isopotential chamber (Welnet). The molecular ions were focused with an Eizen lens, and eventually they were directed alongside the quadrupole mass filter. The upper detection limit of this filter was 300 amu. The ions after entering in the mass filter, were deflected at right angle, and they were detected using a high gain 108, secondary electron multiplier (SEM). The signal was then amplified and it was registered using a boxcar integrator and a computer. Regarding the photoablation experiments, the etch depth at 157 nm on the manuscript’s paper, corresponding to a particular fluence, was measured at room temperature in nitrogen buffer gas, by counting the number of pulses required to penetrate the paper. The energy of the laser pulse falling on the sample was attenuated using lithium fluoride plates, and by placing them between the sample and the laser. The laser operating frequency was kept below 1 Hz to avoid cumulative heating effects on the sample. The laser TE 95 54 RR 94 tion at 1064 nm resulted in an increase of the degree of polymerization due to the formation of inter and intramolecular ether bonds. In this communication we have used the molecular fluorine laser at 157 nm to remove foxing marks from a medieval Ptolemaic map (21 cm 30 cm) from the book of S. Münster, ‘‘Nova Graecia secundum omnes eius regions et provincias citra ultra et Hellespontum’’, published by H. Petri in 1585 A.D. Foxing was successfully removed after few laser shots. By applying laser ablation techniques the absorption coefficients and the threshold energy fluences of the paper of the manuscript were determined at 248 nm besides 157 nm. The absorption coefficient at 157 nm was found to be one order of magnitude higher than at 248 nm, suggesting complete photochemical dissociation of the paper fibers without any evidence of heating of the illuminated area (yellowish color), and in agreement with previous results for various organic polymers [7–10]. In order to investigate the basic photochemical mechanism of the photodissociation dynamics of the paper fibers under vacuum ultraviolet (VUV) irradiation, we apply mass spectroscopic techniques. Mass spectroscopy reveals that even at moderate laser energy there was a complete breaking of the molecular bonds. There were no photofragments observed for m/e larger than 30 amu (atomic mass units of m/e). Photofragments with two carbon atoms have a relatively higher probability to be dissociated from the parent cellulose molecule, than heavier photofragments with four carbon atoms. These experimental findings suggest that the bound potential energy surfaces of the excited electronic states of the parent molecule correlate with the dissociative potential energy surfaces of the excited states of the molecular photofragments over a wide energy range above 5 eV. Cellulose is disintegrated to small photofragments atomic, diatomic or triatomic, which are flying apart with supersonic speed. In addition high spatial resolution energy dispersive X-ray system (EDXS) analysis over the effected areas indicate the presence of iron, suggesting that biological activity is taking place preferentially in paper areas containing iron. 53 DP RO OF E. Sarantopoulou et al. / Applied Surface Science 9611 (2002) 1–6 EC 2 Fig. 1. Experimental set-up for recording the mass spectrum from small pieces of the old paper, remains of conventional preservation. LB, laser beam; L, lens; VC, vacuum chamber; TM, turbo molecular pump; W, window; S, sample; P, photofragments; QMS, quadrupole mass spectrometer. 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 DP RO OF E. Sarantopoulou et al. / Applied Surface Science 9611 (2002) 1–6 Fig. 2. When an organic molecule is illuminated with laser light at 157 nm (blue arrow) molecular disintegration is taking place. Illumination at longer wavelentgths (red arrow) is usually accompanied by photon emission and heating. 131 132 133 3. Results and discussion 135 3.1. Photo ablation processes 136 In the case of light excitation, mainly two kind of processes are induced on molecules: the first being CO UN 137 RR 134 TE 130 pulse was monitored with a Tektronix 7104 fast oscilloscope and a pyroelectric detector, which was placed behind the sample. In addition high spatial resolution EDXS analysis over the effected areas was used to analyze foxing areas. excitation followed by relaxation to the ground state, and the second being excitation followed by molecular disintegration (Fig. 2). Regarding the first process, the electronic excitations of the molecular specimens could relax by internal conversion to thevibrational excitationsof themolecule. Alternatively, UV excitation light could dissociate the molecule. In this case, the laser energy is expended in breaking the chemical bonds, and forming molecules with smaller number of atoms. The excess energy is converted to translational energy of the photofragments. The energy transfer in this case is considerably faster than vibrational relaxation mentioned previously. Investigation of dissociation dynamics at 157 nm could be assisted from the absorption spectra providing thus information on the excited electronic states of the molecules. However in this case direct absorption using a VUVabsorption spectrometer is impossible and hence an alternative method has to be used. The ablative and etch rate method fits well its results to the Beer’s law and in the case of polymeric materials, the absorption coefficient measurements are in excellent agreement with direct absorption measurements using a VUV absorption spectrometer [8]. The etch depth per pulse, as a function of the incident laser fluence in the case of the old paper is shown in Fig. 3 for 157 nm. The dispersion of the experimental data at high fluence is due to the fluctuations of the energy of the EC 129 3 Fig. 3. Etch rate at 157 nm as a function of fluence. 