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Wireless Cellular Networks with Shadowing B. Blaszczyszyn , M.K. Karray NetGCooP Paris, 12–14 October 2011. – p. 1

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Page 1: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Wireless Cellular Networks withShadowing

B. Błaszczyszyn, M.K. Karray

NetGCooPParis, 12–14 October 2011.

– p. 1

Page 2: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Shadowing

In wireless communications, shadowing is deviation of thepower of the received electromagnetic signal from anaverage value.

Caused by obstacles affecting the wave propagation.

May vary with geographical position and/or radio frequency.

Usually modelled as a random process.

– p. 2

Page 3: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Shadowing

Commonly believed thatthe larger variance (variability?) in the shadowing processthe worse performance of wireless (cellular) communicationnetworks.

– p. 3

Page 4: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Shadowing

Commonly believed thatthe larger variance (variability?) in the shadowing processthe worse performance of wireless (cellular) communicationnetworks.Looks like yet another incarnation of the Ross’s conjecture...

– p. 3

Page 5: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Shadowing

Commonly believed thatthe larger variance (variability?) in the shadowing processthe worse performance of wireless (cellular) communicationnetworks.Looks like yet another incarnation of the Ross’s conjecture...

Happens not always to be true.

– p. 3

Page 6: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Shadowing

Commonly believed thatthe larger variance (variability?) in the shadowing processthe worse performance of wireless (cellular) communicationnetworks.Looks like yet another incarnation of the Ross’s conjecture...

Happens not always to be true.

Sometimes quite the opposite is true:a stochastic resonance...

– p. 3

Page 7: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Shadowing

Commonly believed thatthe larger variance (variability?) in the shadowing processthe worse performance of wireless (cellular) communicationnetworks.Looks like yet another incarnation of the Ross’s conjecture...

Happens not always to be true.

Sometimes quite the opposite is true:a stochastic resonance...

In particular, we will show that the call blocking probability incellular networks is not always increasing with theshadowing variance.

– p. 3

Page 8: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Outline of the Remaining Part of the Talk

Model Description,

Numerical Results

Some Mathematical Results

Concluding Remarks and Questions

– p. 4

Page 9: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

MODEL DESCRIPTION

– p. 5

Page 10: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Geometry of BS’s

Hexagonal network ΦH

∆ distance between adja-cent vertexes, surface ofthe cell

√3∆2/2, thus the

intensity λH = 2/(√3∆2)

BS/km2.

Uniformly shifted to make itstationary.Infinite or finite consideredon torus to neglect bound-ary effects.

1 2 3 4

1 2 3 4

A

B

C

D

A

B

C

D

∆4

∆42

31/2

T4

– p. 6

Page 11: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Geometry of BS’s; cont’d

Poisson network ΦP

number of points of Φp in anyset A, ΦP (A), is Poissonrandom variable with meanλP times the surface of A,

numbers of points ΦP (Ai) ofΦp in disjoint sets Ai are in-dependent random variables.

Intensity λP of BS/km2.Infinite or finite considered ontorus to neglect boundary effects.

– p. 7

Page 12: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Geometry of BS’s; cont’d

Hexagonal

“ideal” model

Poisson

“ad-hoc” deployed network

A general point process Φ?

– p. 8

Page 13: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

(Signal-Power) Path-Loss with Shadowing

Given BS X ∈ Φ (Φ = ΦP or ΦH) and location y ∈ R2 onthe plane, denote by 1/LX(y) the power of the signalreceived at y from X.

– p. 9

Page 14: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

(Signal-Power) Path-Loss with Shadowing

Given BS X ∈ Φ (Φ = ΦP or ΦH) and location y ∈ R2 onthe plane, denote by 1/LX(y) the power of the signalreceived at y from X.Assume:

LX(y) =L (|X − y|)SX(y)

(1)

where

L(·) is a non-decreasing, deterministic path-lossfunction,

SX(·) is a random shadowing field related to the BS X.

– p. 9

Page 15: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Deterministic Path-Loss Function

If not otherwise specified

L (r) = (Kr)β(2)

where K > 0 and β > 2 (path-loss exponent) are someconstants.

– p. 10

Page 16: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Shadowing Distribution

We will always assume that:

{SX(y)} are i.i.d. across BS’s X ∈ Φ and y ∈ R2

non-negative r.v’s.

normalized to E[SX(y)] = 1.

mean path-loss is finite, i.e., E[1/S] < ∞.

– p. 11

Page 17: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Shadowing Distribution

We will always assume that:

{SX(y)} are i.i.d. across BS’s X ∈ Φ and y ∈ R2

non-negative r.v’s.

normalized to E[SX(y)] = 1.

mean path-loss is finite, i.e., E[1/S] < ∞.

