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Copyright © 2017 IJECCE, All right reserved

A New Design of Code for Optical Network for Security

Enhancement

Utkarsh Agrawal

*

and Sumit Gupta

Date of publication (dd/mm/yyyy): 04/03/2017

Abstract — This paper proposes a new method to develop the new code for optical network which uses the Double weight (DW) Code in bipolar mode with an improved ideal in phase cross correlation property at the receiver end. An Encoder is constructed in such way that the power of the cross - correlation pulse of a user is kept constant when another user is transmitting ‘0’ information bit while code assigned to both users is ideal in phase cross correlation. The chip position at the Cross correlation is switched in code to eliminate the continuous presence of a cross correlation spectral chip at the transmitter and receiver end when users in basic code transmit‘0’information bit. Mathematical and simulation analysis is carried out and the result shows the better performance than the existing code like RD and MQC codes.

Keywords — Optical Code Division Multiple Access (OCDMA), Spectral Amplitude Coding (SAC), Modified Quadratic Congruence Code (MQC), Multiple Access Interference (MAI), Modified Frequency Hopping (MFH).

I.

I

NTRODUCTION

In Optical code division multiplexing technique (OCDMA), multiple users share the same bandwidth simultaneously, the Spectral amplitude code(SAC) is one of the methods of OCDMA that have excellent ability to eliminate the Multiple access interference and complementary coding [1-2].In SAC each user assigns unique signature code in on off keying pattern there are several codes available, i.e. optical orthogonal code (OOC), MFH, Random diagonal(RD) and MQC these code have the various types of limiting factor such as too long length ,variable cross correlation (RD)[3-6]. The Long length of code is required the wide band spectrum and narrow filter bandwidth so it is limited in designing. MAI is a major source of noise that is totally eliminated by selecting the code with constant in phase cross correlation property. Double weight (DW) code maintains the constant in phase cross correlation property [7].

Security issue against the eavesdropper is one of the essential factors in OCDMA. In OOK based code, code is transmitted during ‘1’bit transmission and no light transmitted during ‘0’ bit so , by keeping the simple detector at transmitting end information can be detected[12] . A bipolar coding method is proposed to eliminate such a problem by assigning the codes to ‘0’ and ‘1’ information bit. But in bipolar scheme, by observing the spectrum at the transmitter terminal with required filter information can be detected. We have proposed a bipolar form of Double weight code by keeping the constant power of cross-correlation pulse of a user when another user transmitting 0 information while code assigned to both users is ideal in phase cross correlation The

switching of a cross correlation chip of the code is also performed to eliminate the continuous presence of a cross correlation spectral chip at the transmitter and receiver end while ‘0’ or ‘1’ bit is transmitted.

II.

M

ETHODOLOGY

A new design of bipolar code is developed for sending the power in both on and off case. The ‘off’ user has a same cross- correlation as an ‘on’ user, to maintain the power level of cross-correlation pulse to be constant. If both users in the off state than to eliminate the continuous presence of cross-correlation code at receiver end a switching of cross correlation code is performed. The switching of cross correlation pulse is presented the tri code at the transmitter and receiver end.

Basic matrix of double weight code is given as

𝐻0= [0 1 11 1 0] Bipolar form of double weight code

𝐻0= [0 1 1 1 1 010 1 1 10]

When user 1 or 2 are transmitting the 1 than code is given by

𝐻0= [0 1 1 1 1 0 0 0 00 0 0] User 1 is transmits 1 and User2 transmits 0 then

𝐻01= [0 1 1 0 1 0 0 0 00 0 1]

When user 1 or 2 are transmitting the ‘0’ than unity cross correlation position is given by 1’

𝐻02= [0 0 0 0 0 0 10 1 1 10]

Table1. Spectrum of code in two users

User Data bit

Code Position

User1 1 0 1 1 0 0 0

User2 1 1 1 0 0 0 0

User1 1 0 1 1 0 0 0

User2 0 0 1’ 0 0 0 1’

User1 0 0 1’ 0 1’ 0 0

User2 1 1 1 0 0 0 0

User1 0 0 0 0 1’ 1’ 0

User2 0 0 0 0 0 1’ 1’

Z.C.1 U.C.1 Z.C.2 Z.C.1 U.C2 Z.C.2

Mapping technique is used as soon as user increases. Code switching scheme code for information ‘0’ and ‘1’ switched according to the defined sequence so the code cannot be easily detectable at the transmitter side. Code switching sequence varies user to user.

