08.11.2014 Views

A Multi-Carrier UHF Passive RFID System

A Multi-Carrier UHF Passive RFID System

A Multi-Carrier UHF Passive RFID System

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

A <strong>Multi</strong>-<strong>Carrier</strong> <strong>UHF</strong> <strong>Passive</strong> <strong>RFID</strong> <strong>System</strong><br />

Hsin-Chin Liu, Yung-Ting Chen, and Wen-Shin Tzeng<br />

Department of Electrical Engineering<br />

National Taiwan University of Science and Technology<br />

Taipei, 106, Taiwan<br />

hcliu@mail.ntust.edu.tw<br />

Abstract<br />

The “Gen2” specification for <strong>UHF</strong> passive <strong>RFID</strong><br />

system released by EPCglobal has become an intense<br />

research interest. A Gen2 tag derives its power from<br />

the RF wave emitted by a Gen2 <strong>RFID</strong> reader and<br />

responds its modulated backscatter signals to the<br />

reader. Due to the large propagation loss, the<br />

accessible range of a Gen2 tag is hence limited.<br />

Moreover, the readability of a Gen2 tag is often<br />

influenced by the multipath fading problem. In this<br />

paper we propose a multi-carrier <strong>UHF</strong> passive <strong>RFID</strong><br />

system that can effectively extend the accessible range<br />

of a Gen2 tag. In addition, we investigate the multiband<br />

backscatter property of Gen2 tags, which can be<br />

utilized to mitigate the multipath fading problems.<br />

1. Introduction<br />

The Radio frequency identification (<strong>RFID</strong>)<br />

technology with its prosperous market and its diverse<br />

applications has gained much attention recently. Owing<br />

to the low cost, small size, long accessible range tags,<br />

the <strong>UHF</strong> passive <strong>RFID</strong> system is especially promoted<br />

by EPCglobal. In 2005, The “Gen2” specification for<br />

<strong>UHF</strong> passive <strong>RFID</strong> system is released by EPCglobal<br />