Of special interest is:

SX(y) ≡ 1 — no shadowing,

SX(y) = S is log-normal with mean 1; S = e−σ2/2+σN ,where N is standard (0, 1) Gaussian random variable.Call v = σ10/ log 10 logarithmic standard deviation(log-SD) of the shadowing; this is the SD of the path-lossLX(y) expressed in dB.

– p. 11

Page 18: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Spatial Service Policy

A given user at location y ∈ R2 is served by the BS X∗y ∈ Φ

from which it receives the strongest signal (i.e., the weakestpath-loss)

LX∗

y(y) ≤ LX(y) for all X ∈ Φ ,(3)

with any tie-breaking rule.

– p. 12

Page 19: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Spatial Service Policy

A given user at location y ∈ R2 is served by the BS X∗y ∈ Φ

from which it receives the strongest signal (i.e., the weakestpath-loss)

LX∗

y(y) ≤ LX(y) for all X ∈ Φ ,(3)

with any tie-breaking rule.

In the case of no shadowing (SX(y) ≡ 1) and strictlyincreasing path-loss function L(·) the above policycorresponds to the geographically closest BS.

For infinite network models with random shadowing, onehas to prove that the minimum of the path-loss isachieved for some BS.

– p. 12

Page 20: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

QoS “pre-metric” 1: Path-loss Factor

For a given location y ∈ R2 we define the path-loss factor as

l(y) := LX∗

y(y) =

1

maxX∈ΦSX(y)

L(|X−y|)

;(4)

i.e., as the path-loss experienced at y with respect to theserving BS (not to be confused with the path-lossexponent β).

– p. 13

Page 21: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

QoS “pre-metric” 1: Path-loss Factor

For a given location y ∈ R2 we define the path-loss factor as

l(y) := LX∗

y(y) =

1

maxX∈ΦSX(y)

L(|X−y|)

;(4)

i.e., as the path-loss experienced at y with respect to theserving BS (not to be confused with the path-lossexponent β).We will be interested in the mean path-loss factor

E[l(y)] = E[l(

y,Φ, SX(y), X ∈ Φ)

] .

By stationarity (of toroidal or infinite network model)E[l] := E[l(y)] = E[l(0)].

– p. 13

Page 22: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

QoS “pre-metric” 2: Interference Factor

For a given location y ∈ R2 we define the interference factoras

f(y) :=∑

X∈Φ,X 6=X∗

y

LX∗

y(y)

LX(y)=

X∈ΦSX(y)

L(|X−y|)

maxX∈ΦSX(y)

L(|X−y|)

− 1 .(5)

– p. 14

Page 23: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

QoS “pre-metric” 2: Interference Factor

For a given location y ∈ R2 we define the interference factoras

f(y) :=∑

X∈Φ,X 6=X∗

y

LX∗

y(y)

LX(y)=

X∈ΦSX(y)

L(|X−y|)

maxX∈ΦSX(y)

L(|X−y|)

− 1 .(5)

We will be interested in the mean interference factor

E[f(y)] = E[f(

y,Φ, SX(y), X ∈ Φ)

] .

By stationarity (of toroidal or infinite network model)E[f ] := E[f(y)] = E[f(0)].

– p. 14

Page 24: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Why E[l] and E[f ]?

The two QoS “pre-metrics”: mean path-loss factor E[l] andmean interference factor E[f ] are rather elementarycharacteristics, which give insight into more involved QoSmetrics, as e.g. the blocking probability.

– p. 15

Page 25: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking Probability in a Spatial Erlang’s Loss Model

Finite network (on torus), required space-time scenario;

(Poisson) arrival process (in time) of calls to the network,

calls require predefined (exponential) service times,

calls require predefined, fixed bit-rates (CBR),

blocking of arrivals when not enough resources (power,frequency etc),

fraction of blocked arrivals in the long run of the systemis called the blocking probability (bp).

– p. 16

Page 26: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking Probability in a Spatial Erlang’s Loss Model

Finite network (on torus), required space-time scenario;

(Poisson) arrival process (in time) of calls to the network,

calls require predefined (exponential) service times,

calls require predefined, fixed bit-rates (CBR),

blocking of arrivals when not enough resources (power,frequency etc),

fraction of blocked arrivals in the long run of the systemis called the blocking probability (bp).

Erlang’s loss formula: bp it is equal to the conditionalprobability that in the stationary configuration of the(non-blocked) arrival process the system cannot admit anew user, given all users in the current configuration canbe served.

