Experimental research on JTC encryption system based on spiral phase mask and its characteristics

As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to b...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Chen, Qi [verfasserIn] Shen, Xueju [verfasserIn] Lin, Chao [verfasserIn] Wang, Haoyi [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2018

Schlagwörter:	Optical information security JTC encryption system Spiral phase mask Effect of encryption and decryption

Übergeordnetes Werk:	Enthalten in: Optics communications - Amsterdam, 1969, 427, Seite 123-131
Übergeordnetes Werk:	volume:427 ; pages:123-131

DOI / URN:	10.1016/j.optcom.2018.06.037

Katalog-ID:	ELV000222550

Internformat


LEADER	01000caa a22002652 4500
001	ELV000222550
003	DE-627
005	20230524141740.0
007	cr uuu---uuuuu
008	230427s2018 xx \|\|\|\|\|o 00\| \|\|eng c
024	7		\|a 10.1016/j.optcom.2018.06.037 \|2 doi
035			\|a (DE-627)ELV000222550
035			\|a (ELSEVIER)S0030-4018(18)30528-5
040			\|a DE-627 \|b ger \|c DE-627 \|e rda
041			\|a eng
082	0	4	\|a 530 \|q DE-600
084			\|a 33.18 \|2 bkl
084			\|a 33.38 \|2 bkl
084			\|a 50.37 \|2 bkl
100	1		\|a Chen, Qi \|e verfasserin \|4 aut
245	1	0	\|a Experimental research on JTC encryption system based on spiral phase mask and its characteristics
264		1	\|c 2018
336			\|a nicht spezifiziert \|b zzz \|2 rdacontent
337			\|a Computermedien \|b c \|2 rdamedia
338			\|a Online-Ressource \|b cr \|2 rdacarrier
520			\|a As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to be improved. In order to improve its performance, the spiral phase mask (SPM) in singular optics is used as the key mask of the JTC encryption system. Under the JTC encryption system, the influence of SPM’s structure parameters on encryption–decryption effect was analyzed by means of theoretical analysis and numerical simulation. The influence of SPM and RPM on encryption–decryption effect and anti-attack ability were compared, and the initial experiment was conducted. The results indicated that the decryption effect is slightly improved when using SPM, the sensitivity of key is stronger, the key parameters are more, and the ability to resist the COA and CPA algorithm attack can be improved. The initial experiment results also verified the validity and correctness of our proposed method.
650		4	\|a Optical information security
650		4	\|a JTC encryption system
650		4	\|a Spiral phase mask
650		4	\|a Effect of encryption and decryption
700	1		\|a Shen, Xueju \|e verfasserin \|4 aut
700	1		\|a Lin, Chao \|e verfasserin \|4 aut
700	1		\|a Wang, Haoyi \|e verfasserin \|4 aut
773	0	8	\|i Enthalten in \|t Optics communications \|d Amsterdam, 1969 \|g 427, Seite 123-131 \|h Online-Ressource \|w (DE-627)266889247 \|w (DE-600)1468811-6 \|w (DE-576)07596239X \|x 1873-0310 \|7 nnns
773	1	8	\|g volume:427 \|g pages:123-131
912			\|a GBV_USEFLAG_U
912			\|a SYSFLAG_U
912			\|a GBV_ELV
912			\|a GBV_ILN_20
912			\|a GBV_ILN_22
912			\|a GBV_ILN_23
912			\|a GBV_ILN_24
912			\|a GBV_ILN_31
912			\|a GBV_ILN_32
912			\|a GBV_ILN_40
912			\|a GBV_ILN_60
912			\|a GBV_ILN_62
912			\|a GBV_ILN_63
912			\|a GBV_ILN_65
912			\|a GBV_ILN_69
912			\|a GBV_ILN_70
912			\|a GBV_ILN_73
912			\|a GBV_ILN_74
912			\|a GBV_ILN_90
912			\|a GBV_ILN_95
912			\|a GBV_ILN_100
912			\|a GBV_ILN_101
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_224
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_702
912			\|a GBV_ILN_2003
912			\|a GBV_ILN_2004
912			\|a GBV_ILN_2005
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2025
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2038
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2056
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2111
912			\|a GBV_ILN_2112
912			\|a GBV_ILN_2113
912			\|a GBV_ILN_2118
912			\|a GBV_ILN_2122
912			\|a GBV_ILN_2129
912			\|a GBV_ILN_2143
912			\|a GBV_ILN_2147
912			\|a GBV_ILN_2148
912			\|a GBV_ILN_2152
912			\|a GBV_ILN_2153
912			\|a GBV_ILN_2190
912			\|a GBV_ILN_2336
912			\|a GBV_ILN_2507
912			\|a GBV_ILN_2522
912			\|a GBV_ILN_4035
912			\|a GBV_ILN_4037
912			\|a GBV_ILN_4112
912			\|a GBV_ILN_4125
912			\|a GBV_ILN_4126
912			\|a GBV_ILN_4242
912			\|a GBV_ILN_4251
912			\|a GBV_ILN_4305
912			\|a GBV_ILN_4313
912			\|a GBV_ILN_4323
912			\|a GBV_ILN_4324
912			\|a GBV_ILN_4325
912			\|a GBV_ILN_4326
912			\|a GBV_ILN_4333
912			\|a GBV_ILN_4334
912			\|a GBV_ILN_4335
912			\|a GBV_ILN_4338
912			\|a GBV_ILN_4393
936	b	k	\|a 33.18 \|j Optik
936	b	k	\|a 33.38 \|j Quantenoptik \|j nichtlineare Optik
936	b	k	\|a 50.37 \|j Technische Optik
951			\|a AR
952			\|d 427 \|h 123-131