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 DP RO OF 4 E. Sarantopoulou et al. / Applied Surface Science 9611 (2002) 1–6 Table 1 Absorption coefficient a and threshold fluence FT at different wavelengths a (per cm) 104 FT (mJ/cm2) 170 157 nm 1.2 0.4 40 8 4 0.5 12 3 16 3 0.3 0.1 laser beam. As it is generally accepted, the etch depth per pulse, d, is given by the Beer’s law F 1 d ¼ a ln FT 183 3.2. Mass spectroscopy 184 Mass spectra of paper pieces left out after conventional preservation, were recorded at 157 nm and with 175 176 177 178 179 180 181 185 CO 174 UN 173 RR 182 where a is the absorption coefficient (per cm) of the material at a given wavelength, F the fluence of the laser pulse and FT is the threshold fluence which describes the minimum fluence of light where the photodissociation process starts to be competitive to the thermal relaxation processes, such as intersystem crossing or collision quenching. These processes merely degrade the energy without engendering any photodissociation. The values of the threshold fluence FT, and the absorption coefficient a at different wavelengths are tabulated in Table 1, following least square fitting of the Beer’s law to the experimental results. 171 172 TE 167 168 193 nm EC 166 248 nm laser energy around 10 mJ and laser intensity 15 MW/ cm2 in order to produce significant etching of the paper sample due to the fact that only few pieces of paper were available. The background pressure of 2 107 mbar sets the detection limit for the minimum energy of the laser pulse for detecting photofragments at 0.1 mJ. First, the mass spectrum with the old paper sample inside the chamber, was recorded with the F2 laser off. The mass spectrum in this case indicates that there is not any significant paper degassing at the background pressure of 106 mbar. The peaks at 14, 18, 28 and 32 amu, correspond to the presence of N, H2O, N2 and O2, respectively. The mass spectrum of the old paper sample under moderate laser intensity up to 15 MW/ cm2, is indicated in Fig. 4. No fragments were observed for m/e higher than 32, contrary to previous recorded mass spectra at 193 and 248 nm, suggesting that photodissociation of organic molecules at 157 nm is one photon process [8]. Hence, taking into consideration that the molecular weight of the cellulose monomer is 178; we come to the conclusion that there is a complete bond breaking of the polymeric paper fiber chain under irradiation at 157 nm. The photofragments are the products of either direct dissociation of the parent molecule, or recombination of the various excited fragments. It is worthwhile to mention that under these experimental conditions, no fragments with m/e higher than 32 were observed. Fig. 4. Mass spectrum of old paper at 157 nm. 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 201 202 203 204 205 206 207 208 209 210 211 212 213 214 215 DP RO OF TE E. Sarantopoulou et al. / Applied Surface Science 9611 (2002) 1–6 UN CO RR EC Fig. 5. Mass spectrum of foxing areas at 157 nm. Fig. 6. EDXS analysis over the effected areas, indicate the presence of iron. 5 228 4. Conclusions 229 Foxing marks have been efficiently removed from a medieval Ptolemaic map edited in 1580 A.D. using a molecular fluorine laser at 157 nm. The mass spectrum of foxing areas indicates the presence of excess amount of H, OH and H2O, a fact which suggests that the foxing areas consists of organic moieties of a simpler chemical structure than cellulose. High spatial resolution EDXS analysis over the effected areas, indicate the presence of iron, suggesting that biological activity is taking place preferentially in paper areas containing iron. 217 218 219 220 221 222 223 224 225 230 231 232 233 234 235 236 237 238 239 [1] M.L.E. Florian 41 (1996) 65. [2] W. Kautek, S. Pentzien, P. Rudolf, J. Krüger, C.M. Pitelos, H. Bansa, H. Grösswang, E. König, Near-ultraviolet pulsed laser interaction with contaminants and pigments on parchment: spectroscopic diagnostics for laser cleaning safety, in: C. Fotakis, T. Papazoglou, C. Kalpouzos (Eds.), Optics within Life Sciences, vol. 5, Springer, Berlin, 2000, p. 100 and references therein. [3] T.R. Friberg, V. Zafiropoulos, Y. Petrakis, C. Fotakis, in: W. Kautek, E. König (Eds.), Lasers in the Conservation of Artworks I, Restauratorenbläter, Mayer & Co., Wien, 1979, p. 79. [4] W. Kautek, S. Pentzien, P. Rudolph, J. Krüger, E. König, Appl. Surf. Sci. 127–129 (1998) 746. [5] T. Stratoudaki, D. Xenakis, V. Zafiropoulos, D. Anglos, Laser induced breakdown spectroscopy in the analysis of pigments in painted artworks. A database of pigments and spectra, in: C. Fotakis, T. Papazoglou, C. Kalpouzos (Eds.), Optics within Life Sciences, vol. 5, Springer, Berlin, 2000, p. 163. [6] J. Kolar, M. Strlic, S. Pentzien, W. Kautek, Appl. Phys. A 71 (2000) 87. [7] A.C. Cefalas, E. Sarantopoulou, E. Gogolides, P. Argitis, Microelectric Eng. 53 (2000) 123. [8] A.C. Cefalas, N. Vassilopoulos, Z. Kollia, E. Sarantopoulou, C. Skordoulis, Appl. Phys. A 70 (2000) 21. [9] A.C. Cefalas, E. Sarantopoulou, P. Argitis, E. Sarantopoulou, Appl. Phys. A 69 (2000) 929. [10] A.C. Cefalas, E. Sarantopoulou, Microelectric Eng. 53 (2000) 465. UN CO RR 271 References TE 226 227 The mass spectrum of the foxing areas of the old paper sample following illumination with laser light of moderate intensity, up to 15 MW/cm2, is indicated in Fig. 5. The mass spectrum indicates the presence of an excess amount of H, OH and H2O, and the radical group around 28 amu. From the mass spectrum it is evident that the foxing areas consists of organic moieties of simpler chemical structure than cellulose. In addition high spatial resolution EDXS analysis over the effected areas (Fig. 6) indicate the presence of iron, suggesting that biological activity is taking place preferentially in paper areas containing iron. 216 DP RO OF E. Sarantopoulou et al. / Applied Surface Science 9611 (2002) 1–6 EC 6 241 242 243 244 245 246 247 248 249 250 251 252 253 254 255 256 257 258 259 260 261 262 263 264 265 266 267 268 269 270
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