[1]. Because a Gen2 tag derives its power from the RF<br />

waves emitted by a Gen2 <strong>RFID</strong> reader and responds its<br />

modulated backscatter (MBS) signals to the reader, the<br />

accessible range is hence limited due to the large<br />

propagation loss. Besides the free space attenuation,<br />

the multipath fading effect can often result in<br />

readability problems.<br />

In an ordinary EPCglobal Gen2 <strong>RFID</strong> system [1], an<br />

integrated reader not only transmits continuous waves<br />

(CW) to provide energy and the backscatter carrier to<br />

tags, but also sends the pulse-interval encoding (PIE)<br />

reader-to-tag (R-T) commands to tags and receives the<br />

tag-to-reader (T-R) responses. Assuming that the<br />

maximum accessible distance between a reader and a<br />

tag is d<br />

0<br />

, and the power of the CW emitted from the<br />

reader is P cw<br />

as shown in Figure 1(a). In accordance<br />

with the Friis equation [3], the received power of the<br />

P can be presented as Eq.(1).<br />

tag<br />

tag<br />

⎛ λ ⎞<br />

P = P G G<br />

tag cw ⎜ ⎟ , (1)<br />

⎝4π<br />

d<br />

reader tag<br />

0 ⎠<br />

where λ is the wavelength of the CW, G reader<br />

and<br />

G<br />

tag<br />

are the power gains of the reader and tag<br />

antennas respectively.<br />

When the tag is powered up, it listens for the R-T<br />

commands and adjusts its impedance match between<br />

the IC and antenna appropriately to respond the MBS<br />

T-R signals. The power of the MBS signal received at<br />

the reader Prx<br />

can be written as Eq.(2)<br />

2<br />

⎛ λ ⎞<br />

Prx = Ptag ⎜ ⎟ GreaderG<br />

. (2)<br />

tag<br />

⎝4π<br />

d0<br />

⎠<br />

Substituting P from Eq.(1) into Eq.(2), we see<br />

tag<br />

that P<br />

rx<br />

is reverse proportional to the four squares of<br />

d<br />

0<br />

.<br />

The accessible distance of a Gen2 tag is mainly<br />

determined by two factors: the power of the MBS<br />

received at the reader P rx<br />

and the received power of<br />

the tag P tag<br />

. For the former factor, a high sensitivity<br />

reader can solve the weak P rx<br />

problem. However, the<br />

latter one is more troublesome. An intuitive solution of<br />

increasing the P tag<br />

without tag modification is to<br />

enlarge the P cw<br />

. However it is impractical due to<br />

healthy concerns, the industrial, scientific and medical<br />

(ISM) band compliance issues, and the restriction of<br />

the local regulations.<br />

In order to overcome the insufficient P tag<br />

problem,<br />

we propose a multi-carrier <strong>UHF</strong> passive <strong>RFID</strong> system,<br />

2<br />

Proceedings of the 2007 International Symposium<br />

on Applications and the Internet Workshops (SAINTW'07)<br />

0-7695-2757-4/07 $20.00 © 2007


whose diagrammatic sketch is shown in Figure 1(b).<br />

The proposed system not only can provide sufficient<br />

energy to Gen2 tags but also can extend its accessible<br />

range. Furthermore, taking the advantages of multiple<br />

carriers, the reader can be benefited from the frequency<br />

diversity gain and the multipath fading problem can be<br />

mitigated.<br />

The remainder of this paper is organized as follows:<br />

Section 2 introduces the proposed system. Section 3<br />

presents the experimental results. Section 4 draws<br />

conclusions.<br />

2. The <strong>Multi</strong>-carrier <strong>UHF</strong> passive <strong>RFID</strong><br />

system<br />

Unlike the integrated reader in an ordinary <strong>UHF</strong><br />

passive <strong>RFID</strong> system, the reader in a multi-carrier <strong>UHF</strong><br />

