<?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">IJCNS</journal-id><journal-title-group><journal-title>International Journal of Communications, Network and System Sciences</journal-title></journal-title-group><issn pub-type="epub">1913-3715</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijcns.2014.74013</article-id><article-id pub-id-type="publisher-id">IJCNS-44817</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject></subj-group></article-categories><title-group><article-title>
 
 
  Color Information Encoding Based on Phase-Truncated Gyrator Transform Domain
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>uhammad</surname><given-names>Rafiq Abuturab</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Tajuddin</surname><given-names>Ali Ahmad</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Electronics and Communication Engineering, Maulana Azad College of Engineering 
and Technology, Patna, India</addr-line></aff><aff id="aff1"><addr-line>Department of Physics, Maulana Azad College of Engineering and Technology, Patna, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>rafiq.abuturab@gmail.com(URA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>15</day><month>04</month><year>2014</year></pub-date><volume>07</volume><issue>04</issue><fpage>114</fpage><lpage>121</lpage><history><date date-type="received"><day>16</day>	<month>February</month>	<year>2014</year></date><date date-type="rev-recd"><day>16</day>	<month>March</month>	<year>2014</year>	</date><date date-type="accepted"><day>30</day>	<month>March</month>	<year>2014</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>
 
 
   A color information encryption method using phase-truncated gyrator transform domain is proposed. In this technique, the color image is decomposed into R, G and B channels. The decomposed three RBG channels evade the interference of crosstalks efficiently. Each channel is separately modulated to the first random phase mask and then gyrator transformed. The transformed image is phase-truncated to get first encoded image and amplitude-truncated to produce first asymmetric phase key. The obtained image is modulated to the second random phase mask and then again gyrator transformed. The resulted image is phase-truncated to obtain second encoded image and amplitude-truncated to generate second asymmetric phase key. The proposed system includes transformation angles of GT and asymmetric phase keys as decryption keys. The proposed system can be implemented digitally or optically. The optical setup is free from optical misalignment problem. The theoretical analysis and numerical simulation results both validate the proposed technique. 
 
</p></abstract><kwd-group><kwd>Asymmetric Cryptosystem</kwd><kwd> Gyrator Transform</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Optical cryptography techniques have emerged as one of the next generation technologies, in which optical image encryption techniques have been widely studied because of their inherent advantages of high-speed and paralleloptical signal processing. Refregier and Javidi first proposed a double random phase encoding (DRPE) based on the 4-f optical correlator to encode an input image into stationary white noise [<xref ref-type="bibr" rid="scirp.44817-ref1">1</xref>] . Since then, various subsequent DRPE based optical encryption schemes have been introduced [<xref ref-type="bibr" rid="scirp.44817-ref2">2</xref>] -[<xref ref-type="bibr" rid="scirp.44817-ref6">6</xref>] . In all these image encryption techniques, as a monochromatic light is used to illuminate a real color image, color information is lost during decryption process. Since color images provide more information than gray scale images and also the additional color information contribute to a higher level of security. Zhang and Karim proposed a color encryption method based on an indexed image and DRPE [<xref ref-type="bibr" rid="scirp.44817-ref7">7</xref>] . The color image encryption techniques have been further extended [<xref ref-type="bibr" rid="scirp.44817-ref8">8</xref>] -[<xref ref-type="bibr" rid="scirp.44817-ref11">11</xref>] . However, the above proposed optical encryption techniques belong to the category of symmetric cryptosystems, in which the encryption keys are identical to the decryption keys. Qin and Peng proposed an asymmetric cryptosystem based on a phase-truncated Fourier transform (PTFT) to remove the linearity of the DRPE [<xref ref-type="bibr" rid="scirp.44817-ref12">12</xref>] . Recently, the PTFT-based encryption method has been found to be vulnerable to a specific attack based on iterative Fourier transforms, when the two random phase masks (RPMs) are used as public keys to encrypt different plaintexts [<xref ref-type="bibr" rid="scirp.44817-ref13">13</xref>] . The PTFT-based cryptosystem has been researched to resist against specific attack [<xref ref-type="bibr" rid="scirp.44817-ref14">14</xref>] -[<xref ref-type="bibr" rid="scirp.44817-ref16">16</xref>] .