IEEE802.3aq%20Channel%20model%20ad%20hoc%20Task%202:%20Time-varying%20study%20 - PowerPoint PPT Presentation

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IEEE802.3aq%20Channel%20model%20ad%20hoc%20Task%202:%20Time-varying%20study%20

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Petre Popescu, Quake. Yu Sun, Optium. Robert Coenen, Scintera ... Petre Popescu, Quake. Petar Pepeljugoski, IBM. Paul Kolesar, Systimax. Piers Dawe, Agilent ... – PowerPoint PPT presentation

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Title: IEEE802.3aq%20Channel%20model%20ad%20hoc%20Task%202:%20Time-varying%20study%20


1
IEEE802.3aq Channel model ad hocTask 2
Time-varying study modal noise
  • Teleconference notes, 13 Oct 2004
  • Jonathan King

2
Agenda
  • attendees
  • update on activities
  • Time variance in MMF links - further tests
    -Robert Coenen
  • Proposed experiments on time-variation due to
    polarization and MMF shaking and initial results
    - Jonathan King
  • other business
  • next meeting date/time

3
1) Attendees
  • Jonathan King, Big Bear Networks
  • Petre Popescu, Quake
  • Yu Sun, Optium
  • Robert Coenen, Scintera
  • Piers Dawe, Agilent
  • John Ewen, JDSU
  • Petre Popescu, Quake
  • Petar Pepeljugoski, IBM
  • Paul Kolesar, Systimax
  • Piers Dawe, Agilent
  • Bretwood Lock, Phyworks
  • Gary Shaulov, Rsoft
  • Joerg Kropp, Infineon
  • Abijhit Shanbag, Scintera
  • please let me know if you or your organization
    have been missed

4
3)
  • a) Time variance in MMF links - further tests -
    Robert Coenen
  • Further experiments on vibrating a fibre coil
    (total of 10m fibre) vertically vibration
    amplitude was tailored as per GR 63 CORE (1g) A
    5GHz optical tone from a DFB laser was
    transmitted via an OSL launch and the vibration
    sidebands were recorded for worst case vibration
    axis and input polarization.
  • Key findings
  • Sideband height was proportional to the
    amplitude of movement.
  • Second and higher sideband ratios are
    consistantly smaller than first.
  • Max frequency at which vibration induced
    sidebands drop below -24dB (a nominal 'just
    noticeable' value) was 40Hz for the first
    sideband (24-28Hz for second and third
    sidebands).
  • Similar experiments with a 900MHz carrier showed
    significantly reduced envelope modulation,
    showing the effect was due to impulse response
    variation rather than amplitude modulation.
  • Optical switches introduced mode selective loss
    of 1dB before and after the main fibre
  • Questions raised during discussion
  • Was the noise floor affected by vibration,
    indicating a change in HF modal noise ?
  • What was the fibre impulse response, and how
    does the impulse vary through the vibration cycle
    ?

5
3)
  • b) Proposed experiments on time-variation due to
    polarization and MMF shaking and initial results
    - Jonathan King
  • Described test bed for measuring polarization
    and mechanical time varying effects, using a 3
    kinds of polarization explorer and 2 mechanical
    figure of 8 MMF shakers. Initial results compared
    envelopes of impulse response variation for a
    single mechanical MMF shaker (for 2 polarization
    inputs) a single mechanical MMF shaker and a
    polarization scrambler and 2 mechanical MMF
    shakers. Range of impulse response variation for
    last 2 shown to be equivalent.
  • Discussion following
  • TIA-F04 recommends a mechanical fibre shaker
    made up of 3 figure-of-8 elements.
  • There was some discussion the cause of
    polarization dependence of impulse response.
    Joerg Kropp confirmed that in his experiments,
    only polarization was varied, and that mode
    selective loss through the system was negligible.
  • Polarization induced variation of the channel
    was expected to depend somewhat on source type,
    because of spectral width differences.
    Polarization stability of VCSELs was raised as a
    potential issue in combination with the
    polarization effect, but experimental results
    with VCSELs did not show polarization instability
    to be an issue.

6
4) Other business
  • Petar Pepeljugoski requested a time slot in next
    weeks meeting for a presentation modal noise
    calculations

5) Next meeting
  • Wednesday 20th Oct 9.30am PCT, 5.30pm UK
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