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III.

E

NCODER

D

ESIGN

In this design two Broad band sources are used. In the encoder U.C1 represent the unity cross correlation spectrum as in table 1 when both users or any one user transmits ‘1’ and U.C2 represent the unity cross correlation spectrum when both transmit ‘0’. As same as Z.C1 and Z.C2 are a zero cross correlation spectrum of user 1 and 2 when transmit 1. (Z.C1) and (Z.C2) are the zero cross correlation pulse of user 1 and 2 when transmit 0.When user 1 transmit 1 then switch S11 select the Z.C1and U.C1. If user 1 is 0 then S11 selects the Z.C1 and U.C1 or U.C2 depends on the user 2.If user 2 transmits 0 than U.C.2 selects. In the case of 1, U.C2 selects. As same as when user 1 is 0 and user 2 transmit 1 than S1 selects Z.C.2 and U.C.1.

Fig.1Encoder of the proposed design with unity cross correlation code switching.

Table.2 Outputs selection in Encoder of proposed method

User1 User2 Output of S12 Output of S11 Output of S22 Output of S21

1 1 U.C.1 Z.C.1,U.C.1 U.C.1 Z.C.2,U.C.1

1 0 U.C.1 Z.C.1,U.C.1 U.C.1 𝑍. 𝐶2̅̅̅̅̅̅̅̅̅̅̅̅̅̅,U.C1

0 1 U.C.1 𝑍. 𝐶1̅̅̅̅̅̅̅̅̅̅̅̅̅̅,U.C1 U.C.1 Z.C.2,U.C.1 0 0 U.C.2 𝑍. 𝐶1̅̅̅̅̅̅̅̅̅̅̅̅̅̅,U.C2 𝑍. 𝐶2̅̅̅̅̅̅̅̅̅̅̅̅̅̅,U.C.2 𝑍. 𝐶2̅̅̅̅̅̅̅̅̅̅̅̅̅̅,U.C.2

Fig.2 Decoder of the proposed design

IV.

M

ATHEMATICAL

A

NALYSIS

BER1 For analysis of this system we use the Gaussian approximation in our calculation (3,4). This system is based on the direct detection technique so then we only consider the thermal noise (Rth) and shot noise (Rsn) in respect to PIIN. The SNR for electrical signal is the average signal power to noise power SNR = [I/ R]

Let CK(i) denotes the ith element of K user in this code

ZCC than

The following assumptions are made:

Each light source spectrum is flat over the bandwidth [Vo-∆V/2 , Vo– [Vo-∆V/2]where Vo is central frequency and ∆V is the optical source bandwidth in Hertz.

Each power spectral component has an identical spectral width.

Each user has nearly equal power at the transmitter Each user bit stream is synchronized

The power spectral density (PSD) of the received signals can be given as

Where u(v) is the unit step function expressed as:

Than The power spectral density (PSD) of the received signals can be given as

Where u(v) is the unit step function expressed as: Than The power spectral density (PSD) of the received signals can be given as

𝑟(𝑣) =𝑃𝑠𝑟 ∆𝑣∑ 𝑑𝑘 𝑘 𝑘−1 ∑ 𝑐𝑘 𝑁 𝑖−1 (𝑖)𝑟𝑒𝑐𝑡(𝑖)

𝑟𝑒𝑐𝑡(𝑖) = 𝑢 [𝑣 − 𝑣0−

∆𝑣

2𝑁(−𝑁 + 2𝑖 − 2)] − 𝑢 [𝑣 − 𝑣0−

∆𝑣

2𝑁(−𝑁 + 2𝑖)] = 𝑢 [ ∆𝑣

𝑁]

Where 𝑢(𝑣) is the unit step function expressed as:

𝑢(𝑣) = {1, 𝑣 ≥ 00, 𝑣 < 0

∫ 𝐺(𝑣)𝑑𝑣 = ∫ [𝑃𝑠𝑟 ∆𝑣∑ 𝑑𝑘 𝑘 𝑘−1 ∑ 𝐶𝑘(𝑖)𝐶𝐼(𝑖)𝑟𝑒𝑐𝑡(𝑖) 𝑘 𝑖−1 ] 0 0 𝑑𝑣 ∫ 𝐺(𝑣) 0 𝑑𝑣 =𝑃𝑠𝑟 ∆𝑣[∑ 𝑑𝑘 𝑘 𝑘−1 . 𝑊.∆𝑣 𝑁 + ∑ 𝑑𝑘 𝑘 𝑘≠1 .∆𝑣 𝑁]

The value of ∑𝑘𝑘−1𝑑𝑘 is equal to the 𝑤 and for above than

∫ 𝐺𝑑𝑑

0

(𝑣)𝑑𝑣 =𝑃𝑠𝑟[𝑤] 𝐿

The photo current I can be expressed as

𝐼𝑑𝑑 = ℜ ∫ 𝐺𝑑𝑑(𝑣) 0 𝑑𝑣 𝐼𝑑𝑑 = ℜ 𝑃𝑠𝑟[𝑤] 𝐿

The variation of photocurrent due to detection of an ideally un polarized thermal light can be expressed as

〈𝐼2〉 = 〈𝐼

12〉 + 〈𝐼𝑡ℎ2〉

〈𝐼2〉 = 2𝑒𝐵(𝐼

𝑑𝑑) +

4𝐾𝑏𝑇𝑛𝐵

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〈𝐼2〉 = 2𝑒𝐵ℜ [∫ 𝐺

𝑑𝑑(𝑣)𝑑𝑣

0

] +4𝐾𝑏𝑇𝑛𝐵 𝑅𝐿

When all users transmitting 1 than probability of each user sending 1 is ½ than equation …become

〈𝐼2〉 =𝑃𝑠𝑟𝑒𝐵ℜ

𝐿 [(𝐾 − 2 + 𝑤)] +

4𝐾𝑏𝑇𝑛𝐵

𝑅𝐿

The signal to noise ratio of direct detection technique is given by following equation

𝑆𝑁𝑅 =〈𝐼𝑑𝑑〉

2

〈𝐼2

When putting all equation than new formula for SNR will be

𝑆𝑁𝑅 =

ℜ2𝑃𝑠𝑟2𝑤2 𝐿2

𝑃𝑠𝑟𝑒𝐵ℜ

𝐿 ((𝐾 − 2 + 𝑤)) + 4𝐾𝑏𝑇𝑛𝐵

𝑅𝐿 Thus BER is

𝐵𝐸𝑅 =1

2𝑒𝑟𝑓𝑐√ 𝑆𝑁𝑅

8

Typical parameters used in the calculation as below: Photo detector quantum efficiency (g) 0.6 Line-width broadband source (∆V) 3.75 THz Operating wavelength (ko) 1552 nm Electrical bandwidth (B) 311 MHz Data bit rate (Rb) 622 Mbps Receiver noise temperature (Tn) 300 K Receiver load resistor (RL) 1030Ω

V.

R

ESULT AND

D

ISCUSSION

The block diagram of proposed scheme shown in fig 1 the simulation is done for 6 users with a weight of 2. The simulation is done in practical environment in all with all nonlinear effect is kept on. Simulation is performed for the 622Mbit/s for 50 km length of fiber and 2 Gbits/s for 20 km length of fiber with ITU standard single mode fiber (SMF). All the attenuation (α= 0.25dB/km), Dispersion (18ps/nm) is maintained

Fig.2 Eye pattern of 6 users at 50KM for 622Mbits/s

Fig.3. Eye pattern of 6 users at 20KM for 2Gbits/s Decoder side after decoding the signal, the signal covert to electrical by passing to the photo detector and 0.75 GHz low pass Bessel filter (LPF) The dark current value was 5 nA, and the thermal noise coefficient was 1.8x10-23 W/Hz for each of the photo-detectors. The performance of the system was characterized by referring to the BER and eye pattern. BER of the proposed Scheme shown that scheme gives better performance as the number user is increasing with comparatively lower bandwidth due to less number of weight. Shown in fig.4 the BER is provided more than minimum BER (10-9).