– p. 16

Page 27: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking Probability; basic facts cont’d

Multi-Erlang (ME) form of call admission condition:∑

y:X∗

y=X

ϕ(

l(y), f(y))

≤ 1 ,(6)

where the summation is over all users (including a newarrival) to be served by the BS X and ϕ(·, ·) is somefunction of the path-loss and interference factorr (can bemore general) of user y.

– p. 17

Page 28: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking Probability; basic facts cont’d

Multi-Erlang (ME) form of call admission condition:∑

y:X∗

y=X

ϕ(

l(y), f(y))

≤ 1 ,(6)

where the summation is over all users (including a newarrival) to be served by the BS X and ϕ(·, ·) is somefunction of the path-loss and interference factorr (can bemore general) of user y.

If ME admission condition then the Erlang’s loss formulacan be practically evaluated, e.g. discretizing thegeometry and using the Kaufman-Roberts algorithm.

– p. 17

Page 29: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Multi-Erlang; downlink CDMA

ϕ(l, f) =ξ

1 + αξ

1

1 − ǫ

(Nl

P̃+ α+ f

)

;

- P̃ is the maximal BS power,

- ǫ is the fraction of this maximal power used in common(pilot) channels,

- α is the intra-cell orthogonality factor,

- N external noise power

- ξ = ψ−1(r/W ) is the SINR threshold corresponding to therequired bit-rate r of user given the link performancefunction ψ and the system bandwidth W ,

- ψ is the link performance function (e.g. for AWGN channelwith maximal capacity coding ψ(ξ) = log2(1 + ξ) is theShannon’s formula).

– p. 18

Page 30: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Multi-Erlang; downlink OFDMA

ϕ(l, f) =r

Wψ(

(1 − ǫ)/((Nl/P̃ ) + α+ f)) ,

with the notation as for CDMA.

– p. 19

Page 31: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

RESULTS

– p. 20

Page 32: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking Probability

We consider Hexagonal BS models on the torus TN withpower-law path-loss function (2) and log-normal shadowing.

– p. 21

Page 33: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking Probability

We consider Hexagonal BS models on the torus TN withpower-law path-loss function (2) and log-normal shadowing.

For a given realization of the shadowing field (in a suitablydiscretized geometry), we calculate the blocking probabilityvia the Kaufman-Roberts algorithm.

– p. 21

Page 34: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking Probability

We consider Hexagonal BS models on the torus TN withpower-law path-loss function (2) and log-normal shadowing.

For a given realization of the shadowing field (in a suitablydiscretized geometry), we calculate the blocking probabilityvia the Kaufman-Roberts algorithm.

Next, we average over many realizations of the shadowingfield.

– p. 21

Page 35: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking Probability

We consider Hexagonal BS models on the torus TN withpower-law path-loss function (2) and log-normal shadowing.

For a given realization of the shadowing field (in a suitablydiscretized geometry), we calculate the blocking probabilityvia the Kaufman-Roberts algorithm.

Next, we average over many realizations of the shadowingfield.

In practice, for a sufficiently large network (≥ 36 BS in oursetting) just one realization of the shadowing field is enough(spatial ergodicity).

– p. 21

Page 36: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking probability v/s shadowing

0

0.2

0.4

0.6

0.8

1

0 10 20 30 40 50 60

Mea

n bl

ocki

ng p

roba

b.

Logarithmic standard deviation of the shadowing

β=2.53

3.54

4.55

OFDMA, downlink, hexagonal network of 36 BS, cell radius 0.5 km.log-normal shadowing, path-loss exponent β, traffic 34.6 Erlang per km2.

– p. 22

Page 37: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking probability v/s shadowing, cont’d

0

0.2

0.4

0.6

0.8

1

0 10 20 30 40 50 60

Mea

n bl

ocki

ng p

roba

b.

Logarithmic standard deviation of the shadowing

β=2.53

3.54

4.55

OFDMA, downlink, hexagonal network of 36 BS, cell radius 0.5 km.log-normal shadowing, path-loss exponent β, traffic 23.1 Erlang per km2.

– p. 23

Page 38: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking probability v/s shadowing, cont’d

0

0.2

0.4

0.6

0.8

1

0 10 20 30 40 50 60

Mea

n bl

ocki

ng p

roba

b.

Logarithmic standard deviation of the shadowing

β=2.53

3.54

4.55

OFDMA, downlink, hexagonal network of 36 BS, cell radius 0.5 km.log-normal shadowing, path-loss exponent β, traffic 46.2 Erlang per km2.