Indexfelder

author_variant	q c qc x s xs c l cl h w hw
matchkey_str	article:18730310:2018----::xeietleerhntecytossebsdnprlhsms
hierarchy_sort_str	2018
bklnumber	33.18 33.38 50.37
publishDate	2018
allfields	10.1016/j.optcom.2018.06.037 doi (DE-627)ELV000222550 (ELSEVIER)S0030-4018(18)30528-5 DE-627 ger DE-627 rda eng 530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Chen, Qi verfasserin aut Experimental research on JTC encryption system based on spiral phase mask and its characteristics 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to be improved. In order to improve its performance, the spiral phase mask (SPM) in singular optics is used as the key mask of the JTC encryption system. Under the JTC encryption system, the influence of SPM’s structure parameters on encryption–decryption effect was analyzed by means of theoretical analysis and numerical simulation. The influence of SPM and RPM on encryption–decryption effect and anti-attack ability were compared, and the initial experiment was conducted. The results indicated that the decryption effect is slightly improved when using SPM, the sensitivity of key is stronger, the key parameters are more, and the ability to resist the COA and CPA algorithm attack can be improved. The initial experiment results also verified the validity and correctness of our proposed method. Optical information security JTC encryption system Spiral phase mask Effect of encryption and decryption Shen, Xueju verfasserin aut Lin, Chao verfasserin aut Wang, Haoyi verfasserin aut Enthalten in Optics communications Amsterdam, 1969 427, Seite 123-131 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:427 pages:123-131 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik AR 427 123-131
spelling	10.1016/j.optcom.2018.06.037 doi (DE-627)ELV000222550 (ELSEVIER)S0030-4018(18)30528-5 DE-627 ger DE-627 rda eng 530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Chen, Qi verfasserin aut Experimental research on JTC encryption system based on spiral phase mask and its characteristics 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to be improved. In order to improve its performance, the spiral phase mask (SPM) in singular optics is used as the key mask of the JTC encryption system. Under the JTC encryption system, the influence of SPM’s structure parameters on encryption–decryption effect was analyzed by means of theoretical analysis and numerical simulation. The influence of SPM and RPM on encryption–decryption effect and anti-attack ability were compared, and the initial experiment was conducted. The results indicated that the decryption effect is slightly improved when using SPM, the sensitivity of key is stronger, the key parameters are more, and the ability to resist the COA and CPA algorithm attack can be improved. The initial experiment results also verified the validity and correctness of our proposed method. Optical information security JTC encryption system Spiral phase mask Effect of encryption and decryption Shen, Xueju verfasserin aut Lin, Chao verfasserin aut Wang, Haoyi verfasserin aut Enthalten in Optics communications Amsterdam, 1969 427, Seite 123-131 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:427 pages:123-131 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik AR 427 123-131
allfields_unstemmed	10.1016/j.optcom.2018.06.037 doi (DE-627)ELV000222550 (ELSEVIER)S0030-4018(18)30528-5 DE-627 ger DE-627 rda eng 530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Chen, Qi verfasserin aut Experimental research on JTC encryption system based on spiral phase mask and its characteristics 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to be improved. In order to improve its performance, the spiral phase mask (SPM) in singular optics is used as the key mask of the JTC encryption system. Under the JTC encryption system, the influence of SPM’s structure parameters on encryption–decryption effect was analyzed by means of theoretical analysis and numerical simulation. The influence of SPM and RPM on encryption–decryption effect and anti-attack ability were compared, and the initial experiment was conducted. The results indicated that the decryption effect is slightly improved when using SPM, the sensitivity of key is stronger, the key parameters are more, and the ability to resist the COA and CPA algorithm attack can be improved. The initial experiment results also verified the validity and correctness of our proposed method. Optical information security JTC encryption system Spiral phase mask Effect of encryption and decryption Shen, Xueju verfasserin aut Lin, Chao verfasserin aut Wang, Haoyi verfasserin aut Enthalten in Optics communications Amsterdam, 1969 427, Seite 123-131 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:427 pages:123-131 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik AR 427 123-131