passive <strong>RFID</strong> system is decomposed into two parts: a<br />

CW emitter (CWE) and a transceiver. The CWE can be<br />

preset leaky cables or radio source(s) close to tags,<br />

which emit a CW with frequency f<br />

c<br />

to illuminate tags.<br />

The CWE constantly provides energy and the MBS<br />

carrier(s) to the tags. The transceiver, which can be<br />

farther away from the tags, is mainly used to transmit<br />

the R-T commands and receive the T-R responses.<br />

As illustrated in Figure 1(b), the received power of<br />

the tag<br />

P<br />

'<br />

tag<br />

can be presented as Eq.(3).<br />

2<br />

' ' ⎛ λ ⎞<br />

c<br />

tag<br />

=<br />

cw ⎜ ⎟ cwe tag<br />

4π<br />

d1<br />

P P G G , (3)<br />

⎝ ⎠<br />

where P denotes the power of the CW emitted from<br />

'<br />

cw<br />

the CWE,<br />

λ<br />

c<br />

is the wavelength of the CW, and d 1<br />

is<br />

the distance between the CWE and the tag.<br />

G cwe<br />

and<br />

G<br />

tag<br />

are the power gains of the CWE and tag antennas<br />

respectively. In addition, the power of the MBS<br />

received at the reader<br />

P can be written as Eq.(4).<br />

'<br />

rx<br />

2<br />

' '<br />

⎛ λ ⎞<br />

rx<br />

=<br />

tag ⎜ ⎟ rx tag<br />

4π<br />

d2<br />

P P G G , (4)<br />

⎝ ⎠<br />

where G is the power gains of the transceiver, and<br />

rx<br />

d<br />

2<br />

is the maximum accessible distance between the<br />

transceiver and the tag. Assuming that the antenna<br />

gains of the CWE and the transceiver are the same as<br />

that of the integrated reader in an ordinary system<br />

( Gcwe = Grx = Greader<br />

), and the CW frequencies and<br />

powers in both systems are the same<br />

'<br />

( λ = λc,<br />

Pcw = Pcw), the power of received MBS in<br />

both system can be written as Eq.(5).<br />

' 4<br />

Prx<br />

d0<br />

= . (5)<br />

2 2<br />

Prx<br />

d1d2<br />

'<br />

When d1 < d0<br />

and Prx<br />

= Prx<br />

, d2 > d0<br />

can be<br />

derived. In other words, given the same receiver<br />

sensitivity and the same CW emission power, the<br />

proposed system can effectively extend the accessible<br />

distance between a tag and the receiver. Moreover,<br />

because the tags are plentifully illuminated by the<br />

CWE, the problem of insufficient tag operation energy<br />

is avoided.<br />

A simplified normal operation flow of the proposed<br />

system is illustrated in Figure 2. Before issuing an R-T<br />

command, the transceiver turns on the CWE to emit the<br />

CW, so that the tags nearby the CWE are powered up<br />

and ready for the R-T command. When the accessing<br />

operation is finished, the transceiver turns off the<br />

CWE, and the operation is then terminated.<br />

The proposed system may seem similar with an<br />

ordinary Gen2 system, except the additional CWE. As<br />

a matter of fact, they are substantially different. We<br />

discuss three major differences as below:<br />

2.1. The frequency difference between the<br />

transceiver and the CWE<br />

Because the transceiver and the CWE are<br />

separated in our proposed system, the carrier frequency<br />

of the transceiver ( f<br />

t<br />

) and the frequency of CW ( f<br />

c<br />

)<br />

emitted by the CWE can be different. Assuming the<br />

noise is negligible, the RF signal received by a tag can<br />

be expressed as Eq.(6).<br />

s t = m t cos 2π f t + Acos 2π f t+ φ t , (6)<br />

() () ( t ) ( c ())<br />

where<br />

⎧A , when high level is sent<br />

m()<br />

t =<br />

t<br />

⎨ denotes the<br />

⎩ 0, when low level is sent<br />

waveform of an R-T command from the transceiver,<br />

A denotes the amplitude of the RF signal transmitted<br />

t<br />

by the transceiver, A denotes the amplitude of the CW<br />

emitted by the CWE, and φ () t is the phase different<br />

between the two carriers. Let ∆ f = fc − ft<br />

. After<br />

some manipulations, Eq.(6) can be rewritten as Eq.(7).<br />

s( t) = ⎡<br />

⎣m( t) + Acos( 2π∆ ft+<br />

φ( t)<br />

) ⎤<br />

⎦cos( 2π<br />

ftt)<br />

.(7)<br />

+ Asin 2π∆ ft+<br />

φ t sin 2π<br />

f t<br />

( ()) ( t )<br />

The signal s()<br />

t is firstly passed through the<br />

envelope detection circuit inside the tag IC as shown in<br />

Proceedings of the 2007 International Symposium<br />

on Applications and the Internet Workshops (SAINTW'07)<br />

0-7695-2757-4/07 $20.00 © 2007


Figure 3 [2]. Let s () t denote the output of the circuit<br />

as presented in Eq.(8).<br />