– p. 24

Page 39: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Blocking probability v/s shadowing, cont’d

0

0.2

0.4

0.6

0.8

1

0 10 20 30 40 50 60

Mea

n bl

ocki

ng p

roba

b.

Logarithmic standard deviation of the shadowing

β=2.53

3.54

4.55

CDMA, downlink, hexagonal network of 36 BS, cell radius 0.5 km.log-normal shadowing, path-loss exponent β, traffic 46.2 Erlang per km2.

– p. 25

Page 40: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Back to Basics

Let’s try to understand the impact of the model parameters(in particular the variance of the shadowing) on E[l] andE[f ].

– p. 26

Page 41: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

E[l] in the Hexagonal Network; Simulation

100

150

200

250

300

350

400

450

500

550

0 10 20 30 40 50 60

10lo

g 10(

E[l(

0)])

Logarithmic standard deviation of the shadowing

β=3, T6T10T30

β=4, T6T10T30

β=5, T6T10T30

– p. 27

Page 42: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

E[f ] in the Hexagonal Network; Simulation

0

0.5

1

1.5

2

0 10 20 30 40 50 60

E[f(

0)]

Logarithmic standard deviation of the shadowing

β=3, T6T10T30

β=4, T6T10T30

β=5, T6T10T30

– p. 28

Page 43: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Observations for the Hexagonal Network

Mean path-loss factor increases in (log-SD of) theshadowing, increases in path-loss exponent, but(slightly) decreases in the network size.

Mean interference factor is not monotone in shadowing:first increases and then decreases (to 0, cf Prop. 1). Itdecreases in the path-loss exponent and increases inthe network size.

For more than 100 BS and reasonable path-loss modelassumptions E[l(0)] and E[f(0)] correspond to these inthe infinite model. However, for large values of log-SD ofthe shadowing E[f(0)] non-negligibly increases with thenetwork size.

– p. 29

Page 44: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Understanding the Blocking Probability

Graphical explanationof the possible non-monotonicityof the blocking probability.

+

=

variance of the shadowing

blocking probability

path−loss factor

interference factor

– p. 30

Page 45: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Poisson Network, path-loss factor

100

150

200

250

300

350

400

450

500

550

0 10 20 30 40 50 60

10lo

g 10(

E[l(

0)])

Logarithmic standard deviation of the shadowing

β=3, T6T10T30

R2

β=4, T6T10T30

R2

β=5, T6T10T30

R2

– p. 31

Page 46: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Poisson Network, interference factor

0

0.5

1

1.5

2

0 10 20 30 40 50 60

E[f(

0)]

Logarithmic standard deviation of the shadowing

β=3, T6T10T30

R2

β=4, T6T10T30

R2

β=5, T6T10T30

R2

– p. 32

Page 47: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Observations for Poisson network

Mean path-loss factor increases in shadowing, increasesin path-loss exponent, but decreases in the network size(same as for Hexagonal).

Mean interference factor decreases in the shadowing(unlike in Hexagonal!). It decreases in the path-lossexponent and increases in the network size (Same as forHexagonal).

For infinite Poisson network with arbitrary distribution ofshadowing, the QoS “pre-metrics” are known explicitlyand do not depend on the shadowing!; cf. Prop 3.

For large log-SD of the shadowing, the QoS“pre-metrics” of Hexagonal and Poisson network arevery similar.

– p. 33

Page 48: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

SO, WHAT CAN BE PROVED?SOME MATHEMATICAL RESULTS.

– p. 34

Page 49: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Log-Normal Shadowing with mean 1

S = e−σ2/2+σN where N is the standard Gaussian randomvariable. For any fixed ǫ > 0 we have

P{S ≥ ǫ} = P{N ≥ σ/2 + (log ǫ)/σ} σ→∞−→ 0 ,

which shows that the random variable S converges inprobability to 0 (hence path-loss 1/S converges to ∞).

This shows that path-loss factor l(y) converges in probabilityand in expectation to infinity.

– p. 35

Page 50: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Finite Networks, Increasing Shadowing

Proposition 1 Assume an arbitrary, fixed, finite pattern{X1, X2, . . . , Xn} of BS locations. Consider anydeterministic path-loss function 0 < L(r) < ∞ and(independent) log-normal shadowing SXi

(·) with thelog-SD v. Then for any location y we have

limv→∞

f(y) = 0 in probability.

Log-normal shadowing amplifies the ratio between thestrongest signal and all other signals thus reducing theinterference.

