<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OPJ</journal-id><journal-title-group><journal-title>Optics and Photonics Journal</journal-title></journal-title-group><issn pub-type="epub">2160-8881</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/opj.2016.68B009</article-id><article-id pub-id-type="publisher-id">OPJ-70301</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  1310 nm Source Spectral-Domain Optical Coherence Tomography for Chinese Pigment and Jadeite Research
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hao</surname><given-names>Sun</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Tingting</surname><given-names>Gang</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Manli</surname><given-names>Hu</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Nan</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Rongxin</surname><given-names>Tong</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xiaobo</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Qunxi</surname><given-names>Zhang</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jianhong</surname><given-names>Zhou</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Shaanxi History Museum, Xi’an, China</addr-line></aff><aff id="aff2"><addr-line>School of Physics, Northwest University, Xi’an, China</addr-line></aff><aff id="aff4"><addr-line>School of cultural heritage, Northwest University, Xi’an, China</addr-line></aff><aff id="aff1"><addr-line>School of Physics and Optoelectronic Engineering, Xidian University, Xi’an, China</addr-line></aff><pub-date pub-type="epub"><day>25</day><month>08</month><year>2016</year></pub-date><volume>06</volume><issue>08</issue><fpage>48</fpage><lpage>52</lpage><history><date date-type="received"><day>29</day>	<month>April</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>20</month>	<year>August</year>	</date><date date-type="accepted"><day>25</day>	<month>August</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   
   Optical Coherence Tomography (OCT) technique is a nondestructive optical detection technology based on low-coherence interferometer and it has become an attractive cultural heritage research method. A 1310 nm source spectral-domain optical coherence tomography (SD-OCT) system based on optical fiber Michelson interferometer and optical spectrum analyzer is proposed and demonstrated for Chinese cultural heritage research. The cross-section OCT images of Chinese pigment samples and jadeite samples can provide a lot of valuable microstructure information for the Chinese cultural heritage research and identification works. 
  
 
</p></abstract><kwd-group><kwd>Optical Coherence Tomography</kwd><kwd> Spectral-Domain OCT</kwd><kwd> Cultural Heritage</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Optical coherence tomography technology was first proposed in 1991 by D. Huang et al. [<xref ref-type="bibr" rid="scirp.70301-ref1">1</xref>], and was used in ophthalmology clinical medical research in 1995. Subsequently, OCT technology got extensive applications in fund of biopsy, oral imaging, dental caries and skin tissues imaging [<xref ref-type="bibr" rid="scirp.70301-ref2">2</xref>]-[<xref ref-type="bibr" rid="scirp.70301-ref4">4</xref>]. In the past ten years, OCT technique researching progress is rapid, its resolution, scanning speed and imaging depth have been greatly improved, and successively developed frequency-domain OCT, Doppler OCT and polarization sensitive OCT. With the growing maturity in medical diagnosis application, researchers expanded the application range of OCT Technology gradually to industrial inspection and artwork research.</p><p>From 2004, OCT technology began to be used for surface structure imaging detection of jade [<xref ref-type="bibr" rid="scirp.70301-ref5">5</xref>], ceramic [<xref ref-type="bibr" rid="scirp.70301-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.70301-ref7">7</xref>] and painting [<xref ref-type="bibr" rid="scirp.70301-ref8">8</xref>]. Especially, researchers obtained many achievements in the study of western painting compared with the traditional microscopic imaging technology. The varnish and paint layers of western painting can be distinguished easily according to their OCT images of cross sections [<xref ref-type="bibr" rid="scirp.70301-ref9">9</xref>]. The axial resolution of painting’s OCT images reached about 10 microns, and the detecting depth was up to 400 microns. OCT imaging has been used to solve the detection problem of under-drawing under the subsurface such as varnishes and glazes due to the ability that OCT can obtain microstructure information [<xref ref-type="bibr" rid="scirp.70301-ref10">10</xref>]. And Liang et al. reported the first application of in situ OCT imaging on wall paintings combined OCT technology and hyper-spectral imaging technology [<xref ref-type="bibr" rid="scirp.70301-ref11">11</xref>].