e<br />

e<br />

2 2<br />

() = () + + 2 () cos( 2π∆ + φ()<br />

)<br />

s t m t A Am t ft t<br />

.(8)<br />

Utilizing the Taylor series, se<br />

() t can be expanded as<br />

Eq.(9).<br />

2 2 1<br />

⎡2Am () t cos( 2π∆ ft + φ()<br />

t ) ⎤<br />

Se<br />

() t = A + m () t i{1 + ⎢<br />

⎥<br />

2 ⎢<br />

2 2<br />

⎣<br />

A + m () t ⎥<br />

⎦<br />

2<br />

1<br />

⎡2Am() t cos ( 2π∆ ft + φ()<br />

t ) ⎤<br />

− ⎢<br />

⎥ + remainders}<br />

8<br />

2 2<br />

⎢<br />

⎣<br />

A + m () t ⎥<br />

⎦<br />

.(9)<br />

se<br />

() t is then passed through the LPF as depicted in<br />

Figure 3. Assuming ∆f<br />

is sufficiently large; the high<br />

frequency terms are filtered by the LPF. The<br />

output se<br />

() t can be approximated as Eq.(10).<br />

2 2 1<br />

se<br />

() t = A + m () t −<br />

. (10)<br />

2 2<br />

4 A + m () t<br />

As shown in experimental results, the R-T<br />

command can be correctly recognized by Gen2 tags<br />

under such a circumstance. Contradictorily, when ∆ f<br />

is small, the R-T command is distorted by the CW<br />

emitted by the CWE, and Gen2 tags do not respond the<br />

command.<br />

2.2. The modulation depth of R-T commands<br />

In [1], the modulation depth (MD) of a valid R-T<br />

command is specified to be greater than 80% and less<br />

than 100% in terms of the incident electric field<br />

strength at the tags. The MD is defined as Eq.(11).<br />

EA<br />

− EB<br />

MD = , (11)<br />

EA<br />

where E<br />

A<br />

and E<br />

B<br />

denote the maximum and<br />

minimum amplitudes of the RF envelope in an R-T<br />

command respectively. Figure 4(a) and Figure 4(b)<br />

illustrate an R-T command in an ordinary Gen2 system<br />

and in the proposed system respectively. From Eq.(10)<br />

and Eq.(11), the MD in our proposed system can be<br />

2 2 2 2<br />

A + A − A / A + A .For the<br />

presented as ( t )<br />

typical MD=90%, the power relation between the CWE<br />

and the transceiver can be derived as Eq.(12).<br />

t<br />

P / d + P / d − P / d<br />

' ' '<br />

cw 1 tx 2 cw 1<br />

'<br />

'<br />

Pcw<br />

/ d1+<br />

Ptx<br />

/ d2<br />

= 90% , (12)<br />

'<br />

where P<br />

tx<br />

denotes the maximum transmission power<br />

of the transceiver while sending an R-T command.<br />

2.3. The detection symbol in R-T Commands<br />

In order to decode an R-T command, the tag IC must<br />

have a PIE decoder, which is an edge detector [2]. A<br />

regular Gen2 R-T command cannot be directly used in<br />

the proposed system, because the first falling edge and<br />

the last rising edge of the R-T command, as depicted in<br />

Figure 4(a), cannot be detected by tags. In order to be<br />

compliant with Gen2 tags, two short detection symbols<br />

are added to the head and the tail of each R-T<br />

command in the proposed system as illustrated in<br />

Figure 4(b).<br />

3. Experimental results<br />

An Agilent 89601 vector signal analyzer<br />

incorporating with an Agilent E4445A spectrum<br />

analyzer is used to capture the communication signals<br />

between the transceiver and a Gen2 tag. The<br />

frequencies of the CWE and the transceiver are<br />

915MHz and 917MHz respectively. The R-T Tari is<br />

25us, and the duration of the both detection symbols<br />

are 11us. The powers of the CWE and the transceiver<br />

are adequately adjusted, so that the MD requirement is<br />

satisfied. The snapshots are taken nearby the tags.<br />

Figure 5 shows that the tag MBS is relatively strong.<br />

Under such a circumstance, the accessible range of the<br />

tag can be extended to 4 times longer than that of an<br />

ordinary Gen2 system with the same emission power.<br />

Figure 6 demonstrates an interesting multi-band<br />

backscatter property of Gen2 tags. We let the<br />

transceiver not only send the R-T commands but also<br />

send a low power CW during the tag responses. We<br />

found that the tag MBS presents not only in the carrier<br />

frequencies of CWE but also in the carrier frequencies<br />

of the transceiver (917MHz) as illustrated in Figure 6.<br />

This phenomenon implies that we can apply the<br />

frequency diversity technology (using a multi-carrier<br />

CWE, for instance) to enhance the quality of the tag<br />

MBS and to mitigate the multipath fading problem.<br />

4. Conclusion<br />

In this paper, we proposed a multi-carrier <strong>UHF</strong><br />

passive <strong>RFID</strong> <strong>System</strong>, which can effectively extend the<br />