– p. 36

Page 51: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Finite Networks, Increasing Shadowing

Proposition 1 Assume an arbitrary, fixed, finite pattern{X1, X2, . . . , Xn} of BS locations. Consider anydeterministic path-loss function 0 < L(r) < ∞ and(independent) log-normal shadowing SXi

(·) with thelog-SD v. Then for any location y we have

limv→∞

f(y) = 0 in probability.

Log-normal shadowing amplifies the ratio between thestrongest signal and all other signals thus reducing theinterference.

Corollary 1 The mean interference factor E[f(0)] in thePoisson and hexagonal network on the torus TN , withlog-normal shadowing converges in distribution and inexpectation to 0 when log-SD of the shadowing goes to ∞.

– p. 36

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Finding Serving BS in Infinite Networks

Proposition 2 Consider infinite Poisson Φ = ΦP orhexagonal Φ = ΦH model of BS, with shadowing whosemarginal distribution has finite moment of order 2/β (a).Then there exist almost surely the serving BS, i.e., X∗

0 ∈ Φ

satisfying (3). Moreover, the interference factor calculatedwith respect to the restriction of Φ to TN , i.e., f(0, Φ̃TN ),converges almost surely and in expectation to f(0, Φ̃).

ai.e., E[S2/β] < ∞. Note that 2/β < 1 and thus the above assumption follows

from our default assumption E[S] = 1 < ∞.

– p. 37

Page 53: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Infinite Poisson Network

Proposition 3 Assume infinite Poisson network with thedeterministic path-loss function (2). The distribution of thepath-loss factor l(0) = l(0, Φ̃) and interference factorf(0) = f(0, Φ̃) do not depend on the (marginal) distributionof the shadowing field S = SX(y) provided E[S2/β] < ∞.Moreover, their expectations are given by

E[f(0)] =2

β − 2,

E[l(0)] =KβΓ(1 + β/2)

(πλE[S2/β])β/2,

where Γ(a) =∫∞

0ta−1e−tdt. Also, the distribution function

of l(0) admits a simple explicit expression.

– p. 38

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CONCLUDING REMARKS& QUESTIONS

– p. 39

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Concluding Remarks

Random shadowing is believed to degrade the QoS.

– p. 40

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Concluding Remarks

Random shadowing is believed to degrade the QoS.

Studying two QoS “pre-metrics” (path-loss with respectto the serving BS and interference factor) one discoversa more subtle reality.

– p. 40

Page 57: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Concluding Remarks

Random shadowing is believed to degrade the QoS.

Studying two QoS “pre-metrics” (path-loss with respectto the serving BS and interference factor) one discoversa more subtle reality.

As commonly expected: strong variance of theshadowing increases the mean path-loss with respect tothe serving BS, which in consequence, degradates mostof the QoS metrics.

– p. 40

Page 58: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Concluding Remarks

Random shadowing is believed to degrade the QoS.

Studying two QoS “pre-metrics” (path-loss with respectto the serving BS and interference factor) one discoversa more subtle reality.

As commonly expected: strong variance of theshadowing increases the mean path-loss with respect tothe serving BS, which in consequence, degradates mostof the QoS metrics.

However, the mean interference is not monotonic in thevariance of the shadowing. It first increases and thendecreases (asymptotically to zero!), when the shadowingvariance goes to infinity.

– p. 40

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Concluding Remarks; cont’d

For moderate shadowing, when the QoS is not yetcompromised by the path-loss conditions, it may profitfrom the reduction of the interference. This is becauseincreasing variance of the shadowing tends to "separate"the strongest (serving BS) signal from all other signals.

– p. 41

Page 60: Wireless Cellular Networks with Shadowingblaszczy/Shadowing_NetGCooP.pdf · Intensity λP of BS/km 2. Infinite or finite considered on torus to neglect boundary effects. – p

Concluding Remarks; cont’d

For moderate shadowing, when the QoS is not yetcompromised by the path-loss conditions, it may profitfrom the reduction of the interference. This is becauseincreasing variance of the shadowing tends to "separate"the strongest (serving BS) signal from all other signals.

Such phenomenon can be compared to stochasticresonance phenomena observed for some otherstochastic models.

– p. 41

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Concluding Remarks; cont’d

For moderate shadowing, when the QoS is not yetcompromised by the path-loss conditions, it may profitfrom the reduction of the interference. This is becauseincreasing variance of the shadowing tends to "separate"the strongest (serving BS) signal from all other signals.

Such phenomenon can be compared to stochasticresonance phenomena observed for some otherstochastic models.

Might shed new light, in particular on the design ofindoor communication scenarios.

– p. 41

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QUESTIONS OR COMMENTS?

THANK YOU

– p. 42