allfieldsGer	10.1016/j.optcom.2018.06.037 doi (DE-627)ELV000222550 (ELSEVIER)S0030-4018(18)30528-5 DE-627 ger DE-627 rda eng 530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Chen, Qi verfasserin aut Experimental research on JTC encryption system based on spiral phase mask and its characteristics 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to be improved. In order to improve its performance, the spiral phase mask (SPM) in singular optics is used as the key mask of the JTC encryption system. Under the JTC encryption system, the influence of SPM’s structure parameters on encryption–decryption effect was analyzed by means of theoretical analysis and numerical simulation. The influence of SPM and RPM on encryption–decryption effect and anti-attack ability were compared, and the initial experiment was conducted. The results indicated that the decryption effect is slightly improved when using SPM, the sensitivity of key is stronger, the key parameters are more, and the ability to resist the COA and CPA algorithm attack can be improved. The initial experiment results also verified the validity and correctness of our proposed method. Optical information security JTC encryption system Spiral phase mask Effect of encryption and decryption Shen, Xueju verfasserin aut Lin, Chao verfasserin aut Wang, Haoyi verfasserin aut Enthalten in Optics communications Amsterdam, 1969 427, Seite 123-131 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:427 pages:123-131 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik AR 427 123-131
allfieldsSound	10.1016/j.optcom.2018.06.037 doi (DE-627)ELV000222550 (ELSEVIER)S0030-4018(18)30528-5 DE-627 ger DE-627 rda eng 530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Chen, Qi verfasserin aut Experimental research on JTC encryption system based on spiral phase mask and its characteristics 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to be improved. In order to improve its performance, the spiral phase mask (SPM) in singular optics is used as the key mask of the JTC encryption system. Under the JTC encryption system, the influence of SPM’s structure parameters on encryption–decryption effect was analyzed by means of theoretical analysis and numerical simulation. The influence of SPM and RPM on encryption–decryption effect and anti-attack ability were compared, and the initial experiment was conducted. The results indicated that the decryption effect is slightly improved when using SPM, the sensitivity of key is stronger, the key parameters are more, and the ability to resist the COA and CPA algorithm attack can be improved. The initial experiment results also verified the validity and correctness of our proposed method. Optical information security JTC encryption system Spiral phase mask Effect of encryption and decryption Shen, Xueju verfasserin aut Lin, Chao verfasserin aut Wang, Haoyi verfasserin aut Enthalten in Optics communications Amsterdam, 1969 427, Seite 123-131 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:427 pages:123-131 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik AR 427 123-131
language	English
source	Enthalten in Optics communications 427, Seite 123-131 volume:427 pages:123-131
sourceStr	Enthalten in Optics communications 427, Seite 123-131 volume:427 pages:123-131
format_phy_str_mv	Article
bklname	Optik Quantenoptik nichtlineare Optik Technische Optik
institution	findex.gbv.de
topic_facet	Optical information security JTC encryption system Spiral phase mask Effect of encryption and decryption
dewey-raw	530
isfreeaccess_bool	false
container_title	Optics communications
authorswithroles_txt_mv	Chen, Qi @@aut@@ Shen, Xueju @@aut@@ Lin, Chao @@aut@@ Wang, Haoyi @@aut@@
publishDateDaySort_date	2018-01-01T00:00:00Z
hierarchy_top_id	266889247
dewey-sort	3530
id	ELV000222550
language_de	englisch
fullrecord	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">ELV000222550</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230524141740.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230427s2018 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1016/j.optcom.2018.06.037</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)ELV000222550</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(ELSEVIER)S0030-4018(18)30528-5</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rda</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">DE-600</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.18</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.38</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">50.37</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Chen, Qi</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Experimental research on JTC encryption system based on spiral phase mask and its characteristics</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2018</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to be improved. In order to improve its performance, the spiral phase mask (SPM) in singular optics is used as the key mask of the JTC encryption system. Under the JTC encryption system, the influence of SPM’s structure parameters on encryption–decryption effect was analyzed by means of theoretical analysis and numerical simulation. The influence of SPM and RPM on encryption–decryption effect and anti-attack ability were compared, and the initial experiment was conducted. The results indicated that the decryption effect is slightly improved when using SPM, the sensitivity of key is stronger, the key parameters are more, and the ability to resist the COA and CPA algorithm attack can be improved. The initial experiment results also verified the validity and correctness of our proposed method.