accessible range of Gen2 tags. Moreover, the multiband<br />

backscatter property of Gen2 tags, which is<br />

Proceedings of the 2007 International Symposium<br />

on Applications and the Internet Workshops (SAINTW'07)<br />

0-7695-2757-4/07 $20.00 © 2007


explored in this paper, can be utilized in future <strong>RFID</strong><br />

system design.<br />

Acknoledgement<br />

Amplitude<br />

First falling<br />

edge<br />

Last rising<br />

edge<br />

E A<br />

This study is partially supported by the National<br />

Science Council of Taiwan under grant no.NSC94-<br />

2218-E-011-011 and Yuen Foong Yu Paper MFG. CO.<br />

References<br />

[1] EPC TM Radio-Frequency Identity Protocols Class-1<br />

Generation-2 <strong>UHF</strong> <strong>RFID</strong> Protocol for Communications at<br />

860MHz-960MHz Version 1.09,<br />

http://www.epcglobalinc.org, 2005.<br />

[2] Zheng Zhu, “<strong>RFID</strong> Analog Front End Design Tutorial,”<br />

http://autoidlabs.eleceng.adelaide.edu.au/Tutorial/<strong>RFID</strong>a<br />

nadesign.pdf, 2004.<br />

[3] A Paulraj, R. Nabar, and D. Core, Introduction to Space-<br />

Time Wireless Communications, Cambridge University<br />

Press, 2003.<br />

(a)<br />

(b)<br />

TAG TAG<br />

P<br />

tag<br />

P<br />

'<br />

tag<br />

d 1<br />

d 0<br />

d 2<br />

'<br />

P cw<br />

CWE<br />

P rx<br />

P cw<br />

Reader<br />

'<br />

P rx<br />

Transceiver<br />

'<br />

P tx<br />

Figure 1. (a) An ordinary <strong>UHF</strong> passive <strong>RFID</strong><br />

system. (b)The multi-carrier <strong>UHF</strong> passive <strong>RFID</strong><br />

system.<br />

Amplitude<br />

E A<br />

(a)<br />

Head Detection<br />

Symbol<br />

E B<br />

E B<br />

(b)<br />

Figure 4. (a) The amplitudes of the RF envelope<br />

in an R-T command in an ordinary Gen2 system.<br />

(b) The amplitudes of the RF envelope in an R-T<br />

command in the proposed system.<br />

t<br />

Tail Detection<br />

Symbol<br />

t<br />

CWE<br />

on<br />

CW<br />

off<br />

Transceiver<br />

Turn on<br />

Query<br />

…<br />

Turn off<br />

Gen2 tags<br />

Figure 2. A simplified operation flow for the multicarrier<br />

<strong>UHF</strong> passive <strong>RFID</strong> system.<br />

t<br />

Figure 5. A snapshot of the R-T and T-R<br />

communications around 915 MHz, which is the<br />

frequency of the CW emitted by the CWE.<br />

Antenna<br />

Rectifier<br />

LPF<br />

Hysteresis<br />

Comapator<br />

Envelope<br />

Detector<br />

Figure 3. The RF envelope detection and low pass<br />

filter inside an <strong>UHF</strong> passive tag [2].<br />

Figure 6. A snapshot of the R-T and T-R<br />

communications around 917 MHz, which is the<br />

carrier frequency of the transceiver.<br />

Proceedings of the 2007 International Symposium<br />

on Applications and the Internet Workshops (SAINTW'07)<br />

0-7695-2757-4/07 $20.00 © 2007

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!