</p><p>In this paper, for the first time, to our knowledge, a new asymmetric color image cryptosystem based on gyrator transform (GT) domain is proposed. In this method, the color image is divided into R, G and B channels. Each of these channels is independently attached to the first RPM placed at the image plane and then gyrator transformed. The transformed image is phase-truncated to get first encoded image and amplitude-truncated to produce first decryption phase key. The transformed image is attached to the second RPM placed at the gyrator transform plane and then again gyrator transformed. The resulted image is phase-truncated to get second encoded image and amplitude-truncated to generate second decryption phase key. The proposed system provides transformation angles of GT as additional keys and decryption phase keys as asymmetric keys. Consequently, a high robustness against existing attacks can be achieved. Numerical simulations show the validity and viability of the proposed technique.</p></sec><sec id="s2"><title>2. Gyrator Transform</title><p>The gyrator transform (GT) is defined as a linear canonical transform which produces the twisted rotation in position-spatial frequency planes of phase space. Thus, the GT operation of a two-dimensional function <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\78bfccc2-ceeb-4e78-81b0-f8d31faa09da.png" xlink:type="simple"/></inline-formula> with parameter<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\190bc967-be37-4f67-b24e-c15c79cbf967.png" xlink:type="simple"/></inline-formula>, known as transformation angle, is defined as [<xref ref-type="bibr" rid="scirp.44817-ref17">17</xref>]</p><disp-formula id="scirp.44817-formula67318"><label>(1)</label><graphic position="anchor" xlink:href="htmlimages\2-9701855x\777e4b88-df8f-4e2a-af04-5fe2ef0cdac9.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\98c6864b-1a51-4186-a279-eaa82b0b2df6.png" xlink:type="simple"/></inline-formula> denotes gyrator transform operator, <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\4de5ded2-8473-4d15-bd8b-3f5cb7ce2707.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\d34fa6ab-924c-498a-8075-c0a09523f4a7.png" xlink:type="simple"/></inline-formula> are the input and output coordinates, respectively. The GT can be realized by an optimized flexible optical system having plano-convex cylindrical lenses. The angle parameter <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\c3f50891-d092-4a0b-b283-2aaa34d42050.png" xlink:type="simple"/></inline-formula> is changed by the proper rotation of these lenses [<xref ref-type="bibr" rid="scirp.44817-ref18">18</xref>] . Recently, the gyrator transformbased security systems for gray image [<xref ref-type="bibr" rid="scirp.44817-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.44817-ref20">20</xref>] and color image [<xref ref-type="bibr" rid="scirp.44817-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.44817-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.44817-ref16">16</xref>] have been extensively studied.</p></sec><sec id="s3"><title>3. Proposed Method</title><p>In this method, an original color image is segregated into R, G and B color components. For simplicity, only red component is considered for the proposed cryptosystem. Let <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\53eb09a0-3b5f-4877-807d-c4f037e80052.png" xlink:type="simple"/></inline-formula> be original color image.<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\7d4cfc24-076a-4915-b51a-d04b6ac1c0e7.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\c7bc7b79-7f70-4490-adfe-9c7242fd4b82.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\08ce52ec-5c23-4a9c-b2e2-ed9ea1f86b41.png" xlink:type="simple"/></inline-formula> be its red, green and blue components, respectively. For simplicity, only red channel is illustrated. The subscript r has been used for red component. Let <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\ef7064db-283a-44f8-a1f8-3f01596c1054.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\f676f8c3-a8a0-4f28-82af-17e8e747eb9c.png" xlink:type="simple"/></inline-formula> be independent random phase masks at input and transform planes, respectively. The RPM <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\10405198-c8a3-467d-8b3a-257a6ace7758.png" xlink:type="simple"/></inline-formula> multiplied by <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\54e23ce4-c312-4f34-91f4-19be2f466b0b.png" xlink:type="simple"/></inline-formula> is gyrator transformed at rotation angles <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\5cb4e137-095b-4af8-b348-4cab054ebffb.png" xlink:type="simple"/></inline-formula> and then phase truncated to obtain encoded image<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\9fef8978-dbc2-4caf-89a0-c229fb578d2c.png" xlink:type="simple"/></inline-formula>. The resulted image <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\f335ad92-b403-457d-8e19-9821c12ea7d0.png" xlink:type="simple"/></inline-formula> multiplied by <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\a8aa42ea-4f63-468f-9bc6-8f380959f774.png" xlink:type="simple"/></inline-formula> is gyrator transformed at rotation <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\28668ca1-10a5-4bb2-997f-11273831f4f4.png" xlink:type="simple"/></inline-formula> and then phase truncated to get final encoded image <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\030bab7b-308c-46ec-b040-a08df8e46b8d.