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    An Overview of Modeling of Ultra Wide Band

    Indoor Channels

    Z. Irahhauten, H. Nikookar and G. Janssen

    Center for Wireless Personal Communications (CWPC)

    Department of Electrical Engineering, Mathematics and Computer Science-Delft University of Technology

    Mekelweg 4, 2628 CD Delft, The Netherlands

    Phone:+31-15-278 13 89, Fax: +31-15-278 40 46

    Email: {Z.Irahhauten, H.Nikookar, G.Janssen}@EWI.tudelft.nl

    Abstract In this paper an overview of the reported param-eters of the Ultra Wide Band (UWB) indoor wireless channelis presented. First, an introduction to UWB technology as well

    as UWB wireless channels is provided. Then, impulse responsemodel for the wireless indoor channel is introduced. The availableUWB channel measurements results in indoor environments areconsulted and accordingly, the major UWB channel parametersare presented and compared to those of conventional narrowband(i.e. narrowband as well as wide-band) systems (CNS). Thenovelty of this work is related to gathering different UWBwireless channel parameters, analysis and comparison, leadingto a conclusion on modeling of impulse radio channel.

    I. INTRODUCTION

    The world is now in a stage of major telecommunications

    revolutions. The need for multimedia communications and

    new flexible communication capabilities with high data rates

    and high Quality of Service (QoS) requirements becomeincreasingly important. To fulfill these demands, advanced

    research is needed in the field of communications. New

    wireless communication systems based on UWB technology

    have been introduced recently. The Federal Communication

    Commissions (FCC) recognized the significance of UWB

    technology in 1998 and initiated the regulatory review process

    of the technology. Consequently, FCC authorized the UWB

    technology for commercial uses with different applications,

    different operating frequency bands as well as the transmitted

    power spectral densities.

    Generally, UWB communications is based on the transmis-

    sion of very short pulses with relatively low radio energy. It has

    been in use for military applications and it may see increased

    use in the future for wireless communications and ranging

    according to its fine time resolution and its material penetration

    capability. UWB radio signals occupy a bandwidth more than

    the 25% of the center frequency [1]. This large bandwidthallows a very high capacity and accordingly, high processing

    gains that allow access of large number of users to the system.

    Meanwhile, since UWB can be a carrierless (i.e. baseband)

    radio technology, it requires no mixer. Therefore, the imple-

    mentation of a such system can be made simple, which means

    that low cost transmitters/receivers can be achieved when

    compared to the conventional radio frequency (RF) carrier

    systems.Several ways exist to build a model of the mobile radio

    propagation channel. One major way, which is concentrated

    in this paper, is to use stochastic methods, which describe the

    random behaviour of the UWB wireless channel at any time

    and for different propagation environments using a statistical

    approach.

    The structure of the paper is as follows. In section II the

    impulse response model of UWB channel is introduced, and

    relevant channel parameters are presented based on the results

    of UWB measurements reported in the literature. Comprehen-

    sive comparison and analysis of those channel parameters of

    UWB and CNS is given in section III. Concluding remarks

    appear in section IV.

    II. UWB MEASUREMENTS AND MODELS

    The UWB wireless channel can be fully described by its

    time-variant impulse response function h(t, ), which can beexpressed as follows:

    h(t, ) =Nn=1

    an(t)(t n(t))ejn(t) (1)

    where is the delay, t refers to the impulse response at instantt and is the Dirac delta function. The parameters of thenth path an , n , n and N are amplitude, delay, phase andnumber of multipath components, respectively. When UWB is

    a baseband signal, the phase in equation 1 can be kept out of

    consideration. The recent results of UWB measurements and

    channel modeling can be found in [2][9]. In the following,

    important models for UWB channel parameters are discussed.

    Power delay profile

    The average received power as function of the excess

    delay is called Power Delay Profile (PDP). UWB

    measurements performed in an office building show that

    the PDP is an exponential decreasing function with the

    delay [2], [3]. The Time Decay Constant (TDC) seems

    to follow a Lognormal distribution with mean of39.8 nsand standard deviation of 1.2 dB in an office building [2].Moreover, the reported results in [2], shows that the

    mean TDC is 29 35 ns and 41 56 ns for LOS andNLOS, respectively. However, the same author of [2],

    introduced another model refers to double exponential

    model based on clustering to characterize the PDP inUWB channel [4] and the corresponding parameters

    are shown in Table I. Furthermore, the reported results

    of [9] show that double exponential decay model seems

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    to match the UWB channel measurements for LOS as

    well as NLOS propagation. The UWB measurements

    performed in corridor show also that cluster phenomenon

    can be observed [5].

