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Course contents

  • How to Use This Course
  • Reading Path
  • STA Glossary
  • STA Metrics Reference
  • STA Mastery Cheatsheet
  • Timing Paths and Checks16
  • Constraints & SDC Fundamentals20
  • Delay Graph & Path Analysis16
  • Beyond Setup and Hold16
  • Multi-Corner Multi-Mode Signoff16
    • Corner and Mode Matrix Design
    • Library Sets and Operating Conditions
      • Library Sets
      • Operating Conditions
      • RC Corner Mapping
      • Temperature Inversion
    • Signoff vs Implementation Views
    • MMMC Debug Playbook
  • OCV, AOCV, POCV and Variation16
  • Crosstalk and Noise16
  • ECO and Closure16
  • STA Debug Playbook16
  • STA Interview Prep26
  • Capstone Timing Signoff Lab4
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‹Library Sets and Operating Conditions
  1. Topics
  2. Static Timing Analysis
  3. Multi-Corner Multi-Mode Signoff
  4. Library Sets and Operating Conditions
  5. Operating Conditions

Part 5 · Multi-Corner Multi-Mode · All levels

Operating Conditions

Operating conditions name the voltage and temperature of a scenario; a supply droop costs more nanoseconds at low voltage, so it matters most there.

On this page

    Why it matters

    Libraries are characterised at discrete points. The supply seen by cells in the chip is not exactly the characterised one: it sags under load. Understanding how steeply delay depends on voltage shows how much a small droop costs in nanoseconds, and why the cost is largest at low-voltage corners.

    Voltage sensitivity (illustrative)

    example.py
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    # Relative delay of a reference path at three characterised voltages (typical process, hot).
    points = {0.72: 1.30, 0.80: 1.00, 0.88: 0.82}
    slope_low = (points[0.72] - points[0.80]) / (0.80 - 0.72)      # delay change per volt, low segment
    slope_high = (points[0.80] - points[0.88]) / (0.88 - 0.80)
    assert abs(slope_low - 3.75) < 1e-9 and abs(slope_high - 2.25) < 1e-9
    assert slope_low > slope_high
    # 30 mV of droop at the low corner, applied to a path that takes 0.90 ns there (linear estimate)
    droop = 0.030
    delta = 0.90 * droop * slope_low / points[0.72]
    assert round(delta, 3) == 0.078
    print("PASS: slope low", slope_low, "high", slope_high, "; 30 mV droop adds about", round(delta, 3), "ns to a 0.90 ns path")

    Between 0.72 V and 0.80 V relative delay changes by 3.75 per volt, between 0.80 V and 0.88 V by only 2.25 per volt in absolute terms. Relative to each path's own delay that is 3.75 / 1.30, about 2.9 per volt at 0.72 V, against 2.25 / 0.82, about 2.7 per volt at 0.88 V: almost the same fractionally. A droop costs more nanoseconds at low voltage mostly because the path is longer in ns there. A 30 mV droop on a 0.90 ns path at 0.72 V is therefore worth roughly 0.078 ns, about 8.7% of the path as a linear estimate at 0.72 V. This is a linear estimate for orientation only; real analysis uses libraries at the lowered voltage or a calibrated margin, not this line.

    How droop is handled

    Method

    Idea

    Cost

    Margin in the corner

    Characterise the corner at a lower voltage than nominal

    Pessimism applied everywhere

    Voltage-aware libraries

    Run a scenario at the drooped voltage for affected regions

    More libraries and scenarios

    Derate on affected cells

    Apply a delay derate to cells in hot regions

    Needs a trustworthy droop map

    What the review looks for

    • Slow (setup) corners use nominal minus tolerance and droop, and fast (hold) corners use nominal plus tolerance, each justified against the agreed budget.

    • The droop budget comes from power analysis and is reviewed when the floorplan or activity changes.

    • Low-voltage scenarios get the closest review, because a droop costs most nanoseconds there.

    Common pitfall

    Using nominal voltage for the slow corner. The slow corner is the one that must also include the supply tolerance and droop, or it is not slow enough.

    Interview

    Say that a droop costs more nanoseconds at low voltage mostly because the path is longer in ns, so the low-supply corner is the most voltage-critical in absolute terms.

    Check yourself Why is a 30 mV droop at 0.88 V cheaper in nanoseconds than at 0.72 V?

    The absolute delay-versus-voltage slope is smaller at high voltage (2.25 against 3.75 per volt in the example), and the base delay is smaller too, so the same voltage change moves delay less in ns. Fractionally the sensitivities are almost the same: about 2.9 per volt at 0.72 V against about 2.7 per volt at 0.88 V.

    Related topics

    • Library Sets

    • Next: RC Corner Mapping

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    See also

    • Temperature Inversion