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.44817-ref12">12</xref>] .</p><disp-formula id="scirp.44817-formula67319"><label>(2)</label><graphic position="anchor" xlink:href="htmlimages\2-9701855x\c9c6b4b6-03ea-44bc-88cf-f48260fcd442.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.44817-formula67320"><label>(3)</label><graphic position="anchor" xlink:href="htmlimages\2-9701855x\d6ee0aa4-ff1e-4b08-9f16-4b55a957a14f.png"  xlink:type="simple"/></disp-formula><p>The operator <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\c2d78c79-c1d3-4f90-b3f0-f1a10478f24c.png" xlink:type="simple"/></inline-formula> denotes phase truncation. Similarly, the amplitudes truncations of both <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\ecb2d48c-b8c8-40c7-a1a9-2fc12457c4ab.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\feb03991-b850-4c98-99e8-d67af891950a.png" xlink:type="simple"/></inline-formula> generate first and second asymmetric phase keys.</p><disp-formula id="scirp.44817-formula67321"><label>(4)</label><graphic position="anchor" xlink:href="htmlimages\2-9701855x\c954a450-4e85-4b46-9843-4ba3e5985ed4.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.44817-formula67322"><label>(5)</label><graphic position="anchor" xlink:href="htmlimages\2-9701855x\67bcd103-067e-401c-aa95-ccd90fb3953f.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\a43bbdb3-782c-4ffd-9696-4a70ffcbf632.png" xlink:type="simple"/></inline-formula> indicates the operator of amplitude truncation.</p><p>The decryption process is straightforward and much simpler compared with encryption process.</p><disp-formula id="scirp.44817-formula67323"><label>(6)</label><graphic position="anchor" xlink:href="htmlimages\2-9701855x\617856b7-9385-4af3-9429-f379b371d66d.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.44817-formula67324"><label>(7)</label><graphic position="anchor" xlink:href="htmlimages\2-9701855x\783ef29b-9b21-445c-8b56-f98a806b09c5.png"  xlink:type="simple"/></disp-formula><p>The blue and green channels are encrypted and decrypted by the same procedure.</p><p>The encryption process is performed digitally whereas the decryption process can be implemented using optoelectronic device. The GT can be implemented by using three generalized lenses (indicated as<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\5d57e3a7-1144-4d77-8bdf-baf09f5bf764.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\9f8e59e5-0005-41e6-aa18-9a277d781fbb.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\d63bdd7f-3c08-442a-8fb1-9f0cb38bae57.png" xlink:type="simple"/></inline-formula>) with fixed equal distances <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\ad8637aa-5b52-40bc-ad67-7cdcbc66ed52.png" xlink:type="simple"/></inline-formula> between them. Each generalized lens corresponds to the combination of two identical plano-convex cylindrical lenses of the same power. The first and third identical generalized lenses of focal length <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\88aa01aa-0b3c-4f2b-8752-a5159ef2fe7f.png" xlink:type="simple"/></inline-formula> are rotated with respect to each other. The second generalized lens of a focal length <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\076d39c2-2e8d-4aab-9d82-5e256e30f4aa.png" xlink:type="simple"/></inline-formula> is fixed. These lenses are properly rotated to vary the transformation angle <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\f9c28f6f-863d-4564-8e14-9afca1441ba8.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.44817-ref18">18</xref>] .</p><p>The optical setup is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> &amp; <xref ref-type="fig" rid="fig2">Figure 2</xref>. For convenience, only the red channel is considered. The encrypted red-channel <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\0ce0e7fc-59b5-4fdf-8935-1e1892ba96cf.png" xlink:type="simple"/></inline-formula> is multiplied with decryption phase key<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\0dbf5f20-753a-431b-9c66-41eca0c73d95.png" xlink:type="simple"/></inline-formula>, displayed on first Spatial Light Modulator (SLM), illuminated by a collimated beam and then optically transformed by first GT. The intensity of image recorded by a CCD 1 camera. Now the transformed image is multiplied with decryption phase key<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\120215ed-91a1-40d8-ba99-92c354c64035.png" xlink:type="simple"/></inline-formula>, displayed on the second SLM, illuminated by the collimated beam and then optically transformed by second GT. The intensity of image is recorded by the CCD 2 camera. The same process is repeated with encrypted greenand blue-channels to obtain corresponding green and blue channels. Finally, the decrypted color channels are combined into decrypted color image by using a computer system.