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Hi Ali Thanks for your e-mail - the statement to note recent work in T.11 is just that – we should take note of the work and look at what the consequences are for Ethernet rates. My understanding of the spreadsheet is that the MPN penalty is counted just once: the average effect of chromatic dispersion for a multimode source with a given rms spectral width is included in the ISI penalty; the MPN term just accounts for the noise term due to power moving around between laser modes. Can you explain what you mean by double counting ? Thanks jonathan From: Ali Ghiasi [mailto:aghiasi@xxxxxxxxxxxx] Jonathan In regard to statement given in your presentation, I like to add some more color to this statement • Note: recent work on MPN treatment, by David Cunningham, shown in T11 (Fibre Channel), indicates that FEC is a necessity for 100m links 32GFC operates at 28.05 GBd, current spreadsheet model do show very steep increase in penalty as result of mode partition noise and cross terms. The FC group wants to support 100 m on OM4 fiber, with current noise model even with a simple FFE EQ FEC would be required to close the link budget. Also the same spreadsheet shows that if we added FEC with overhead and operated at 28 GBd instead of 25.78 with 2.5 dBo or 5 dBe penalty we could be worse off than using FEC. So our only option would be to use inband FEC which has higher latency. With 100GNGOPTX investigating 2nd generation set of PMD where there already exist set of solution, as a group we have to deliver a solution which allow seamless migration from 40G-SR4 and is lower cost than 100G-SR10. If it requires fundamental investigation then the group need to undertake it! My concern with current spreadsheet model which I have also shared with David Cunningham is how B (bandwidth) is used for calculation of MPN, for mode partition noise and the cross term for detail analysis please see David presentation B= 1/(T-DCD) where T is the 1/Baudrate â=π.B.D.L.σλ.λ σmpn = kOMA/√2 . [1 - e^(-β^2)] I do agree in the ISI calculation we should use DCD to increase the effective baudrate but if you have slow laser which is the case for 25.78 operation both ISI and MPN do not increase the laser is toggling faster but never reaches steady state! The spreadsheet already captures the ISI penalty and double counting might have been negligible at lower speed when the laser were fast but double counting at these speed breaks the link or we end up with a link significantly shorter! What seems reasonable here is to use the current B for ISI penalty calculation but for MPN and Cross use the following B1= 0.35/(Teff) where Teff is the RMS mean of sqrt(Trise^2+Tfall^2/2) as I expect current Ts is in the spreadsheet is the Tfall time. Thanks, Ali On Feb 13, 2012, at 5:52 PM, Jonathan King wrote: Dear all, Here is my presentation for the MMF ad hoc call , 14th Feb 2012 This is intended to be an introduction to, and framework for, discussion on what we do as an ad hoc to progress towards an MMF objective. Best wishes jonathan From: Anslow, Peter [mailto:panslow@xxxxxxxxx] Hi, By popular request, we have moved this meeting to Tuesday 14 February at the same time as before. (With apologies to Paul who now can’t attend.) Hi, As mentioned by Dan, Jonathan and I are planning to hold an SMF Ad Hoc meeting immediately followed by an MMF Ad Hoc meeting (1 hour each) starting at 8:00 am Pacific on Tuesday 14February. Peter Anslow from Ciena has invited you to join a meeting on the Web, using WebEx. Please join the meeting 5-10 minutes early so we may begin on time. 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