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Optical information security</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">JTC encryption system</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Spiral phase mask</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Effect of encryption and decryption</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Shen, Xueju</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Lin, Chao</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Wang, Haoyi</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Optics communications</subfield><subfield code="d">Amsterdam, 1969</subfield><subfield code="g">427, Seite 123-131</subfield><subfield code="h">Online-Ressource</subfield><subfield code="w">(DE-627)266889247</subfield><subfield code="w">(DE-600)1468811-6</subfield><subfield code="w">(DE-576)07596239X</subfield><subfield code="x">1873-0310</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:427</subfield><subfield code="g">pages:123-131</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ELV</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_32</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_74</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_90</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_100</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_101</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_150</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_224</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_702</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2003</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2004</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2005</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2011</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2015</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2020</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2021</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2025</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2027</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2034</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2038</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2044</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2048</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2049</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2050</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2056</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2059</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2061</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2064</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2065</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2068</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2111</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2113</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2118</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2122</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2129</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2143</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2147</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2148</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2152</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2153</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2190</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2336</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2507</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2522</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4035</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4242</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4251</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4326</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4333</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4334</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4393</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.18</subfield><subfield code="j">Optik</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.38</subfield><subfield code="j">Quantenoptik</subfield><subfield code="j">nichtlineare Optik</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">50.37</subfield><subfield code="j">Technische Optik</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">427</subfield><subfield code="h">123-131</subfield></datafield></record></collection>
author	Chen, Qi
spellingShingle	Chen, Qi ddc 530 bkl 33.18 bkl 33.38 bkl 50.37 misc Optical information security misc JTC encryption system misc Spiral phase mask misc Effect of encryption and decryption Experimental research on JTC encryption system based on spiral phase mask and its characteristics
authorStr	Chen, Qi
ppnlink_with_tag_str_mv	@@773@@(DE-627)266889247
format	electronic Article
dewey-ones	530 - Physics
delete_txt_mv	keep
author_role	aut aut aut aut
collection	elsevier
remote_str	true
illustrated	Not Illustrated
issn	1873-0310
topic_title	530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Experimental research on JTC encryption system based on spiral phase mask and its characteristics Optical information security JTC encryption system Spiral phase mask Effect of encryption and decryption
topic	ddc 530 bkl 33.18 bkl 33.38 bkl 50.37 misc Optical information security misc JTC encryption system misc Spiral phase mask misc Effect of encryption and decryption
topic_unstemmed	ddc 530 bkl 33.18 bkl 33.38 bkl 50.37 misc Optical information security misc JTC encryption system misc Spiral phase mask misc Effect of encryption and decryption
topic_browse	ddc 530 bkl 33.18 bkl 33.38 bkl 50.37 misc Optical information security misc JTC encryption system misc Spiral phase mask misc Effect of encryption and decryption
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
format_main_str_mv	Text Zeitschrift/Artikel
carriertype_str_mv	cr
hierarchy_parent_title	Optics communications
hierarchy_parent_id	266889247
dewey-tens	530 - Physics
hierarchy_top_title	Optics communications
