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1 Mar. 7 doc.: IEEE c Project: IEEE P8.5 Working Group for Wireess Persona Area Networks N (WPANs) Tite: [A new LOS kiosk channe ode based on TSV ode] Date Subitted: [March, 7] Source: [Katsuyoshi Sato, Hirokazu Sawada, Yozo Shoji, Chang-Soon Choi, Ryuhei Funada, Hiroshi Harada, Shuzo Kato, Masahiro Uehira] Copany [Nationa Institute of Inforation and Counications Technoogy] Address [3-4, Hikari-no-Oka, Yokosuka, Kanagawa, , Japan] Voice:[ ], FAX: [ ], E-Mai:[satox@nict.go.jp] Re: [] Abstract: [This contribution describes a LOS kiosk channe ode based on TSV ode.] Purpose: [Contribution to W TG3c eeting.] Notice: This docuent has been prepared to assist IEEE P8.5. It is offered as a basis for discussion and is not binding on the contributing individua(s) or organization(s). The ateria in this docuent is subject to change in for and content after further study. The contributor(s) reserve(s) the right to add, aend or withdraw ateria contained herein. Reease: The contributor acknowedges and accepts that this contribution becoes the property of IEEE and ay be ade pubicy avaiabe by P8.5. Side

2 Mar. 7 doc.: IEEE c A new LOS kiosk channe ode based on TSV ode Katsuyoshi Sato, Hirokazu Sawada, Yozo Shoji, Chang-Soon Choi, Ryuhei Funada, Hiroshi Harada, Shuzo Kato, and Masahiro Uehira Nationa Institute of Inforation and Counication Technoogy (NICT), Japan Side

3 Mar. 7 doc.: IEEE c Suary Current kiosk environent (UM5) epoys LOS office channe ode (CM3) Soe channe ode users caied that the channe ode for UM5 contains excessivey strong refections We re-easured the propagation characteristics of the kiosk environent and created a new channe ode We suggest that the new channe ode be added on the current ode (UM5) Side 3

4 Mar. 7 doc.: IEEE c Probe of kiosk (UM5) channe ode Kiosk and office environents are quite different The eta was of offices cause strong refections, however, this is not true for kiosks In kiosk environents, distance between server and PDA is and huan body bocks arge deay refection waves, so the deay spread wi be saer than that in LOS office environents More suitabe channe ode for kiosk environents is required Side 4

5 Mar. 7 Measureent environent doc.: IEEE c Entrance ha of buiding With Objects that ook ike kiosk servers With Huan body Side 5

6 Mar. 7 Window Measureent environent 4. doc.: IEEE c Rotation Tabe (Step 5 ) Network Anayzer 6. Huan body Rx.5. Tx.5 Antenna Height:. Wa Wa Foor pan of LOS kiosk environent Side 6

7 Mar. 7 doc.: IEEE c Measureent environent Large roo in buiding:.x5.4 (situation: such as convenience store) Surrounded by paster boards and gass windows With Huan body Side 7

8 Mar. 7 doc.: IEEE c Wa 5.4 Wa tabes TV. Tx Rx.5..5 Huan body Ceiing Height:.7 Wa 3. Network Anayzer Measureent environent 6.9 Antenna Height:. 3. Piar Window Piar Side 8

9 Mar. 7 doc.: IEEE c Measureent conditions Instruent Center frequency Bandwidth Tie resoution Distance resoution # of frequency points Frequency step Averaging interva HP85C VNA 6.5 GHz 3 GHz.333 ns 9. c MHz 8 steps Caibration perfored with reference separation Tie resoution and distance resoution were deterined by bandwidth Side 9

10 Mar. 7 doc.: IEEE c Measureent conditions (cont ) Antenna: Conica horn antenna Poarization: Vertica Bea-width: Tx:3 and Rx 3 Conica horn antenna Bea-width 3 deg. Side

11 Mar. 7 doc.: IEEE c Exape: PDP (Power deay profie) in easureent environent (Bea width: Tx=3, Rx=3) Reative apitude [db] LOS direct-path coponent custers Tx Rx Deay tie [ns] Side

12 Mar. 7 doc.: IEEE c Ipuse response LOS direct path coponent Reative Apitude β Ω Rician factor (ΔK) Sa Rician factor (Δk) S-V ode response Γ,Λ,γ,λ Tie of Arriva By setting Γ =, TSV ode can generate ipuse response for LOS kiosk channe without any odification

13 Mar. 7 Side 3 doc.: IEEE c TSV ode for LOS kiosk environent () () ( ) ( ) L M T t t t h,,, ψ ϕ δ τ δ α δ β Ψ + = = = TSV ode = Two-path coponent + S-V coponent Refer to Appendix A for each paraeter Γ + = D h h j G G G G D f r t r t D exp λ π μ β Refection coefficient: Γ Modified TSV ode = Direct-path coponent + S-V coponent () () ( ) ( ) L M T t t t h,,, ψ ϕ δ τ δ α δ β Ψ + = = = t r D G G D = << μ β For LOS desk top environent (6/97) For LOS kiosk environent Statistica factors in both two-path and S-V Statistica factors in ony S-V

14 Mar. 7 doc.: IEEE c TSV ode paraeters to be extracted σ n(h (t)) AoA Ω σ γ Γ Δk Γ : custer decay factor / Λ : custer γ : ray decay factor / λ : ray arriva rate arriva rate σ : custer ognora standard deviation σ : ray ognora standard deviation σ φ : Ange spread of ray within custer σ φ Ω (Lapace distribution) : Average power of of the first custer the first ray Direct-path Response /Λ /λ ToA Sa Rican factor Δk and Ω are necessary for TSV ode Side 4

