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A Multi-Carrier UHF Passive RFID System

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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

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