isfreeaccess_txt	false
familylinks_str_mv	(DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X
title	Experimental research on JTC encryption system based on spiral phase mask and its characteristics
ctrlnum	(DE-627)ELV000222550 (ELSEVIER)S0030-4018(18)30528-5
title_full	Experimental research on JTC encryption system based on spiral phase mask and its characteristics
author_sort	Chen, Qi
journal	Optics communications
journalStr	Optics communications
lang_code	eng
isOA_bool	false
dewey-hundreds	500 - Science
recordtype	marc
publishDateSort	2018
contenttype_str_mv	zzz
container_start_page	123
author_browse	Chen, Qi Shen, Xueju Lin, Chao Wang, Haoyi
container_volume	427
class	530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl
format_se	Elektronische Aufsätze
author-letter	Chen, Qi
doi_str_mv	10.1016/j.optcom.2018.06.037
dewey-full	530
author2-role	verfasserin
title_sort	experimental research on jtc encryption system based on spiral phase mask and its characteristics
title_auth	Experimental research on JTC encryption system based on spiral phase mask and its characteristics
abstract	As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to be improved. In order to improve its performance, the spiral phase mask (SPM) in singular optics is used as the key mask of the JTC encryption system. Under the JTC encryption system, the influence of SPM’s structure parameters on encryption–decryption effect was analyzed by means of theoretical analysis and numerical simulation. The influence of SPM and RPM on encryption–decryption effect and anti-attack ability were compared, and the initial experiment was conducted. The results indicated that the decryption effect is slightly improved when using SPM, the sensitivity of key is stronger, the key parameters are more, and the ability to resist the COA and CPA algorithm attack can be improved. The initial experiment results also verified the validity and correctness of our proposed method.
abstractGer	As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to be improved. In order to improve its performance, the spiral phase mask (SPM) in singular optics is used as the key mask of the JTC encryption system. Under the JTC encryption system, the influence of SPM’s structure parameters on encryption–decryption effect was analyzed by means of theoretical analysis and numerical simulation. The influence of SPM and RPM on encryption–decryption effect and anti-attack ability were compared, and the initial experiment was conducted. The results indicated that the decryption effect is slightly improved when using SPM, the sensitivity of key is stronger, the key parameters are more, and the ability to resist the COA and CPA algorithm attack can be improved. The initial experiment results also verified the validity and correctness of our proposed method.
abstract_unstemmed	As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to be improved. In order to improve its performance, the spiral phase mask (SPM) in singular optics is used as the key mask of the JTC encryption system. Under the JTC encryption system, the influence of SPM’s structure parameters on encryption–decryption effect was analyzed by means of theoretical analysis and numerical simulation. The influence of SPM and RPM on encryption–decryption effect and anti-attack ability were compared, and the initial experiment was conducted. The results indicated that the decryption effect is slightly improved when using SPM, the sensitivity of key is stronger, the key parameters are more, and the ability to resist the COA and CPA algorithm attack can be improved. The initial experiment results also verified the validity and correctness of our proposed method.
collection_details	GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393
title_short	Experimental research on JTC encryption system based on spiral phase mask and its characteristics
remote_bool	true
author2	Shen, Xueju Lin, Chao Wang, Haoyi
author2Str	Shen, Xueju Lin, Chao Wang, Haoyi
ppnlink	266889247
mediatype_str_mv	c
isOA_txt	false
hochschulschrift_bool	false
doi_str	10.1016/j.optcom.2018.06.037
up_date	2024-07-06T17:15:03.419Z
_version_	1803850721181827072
fullrecord_marcxml	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">ELV000222550</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230524141740.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230427s2018 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1016/j.optcom.2018.06.037</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)ELV000222550</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(ELSEVIER)S0030-4018(18)30528-5</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rda</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">DE-600</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.18</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.38</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">50.37</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Chen, Qi</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Experimental research on JTC encryption system based on spiral phase mask and its characteristics</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2018</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">As a practical encryption method, the joint transform correlator (JTC) encryption method is one of the hot spots of optical encryption research. However, the key mask of JTC encryption system is usually random phase mask (RPM), the decryption effect of the image and the anti-attack ability need to be improved. In order to improve its performance, the spiral phase mask (SPM) in singular optics is used as the key mask of the JTC encryption system. Under the JTC encryption system, the influence of SPM’s structure parameters on encryption–decryption effect was analyzed by means of theoretical analysis and numerical simulation. The influence of SPM and RPM on encryption–decryption effect and anti-attack ability were compared, and the initial experiment was conducted. The results indicated that the decryption effect is slightly improved when using SPM, the sensitivity of key is stronger, the key parameters are more, and the ability to resist the COA and CPA algorithm attack can be improved. The initial experiment results also verified the validity and correctness of our proposed method.