15 Channe ode LOS Kiosk easureent environent LOS Kiosk easureent environent LOS office Mar. 7 Paraeter Tx:3 Rx:3 Tx:3 Rx:3 Tx:3 Rx:3 Side 5 doc.: IEEE c Extracted TSV ode paraeters TSV Mode Ω (d) [db] -3.7D Sa Rician effect k (Δk). db 9.dB.9dB Γ [ns] S-V ode oriented paraeters /Λ [ns] γ [ns] /λ [ns] σ custer σ ray σ φ [deg] Siga and of kiosk environent are saer than those of LOS office environent Refer to Appendix B and C for each paraeter Nuber of custers N 5 7 6

16 Mar. 7 doc.: IEEE c Concusions Propagation characteristics of Kiosk environents were reeasured and TSV ode paraeters have been extracted A new channe ode for LOS kiosk environent has been created The New LOS Kiosk channe ode shoud be added on to the current UM5 channe ode Side 6

17 Mar. 7 doc.: IEEE c Appendix A: Definition of TSV ode A NLOS : Constant attenuation for NLOS Path nuber of G ti and G (: direct, : refrect) ri Two-path paraeters (4) S-V paraeters (7) d h h Unifor : Distance between Tx and Rx Unifor : Height of Unifor : Height of μ Average of distance between Tx and Rx Γ d α : Refection coefficient Γ Γ CIR: β [db] = og Tx Rx : LOS Desktop environent (incident ange π ) L M () t = β δ () t + α, δ ( t T τ, ) δ ( ϕ Ψ ψ ) h, = = (Copex ipuse response) τ γ k : Other LOS/NLOS environent [ δ ( ) ] G (, Ψ + ψ ), α Unifor [,π ) T Γ, =Ω, e e r,, Two-path response μ d d G G t r π h h + Gt Gr Γ exp j PLd λ f d ( μ ) d ( ) ( ) d PL = + d μ d [db] PLd d nd og PL d ( d ) 4π = [db] og + ANLOS d λ f d Arriva rate: Poisson process p p ( T T ) = Λ exp[ Λ( T T )], [ ( )], > ( τ τ, ( ) ) = λ exp λ τ τ, ( ) Γ : custer decay factor / Λ : custer γ : ray decay factor / λ : ray arriva rate arriva rate (Lapace distribution) > σ : custer ognora standard deviation σ : ray ognora standard deviation σ φ : Ange spread of ray within custer K PL d : Path oss of the first ipuse response t: tie[ns] δ( ): Deta function = custer nuber, = ray nuber in -th custer, L = tota nuber of custers; M = tota nuber of rays in the -th custer; T = arriva tie of the first ray of the -th custer; τ, = deay of the -th ray within the -th custer reative to the firs path arriva tie, T ; Ω = Average power of the first ray of the first custer Ψ Unifor[,π); arriva ange of the first ray within the -th custer ψ, = arriva ange of the -th ray within the -th custer reative to the first path arriva ange, Ψ Antenna paraeters () Gt Gr = L M = = ( θ, φ) : Antenna gain of Tx ( θ, ι) : Antenna gain of Rx Rician factor () k : ray Rician effect in each custer α, δ ( t T τ ) δ ( ϕ Ψ ψ ) G (, Ψ + ψ ), β, r, Side 7

18 Mar. 7 doc.: IEEE c n((α, )/α, ) ) - - y= x Γ=3.ns T [ns] Appendix B: Resuts of data anaysis Antenna beawidth n(-cdf) - y=-.546x /Λ=8.3-3 T [ns] Noraized reative power of ray y=-.74x-.99 γ=36.5[ns] Reative deay of ray [ns] n(-cdf) Tx: 3 deg, Rx: 3 deg y=-.99x /λ=.88[ns] τ, [ns] Custer decay factor (Γ) Custer arriva rate (/Λ) Ray decay factor (γ) Ray arriva rate (/λ) cdf AoA of custer [deg] pdf Ange of arriva in custer ( Unifor).5 y=e ( x) σ φ =34. [deg] AoA [deg] Ange spread of ray (σ φ ) cuuative probabiity Measureent Lognora σ = Reative path gain of custer [db] Standard deviation of custer (σ ) cuuative probabiity Measureent Lognora σ = Reative path gain of ray [db] Standard deviation of ray (σ ) Side 8

19 Mar. 7 doc.: IEEE c n((α, )/α, ) ) - - y= x Γ=64.ns T [ns] Appendix C: Resuts of data anaysis Antenna beawidth n(-cdf) - y=-.443x /Λ= T [ns] Noraized reative power of ray y=-.64x-.9 γ=6.[ns] Reative deay of ray [ns] n(-cdf) Tx: 3 deg, Rx: 3 deg y=-.x /λ=.988[ns] τ, [ns] Custer decay factor (Γ) Custer arriva rate (/Λ) Ray decay factor (γ) Ray arriva rate (/λ) cdf AoA of custer [deg] pdf.5 Ange of arriva in custer ( Unifor)..5 y=e ( x) σ φ =45.8 [deg] -5 5 AoA [deg] Ange spread of ray (σ φ ) cuuative probabiity Measureent Lognora σ = Reative path gain of custer [db] Standard deviation of custer (σ ) cuuative probabiity Measureent Lognora σ = Reative path gain of ray [db] Standard deviation of ray (σ ) Side 9

Project: IEEE P Working Group for Wireless Personal Area Networks N

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