</p><p>In this paper, an SD-OCT system with the central wavelength of 1310 nm is proposed for Chinese cultural heritage research. This SD-OCT system used long wavelength light source and high resolution spectrometer can reach a larger detection depth and display the microstructure information of Chinese pigment samples and jadeite samples clearly. The cross-section OCT images demonstrate that the OCT technology can be used to research the polychrome cultural relics and authenticate authenticity of jadeite products effectively.</p></sec><sec id="s2"><title>2. Experimental Setup and Principle</title><p>The schematic diagram of this SD-OCT system is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. This all-fiber OCT system consists of five major components, super luminescent diode (SLD) light source, Michelson interferometer, CCD spectrometer, objective probe with 3&#215; focusing lens and a computer with control circuits. Light emitted from the SLD enters the 2 &#215; 2 20:80 fiber coupler, where it is split into two beams and travel along the reference arm and sample arm respectively. The 2D galvo mirror is used for scanning driver module.</p><p>The center wavelength of SLD light source is 1310 nm and the full width half maximum (FWHM) is 60 nm. The resolution of the used spectrometer is 0.06 nm. The theoretical axial resolution (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70301x5.png" xlink:type="simple"/></inline-formula>) and imaging depth (z<sub>max</sub>) of the SD-OCT can be calculated according to the formulas:</p><disp-formula id="scirp.70301-formula238"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70301x6.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70301-formula239"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70301x7.png"  xlink:type="simple"/></disp-formula><p>where the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70301x8.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70301x9.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70301x10.png" xlink:type="simple"/></inline-formula>and n are the center wavelength, FWHM of light source, wavelength resolution of spectrometer and refractive index of the sample, respectively. Thus the axial resolution in air is calculated about 12.6 μm and the imaging depth is 7.15 mm. Assuming that the refractive index of jadeite materials is ~1.66, the theoretical imaging depth in jadeite objects is about 4.3 mm. But in practical application, the imaging depth is usually within one millimeter due to the differences of absorption and scattering characteristics of target materials with respect to air and biological tissues. The transparency of the target material can also affect the detection depth of OCT system.</p></sec><sec id="s3"><title>3. Results and Analysis</title><p>The SD-OCT system of <xref ref-type="fig" rid="fig1">Figure 1</xref> was constructed in the laboratory and the drive and control program was written by LabVIEW software. The application of SD-OCT in Chinese cultural heritage research was demonstrated by testing some Chinese pigment samples and jadeite beads.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The schematic diagram of SD-OCT system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70301x11.png"/></fig><p>The pigment samples were made by painting the commonly used pigments on the glass slides. After days of natural drying, the pigment layers appeared the phenomenon of cracking, detachment and swell. This is similar to the actual situations of old murals and paintings. These pigment samples can be used to simulate the real cultural relics with pigment layers. After the imaging test of nearly 20 kinds of pigment samples, it was found out that the 1310 nm source SD-OCT system could get clear images of subsurface microstructure of the pigment samples. Figures 2-4 show the representative azurite, gamboges and ochre samples and their cross-section OCT images (red line position), respectively.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref>(b) shows the cross-section OCT image of the broken location of azurite sample where the pigment layer, transparent glass layer, air layer and nethermost objective table can be distinguished clearly. But the OCT image of gamboge sample in <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) is different from <xref ref-type="fig" rid="fig2">Figure 2</xref>(b). Compared to the clear <xref ref-type="fig" rid="fig2">Figure 2</xref>(b), the left and right of <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) have a slight dislocation in vertical direction. This is the result of OCT image representing only the optical path length rather than the true physical depth. Due to the higher refractive index of gamboge sample, the higher optical path length induces the dislocation in vertical direction. The white line with red arrow mark in <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) should be the mirror image of the lower surface of glass. The right half ochre sample in <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) was painted a second layer of ochre pigment and thus the right ochre pigment was thicker than left. The thick pigment layer can be seen clearly in the OCT image in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b). From these cross-section OCT images in Figures 2-4, we can find out that the OCT technology can be used to research the polychrome cultural relics effectively.