</p></sec><sec id="s4"><title>4. Numerical Simulation Results</title><p>Numerical simulations have been carried out on a Matlab 7.11.0 (R2010b) platform to test the feasibility and security of the new proposal. The original color image having size <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\4bf3840a-6337-423e-af45-4cfdba3b2015.png" xlink:type="simple"/></inline-formula> pixels is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(a). The first and second transformation angles of the GT for red, green and blue channels are, respectively, <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\b536eac6-1e31-4e05-a009-2ea01e030599.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\5387d2a6-7f74-4bea-a98e-3784662ec912.png" xlink:type="simple"/></inline-formula>. The encrypted image produced by three-multiplexed channels is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(b). The real parts of three-multiplexed channels of first and second asymmetric phase keys are, respectively, illustrated in <xref ref-type="fig" rid="fig2">Figure 2</xref>(c) and  <xref ref-type="fig" rid="fig2">Figure 2</xref>(d). The retrieved images with arbitrary phase key and with no phase keys are demonstrated in <xref ref-type="fig" rid="fig2">Figure 2</xref>(e) and <xref ref-type="fig" rid="fig1">Figure 1</xref>(f), respectively. The recovered images with the transformation angle for each channel changed by <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\4b1cbaec-b7ae-4f1e-8a08-0c5861c54e57.png" xlink:type="simple"/></inline-formula> and with all correct keys are demonstrated in <xref ref-type="fig" rid="fig2">Figure 2</xref>(g) and <xref ref-type="fig" rid="fig2">Figure 2</xref>(h), respectively. As can be seen from Figures 2(e)-(g), corresponding decrypted images provide no valuable information about the original color image. That means the original image can only be obtained if all the decryption keys are accurate as shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(h).</p><p>To evaluate the reliability of the proposed algorithm quantitatively, the mean square error (MSE) is introduced and defined as</p><disp-formula id="scirp.44817-formula67325"><label>(8)</label><graphic position="anchor" xlink:href="htmlimages\2-9701855x\cb4f0640-e9b7-4a73-a691-0ea16e6361ce.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\82f6185d-b2b6-4d63-8f7b-5b3a5fa80991.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\c6cf8677-9d40-47d2-8282-3077125ba95a.png" xlink:type="simple"/></inline-formula> indicate the original and decrypted image at pixel position<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\9fb5429c-9568-42bd-b387-95218625a71a.png" xlink:type="simple"/></inline-formula>, respectively. <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\208a8be9-3585-4bc6-b1f6-cacf2bed1b9b.png" xlink:type="simple"/></inline-formula>represents the size of the image.</p><p>In <xref ref-type="fig" rid="fig2">Figure 2</xref>(b), the MSE values of encrypted result with all the correct keys are <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\dec2c8f9-b6d1-4a7c-8e8e-3442cde34842.png" xlink:type="simple"/></inline-formula> for red, green and blue channels, respectively. These values are very high, which indicate that no information about the original image can be obtained. The calculated MSE values corresponding to <xref ref-type="fig" rid="fig2">Figure 2</xref>(e) and <xref ref-type="fig" rid="fig2">Figure 2</xref>(f) for red, green and blue channels are <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\f172aa3e-8389-4e23-afc3-81aaac801b44.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\f46ff383-d558-424b-9ad4-7fb9f508ca06.png" xlink:type="simple"/></inline-formula>, respectively. The high MSE values, for arbitrary phase key and no phase keys, sufficiently reveal the strength of the proposed algorithm. The MSE values for a very small error of <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\ac37a1dd-ab27-4668-884d-534469e0558e.png" xlink:type="simple"/></inline-formula> in transformation angle of GT for red, green and blue is<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\068847fe-7830-4017-a549-d48641895954.png" xlink:type="simple"/></inline-formula>. The high MSE results adequately demonstrate the robustness of the proposed system.