    Arrival times

    The arrival times of the multipath components for UWB

    seem to follow a negative exponential distribution andthe arrival rate of the multipath components is found to

    be 1/(2.3 ns) [4]. The number of multipath componentsarriving during an interval of maximum excess delay

    Tmax is equal to N = .Tmax with is the meanarrival rate of multipath components. This parameter is

    carefully investigated for different bin resolutions [10].

    The number of multipath increases when the resolution

    increases. The distribution of the number of path is also

    examined and Rayleigh distribution gives the best fit

    with standard deviation of = 7 and = 30 paths forLOS and NLOS, respectively [10].

    RMS delay spread

    The rms delay spread (RDS) parameter is a good measure

    of multipath spread because it determines the frequency

    selectively of the channel fading, which degrades the

    performance of digital communication systems over radio

    channels [11]. The RDS limits the maximum data trans-

    mission rate, which can reliably supported by the channel.

    In the case without using of diversity or equalization, the

    RDS is inversely proportional to the maximum usable

    data rate of the channel [12]. The RDS is defined as:

    rms =

    2 ()2 (2)

    where and 2 are the first and the second momentsof the power delay profile respectively, and are defined as:

    =n

    a2nn /n

    a2n =n

    P(n)n /n

    Pn(n)

    (3)

    where an, Pn, and n are amplitude, power anddelay, respectively. The results of UWB measurements

    show that RDS follows a Normal distribution with

    mean = 4.7 ns and = 8.2 ns and standarddeviation = 2.3 and = 3.3 for LOS and NLOS,respectively [6]. However, different statistics of RDS

    found in [3] show mean = 812 ns and = 1419 nsand standard deviation = 0.3 1 and = 1 5 forLOS and NLOS cases, respectively. In [10], RDS values

    of respectively, 9 ns and 11.5 ns for LOS and NLOSare reported.

    Fading

    A radio designer should know the fading margin, which

    needs to be taken into account in the selection of

    transmit power. The fading margin in UWB is found

    to be 5 dB [7] and the same result is found in [10].The measurement results reported in [5] show that the

    fading can be modeled by a Rice distribution with

    Rice factor of 9 dB. The results of [4] show thatfading follows a Rayleigh distribution. However, in [2]

    the Gamma distribution is reported to give the best

    fit for the amplitude distribution. In [9], the empirical

    distribution of path amplitudes is computed using a

    Kolmogorov-Smirnov test with 1% significance level,and the results show that Lognormal distribution gives

    the best fit when compared to the Rayleigh distribution

    for both LOS and NLOS cases.

    Correlation

    Wireless communication systems usually suffer formmultipath fading caused by propagation mechanisms such

    reflection, diffraction and scattering due to the obstacles

    in the channel. To combat this problem, techniques like

    diversity are used. This technique is more efficient in

    the case where the received signals are independent,

    but if the received signals are correlated, this leads to a

    limitation of the performance of the system [13]. Two

    types of correlation can be distinguished in the wireless

    channel, temporal and spatial correlation. The former

    means the correlation between multipath components

    arriving at the same profile but at different delays. The

    last means the correlation between multipath component

    collected at different profile but at the same delay [14].

    The temporal correlation is investigated in [2] between

    powers of the multipath components and the results

    show that the correlation coefficient does not exceed 0.2for UWB. The spatial correlation of UWB signals is

    investigated in [15]. The results show that the higher the

    separation distance, the lower the spatial correlation and

    the correlation is higher for LOS than NLOS propagation.

    Path loss

    For developing a good UWB communication system, a

    radio designer must know the path loss (PL) in order

    to determine the coverage area of the system. Path lossis defined as the ratio of the transmit signal power

    to the receive signal power [16]. Based on the UWB

    measurements in [2], the path loss exponent and the

    standard deviation of shadowing are 2.4 and 5.9 dB,respectively, and the best model for the shadowing is

    the Lognormal distribution. Different values for the path

    loss exponent are reported in [6] as 1.7 and 3.5 as wellas for the standard deviation of shadowing as 1.6 dBand 2.7 dB for LOS and NLOS, respectively. Accordingto [10], the path loss exponent and the standard deviation

    of the shadowing for LOS are 1.7 and 1.5 respectively,

    and for NLOS are 4.1 and 3.6, respectively. The relationbetween RDS and path loss is investigated in [6], [8].The results show that the higher the RDS, the higher the

    PL.

    III. COMPARISON AND ANALYSIS

    The PDP in UWB decreases exponentially with the delay

    because later paths experience more attenuation, and also the

    possibility of reflection. Due to strong reflectors situating in

    the channel, the PDP can follow a double exponential function.

    The same model is found for CNS [17], [18] (see Table I).