As in fig 5 and 7 either of 1 or 2 transmits ‘1’ information bit the power level of spectral pulse is constant. Fig .6 and 8 show the spectra of users when both are 1 or 0 bit. So there is no irregulaties occurs as in the existing method in power level when any one user transmits ‘1’ bit and other user transmits ‘0’ bit.fig.9 shows the variation in BER with received power and comparison is also done with MDW code.

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Fig.5 Spectrum of pulse when User 1 transmits 1 and

User2 transmits 0

Fig.6 Spectrum of pulse when User 1 transmits 1 and User2 transmit 1

Fig.7 Spectrum of pulse when User 1 transmits 0 and User2 transmits 1

Fig.8 Spectrum of pulse when User 1 transmits 0 and User2 transmits 0

Fig.9 BER Vs received power

VI.

C

ONCLUSION

In this paper, we have presented the bipolar technique in Double code. An encoder is also designed to maintain the power level of cross correlation pulse to be constant while user transmits 0 or 1. This design enhances the security against the eavesdropper by reducing the probability of code detection at the receiver ends and performance of code also compare with the present design.

R

EFERENCES

[1] J.A. Salehi, “Code division multiple access technique in optical fiber networks- Part I: Fundamentals principles,’’ IEEE Trans.

Commun.,1989, 37,pp: 824-833.

[2] M. Kavehrad and D. Zaccarin,“Optical code-division-multiplexed systems based on spectral encoding of noncoherent sources,” J. Lightw.Technol.,1995 vol. 13, no. 3, pp. 534–545. [3] F. R. K Chung, J. A. Salehi, V. K. Wei, 1989“Optical

Orthogonal Codes: Design, Analysis, and Applications,” IEEE

Trans. Information Theory,1989, vol. 35, no. 3.

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spectral-amplitude-coding optical CDMA systems". IEEE

Photon. Technol Lett.,2004, vol. 16,pp.2383-2385.

[5] Hillal Adnan Fadhil, S.A. Aljunid, R. B. Ahmed, 2009. “Effect of random diagonal code link of an OCDMA scheme for high-speed access networks,” J. Optical Fiber Technology, 2009,15, pp.237-241.

[6] Zou Wei, H.M.H. Shalaby, H. Ghafouri-Shiraz 2001, Modified quadratic congruence code for fiber Bragg-grating-based spectral-amplitude-coding optical CDMA system, J. Lightw.

Technol, 2001,19, pp.1274–1281.

[7] Syed Alwee, Alijunid, Zuraidah Zan, Siti Bariah Ahmad Anas, Mohd Khazani Abdullah 2004. A new code for optical code division multiple access systems. Malaysian Journal of

Computer Science,2004, 17 pp.30-39.

[8] Sangjo Park, Bong Kyu Kim , Chang-Soo Park 2004 ,“Performance enhancement using the bipolar capacity of bipolar coded fiber Bragg gratings and balanced detection in the spectral encoded code-division-multiple-access systems” Optics

Communications 2004,230( 4) , pp.319-324.

[9] Z. Wei and H. Ghafouri-Shiraz 2002, “Proposal of novel code for spectral amplitude-coding optical CDMA system,” IEEE

Photonics Technol.Lett.2002, Vol. 14 (3) pp.414 - 416 .

[10] C.-C. Yang and J.-F. Huang,2002 “Two-dimensional M-matrices coding in spatial/frequency optical CDMA networks,” IEEE

Photon. Technol.Lett., 2002,vol. 15,pp.168–170,

[11] T. Shake, 2005 "Security performance of optical CDMA against eavesdropping," J. Lightwave Technol,2005,23(2),pp.655-670.

A

UTHOR

'

S

P

ROFILE

Sumit Gupta,

He received the B.E. Degree in Electronics and communication engineering and M.tech Degree in VLSI and Microelectronics Design from RGPV, Bhopal. He is now Associate professor in department of Electronics and Communication Engineering Oriental colleges. of technology, Bhopal India. His current research interest includes VLSI, Optical Communication and Digital Communication

Utkarsh Agrawal,

References

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