</p><p>In attack analysis, first the known plaintext attack is considered, in which an attacker knows all the transformation angles and attempts to produce decryption keys from a fake color image of size <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\fdf11282-fd77-408b-a501-1b601bfcf503.png" xlink:type="simple"/></inline-formula> pixels as shown <xref ref-type="fig" rid="fig3">Figure 3</xref>(a); the real parts of the first fake decryption key and second fake decryption key are displayed in <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) and <xref ref-type="fig" rid="fig3">Figure 3</xref>(c). The decrypted image with all fake keys with correct transformation angles is illustrated in Figures 3(d). That means an unauthorized user can not retrieve the original image. So, the proposed technique can resist against brute force attack.</p><p>Second, the robustness of the proposed technique against occlusion attacks on the encrypted data has been examined. The 50%- and 70%- occluded encrypted images are shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) and  <xref ref-type="fig" rid="fig4">Figure 4</xref>(c), respectively. The calculated MSE values corresponding to recovered images with all correct keys as displayed in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(d) for red, green and blue channels, are <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\8fe68c4d-a43c-494f-91bb-b036a14ad2da.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\091b4c72-5ff2-407d-9a5a-0aa2fd1919d8.png" xlink:type="simple"/></inline-formula>, respectively.</p><p>Third, the robustness of the proposed method against noise attacks on the encrypted data has also been checked. The Gaussian and speckle noised encrypted images with variance 0.1 are displayed in <xref ref-type="fig" rid="fig5">Figure 5</xref>(a) and <xref ref-type="fig" rid="fig5">Figure 5</xref>(c), respectively. The resulted MSE values corresponding to retrieved images with all right keys as depicted in <xref ref-type="fig" rid="fig5">Figure 5</xref>(b) and <xref ref-type="fig" rid="fig5">Figure 5</xref>(d) for red, green and blue channels, are  <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\79869bfd-eb9e-46f1-8964-b8e2f3df405b.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\ecce0c58-a70a-4e41-93b9-aec502c90fa0.png" xlink:type="simple"/></inline-formula>, respectively.</p><p>From above results, it can be concluded that if the encrypted data is destroyed by occlusion or degraded by noise in storage and transmission process, the decrypted image with all right keys is recognizable. Therefore, the proposed method has certain robustness against occlusion and noise attacks.</p><p>The sensitive degree of the transformation angle is analyzed and then calculated. The sampling interval is fixed at the range<inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\726ec4b7-8ea5-47aa-8f55-b50431d97316.png" xlink:type="simple"/></inline-formula>, sampling length is taken at 0.01 and other decryption keys are used with correct values. The corresponding MSE curves between original red, green and blue channels and their corresponding decrypted images are depicted in Figures 6(a)-(c). These MSE curves have very narrow downward peaks. The MSE of red channel is quite sensitive as compared to green and blue channels. The value of MSE function becomes zero at <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\d20c5cd3-c6c8-4935-8de0-8bdd49a8b8a0.png" xlink:type="simple"/></inline-formula> with correct decryption keys. The zero-MSE value indicates that the original image is decrypted completely.</p><p></p></sec><sec id="s5"><title>5. Conclusion</title><p>A new information encryption system based phase-truncated gyrator transform domain is presented. The original color image is separated into <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\acc1e665-5aa8-47be-a7a7-ebcc45415357.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\9843fe5e-b243-4601-a5bd-943e780920a0.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="tmlimages\2-9701855x\df3048e9-609e-428d-91c1-6b430686f8f6.png" xlink:type="simple"/></inline-formula> channels. The separated three RBG channels avoid the interference of crosstalks efficiently. The two random phase masks are encryption keys which are used as public keys. The two asymmetric phase keys are decryption keys which are employed as private keys. That means only authorized users can decrypt the original information. The transformation angles of GT as supplementary keys significantly enhance the security of the proposed system. The numerical simulations have shown the effectiveness of this method.</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.44817-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Refregier, P. and Javidi, B. (1995) Optical Image Encryption Based on Input Plane and Fourier Plane Random Encoding. Optics Letters, 20, 767-769. http://dx.doi.org/10.1364/OL.20.000767</mixed-citation></ref><ref id="scirp.44817-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Unnikrishnan, G., Joseph, J. and Singh, K. (2000) Optical Encryption by Double-Random Phase Encoding in the Fractional Fourier Domain. 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