    According to Table I, the arrival rate of multipath components

    is remarkably higher for UWB than for CNS. This is due to the

    high time resolution in UWB, which means that more distinctpaths can be detected as illustrated in Figure 1 where BWrefers to the bandwidth.

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    Received

    signal

    excess delay

    1/BWCNS

    1/BWUWB

    Fig. 1. Illustration of the bandwidth (i.e. resolution) effect on the detectionof multipath components.

    The statistics of RDS for UWB seem to be smaller to those

    of CNS reported in [14]. This is due smaller maximum excess

    delay as well as smaller TDC of the clusters in the UWB case.

    The fading margin is much smaller in UWB than the

    fading margin of CNS, which is about 25 dB. This is becausea large number of received pulses do not interfere with eachother due to the large bandwidth occupied by UWB signals

    (see Figure 1). The condition for destructive interference

    between pulses in indoor propagation environment can

    be found in [19]. The reported Rice factor is remarkably

    small, and consequently, the Rice distribution converges to

    the Rayleigh distribution. However, since the number of

    multipath components arriving at a same delay (i.e. same bin)

    is remarkably small for UWB, the vector summation of the

    signals at that same delay gives less amplitude fluctuations,

    and the modeling of the fading with the Rayleigh distribution

    seems inappropriate. Therefore, some distribution functions

    are introduced to characterize the small-scale rapid fadingvariations in UWB indoor environments such as POCA

    (POlydorou-CApsalis) [20] and NAZU (Nakagawa-Arita-

    Zhang-Udagawa) [21] for the case of NLOS and LOS,

    respectively.

    Different reported path loss exponents are perhaps due to

    different types of the environments in where the measurements

    are performed. Additionally, the Lognormally distributed stan-

    dard deviations of shadowing are smaller for UWB when com-

    pared to those of CNS, which are found 312 dB [22]. Thiscan explained by the fact that UWB has a large bandwidth,

    which allows high capability of penetration trough the walls.A comparison of main UWB and CNS channel parameters are

    summarized in Table II.

    IV. CONCLUSION

    An overview of the reported UWB measurement results and

    channel modeling for indoor propagation environments in the

    literature was given. The UWB indoor wireless channel can

    be described by the impulse response model. The reported

    results show that the received UWB signal power decreases

    exponentially with the excess delay. The double exponential

    model can also be used to describe the PDP. The time decay

    constant depends on the type of the environments. The arrival

    times of the multipath components are negative exponentiallydistributed. The arrival rate of multipath components is higher

    for UWB than CNS due to high time resolution. The re-

    ported results indicate a limited correlation between powers

    ParameterWin Model

    [4]

    UWB CNS

    Saleh -

    Valenzuela [17]

    TDC of clusters

    (ns)

    1/2.30

    1/45.5

    84.1

    27.9

    Intraclusterarrival rate (ns-1)

    Cluster arrival

    rate (ns -1)

    TDC within cluster

    (ns)

    1/5

    1/300

    20

    60

    Spencer et. al [18]

    Building 2Building 1

    7833.6

    6.605.10

    17.316.8

    82.228.6

    Intel Model

    [9]

    1/0.5

    1/60

    1.6

    16

    TABLE I

    PDP DOUBLE EXPONENTIAL MODEL FOR THE UW B AND THE CNS.

    UWB CNS

    LOS

    RDSNLOS

    4-12 (ns)

    8-19 (ns)

    10-100 (ns)

    up to 200 (ns)

    Channel parameter

    Fading margin

    Fading

    distribution

    LOS Gamma / NaZu Rice

    NLOS

    5 dB 25 dB

    RayleighGamma / PoCa

    Path loss

    exponent

    LOS 1.5-2 1-3

    NLOS 2.1-62.4- 4

    Std. of

    Shadowing

    (Lognormal)

    LOS 1.1-2.1dB 3-6 dB

    NLOS 6-12 dB2-5.9 dB

    Temporal correlation 0.2 0.2-0.4

    Number of paths distribution Rayleigh Poisson

    Arrival times distribution Exponential Exponential

    TABLE II

    COMPARISON OF THE PROPOSED CHANNEL PARAMETER IN THE

    LITERATURE FOR UW B AN D CNS.

    of multipath components at the same profile. UWB signal

    are more robust against fading than CNS and the fading can

    be modelled by the Gamma distribution. The RDS seems to

    follow a Normal distribution, and its statistics are higher for

    the case of NLOS. The RDS values are smaller for the UWB

    than the CNS. The path loss increases with the distance. The

    path loss exponent as well as the shadowing standard deviationdepends on the propagation medium, and they are smaller for

    the UWB.

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