</p><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Azurite sample and its cross-section OCT image.</title></caption><fig id ="fig2_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70301x12.png"/></fig></fig-group><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Gamboge sample and its cross-section OCT image.</title></caption><fig id ="fig3_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70301x13.png"/></fig></fig-group><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Ochre sample and its cross-section OCT image.</title></caption><fig id ="fig4_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70301x14.png"/></fig></fig-group><p>Besides the pigment samples, a real jadeite bead and a fake jadeite bead were selected to be tested via OCT imaging method for comparison and analysis (as shown in <xref ref-type="fig" rid="fig5">Figure 5</xref> and <xref ref-type="fig" rid="fig6">Figure 6</xref>). In general, it is hard to distinguish which one is false just depend on observation via human eyes or magnifying glass. The fake jadeite manufactured by the modern technology method used compressed stone powder and glue injection processing is almost convincing. Jadeite is a kind of jade and is known as the “oriental gem” due to its expensive and precious characteristics. China has plenty of ancient jadeite cultural relics, and most of them were beautifully designed and great valuable. Thus the antique collection markets appear a lot of fake jadeites. The authenticity identification of jadeites is increasingly important.</p><p>It can be seen that the two cross-section OCT images of the real and fake jadeite beads (red line position) have obvious difference in <xref ref-type="fig" rid="fig5">Figure 5</xref>(b) and <xref ref-type="fig" rid="fig6">Figure 6</xref>(b). The jadeite bead of <xref ref-type="fig" rid="fig5">Figure 5</xref>(a) is carved by using natural stone material. Its cross-section OCT image in <xref ref-type="fig" rid="fig5">Figure 5</xref>(b) shows the mineral structure of natural jadeite. The dark stripes in vertical direction (A and B with red arrow mark) are caused by strong absorbing particles, which are some granular impurities embedded in the high scattering jadeite material. Comparing the <xref ref-type="fig" rid="fig5">Figure 5</xref>(b) and <xref ref-type="fig" rid="fig6">Figure 6</xref>(b), the special layered structure of the fake jadeite made of glue injection processing is obvious different with the subsurface microstructure of real jadeite. Consequently, the OCT imaging method can be used for authenticating authenticity of jadeite products.</p></sec><sec id="s4"><title>4. Conclusion</title><p>A 1310 nm source SD-OCT system and its application research in Chinese cultural heritage are proposed and demonstrated. We got the subsurface microstructure OCT images of the Chinese pigment samples and jadeite bead samples. These high resolution OCT images can display the valuable microstructure information clearly and auxiliary appraisal authenticity. Consequently, the OCT technology can be a good method for Chinese cultural heritage research.</p><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> A real jadeite bead and its cross-section OCT image.</title></caption><fig id ="fig5_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70301x15.png"/></fig></fig-group><fig-group id="fig6"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> A fake jadeite bead and its cross-section OCT image.</title></caption><fig id ="fig6_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70301x16.png"/></fig><fig id ="fig6_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70301x17.png"/></fig></fig-group></sec><sec id="s5"><title>Acknowledgements</title><p>This work was supported by the National Natural Science Foundation of China (61377087), the National Key Technology Support Program (2013BAH49F03) and the Northwest University Postgraduate Innovative Talents Training Project (YZZ15087, YJG14001 and YZZ14103).</p></sec><sec id="s6"><title>Cite this paper</title><p>Hao Sun,Tingting Gang,Manli Hu,Nan Liu,Rongxin Tong,Xiaobo Liu,Qunxi Zhang,Jianhong Zhou, (2016) 1310 nm Source Spectral-Domain Optical Coherence Tomography for Chinese Pigment and Jadeite Research. 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