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Optical information security</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">JTC encryption system</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Spiral phase mask</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Effect of encryption and decryption</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Shen, Xueju</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Lin, Chao</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Wang, Haoyi</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Optics communications</subfield><subfield code="d">Amsterdam, 1969</subfield><subfield code="g">427, Seite 123-131</subfield><subfield code="h">Online-Ressource</subfield><subfield code="w">(DE-627)266889247</subfield><subfield code="w">(DE-600)1468811-6</subfield><subfield code="w">(DE-576)07596239X</subfield><subfield code="x">1873-0310</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:427</subfield><subfield code="g">pages:123-131</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ELV</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_32</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_74</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_90</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_100</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_101</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_150</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_224</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_702</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2003</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2004</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2005</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2011</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2015</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2020</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2021</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2025</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2027</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2034</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2038</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2044</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2048</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2049</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2050</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2056</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2059</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2061</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2064</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2065</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2068</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2111</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2113</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2118</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2122</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2129</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2143</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2147</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2148</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2152</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2153</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2190</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2336</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2507</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2522</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4035</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4242</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4251</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4326</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4333</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4334</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4393</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.18</subfield><subfield code="j">Optik</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.38</subfield><subfield code="j">Quantenoptik</subfield><subfield code="j">nichtlineare Optik</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">50.37</subfield><subfield code="j">Technische Optik</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">427</subfield><subfield code="h">123-131</subfield></datafield></record></collection>
score	7.401682

Nicht das Richtige dabei?

Schreiben Sie uns!

Experimental research on JTC encryption system based on spiral phase mask and its characteristics

Nicht das Richtige dabei?

Zugang & Verfügbarkeit

Vorhandene Bände

Nicht das Richtige dabei?