PIP

DMT PIP. Same probetype, reader and timing family as the CIP, four times coarser. Runs under both UIOOPS engines and the SODA-2 port's DMT path.

The instrument, as the code sees it

Every row below is read from constants.IMGPROC_CONFIG, the port of imgProc_sm.m's own probe switch. None of it is typed into this page.

probetype1
diodes64
diode resolution (ds)100 um
array reach6.4 mm (64 x 100 um)
timing familydmt
needs a TAS fileno
Stage-2 readerarrayprobe.readers.dmt.read_binary_DMT
image word8-bit, not inverted

What runs today

Imported from the coverage matrix rather than restated, so this table and docs/developer/COVERAGE_MATRIX.md cannot disagree.

Engineserial–chunks–jobs–s2-jobs–jit
arrayprobe_uiopsCROSS-CHECKEDCROSS-CHECKEDCROSS-CHECKEDCROSS-CHECKEDCROSS-CHECKED
arrayprobe_soda2CROSS-CHECKEDCROSS-CHECKEDCROSS-CHECKEDuntestedCROSS-CHECKED

How to read this table.

No shipped preset names this probe. A run needs a campaign preset declared in your own TOML ([run].presets), and [run].preset is required – it has no default.

Where a cell above reads refuses (by design) or REFUSES (DEFECT), the reason is in docs/developer/COVERAGE_MATRIX.md for that exact cell. A refusal here is always preferred to a silently wrong fast answer, and the two words are different: by design means the combination is meaningless, defect means it should work and does not yet.

Caveats

Consequences of this probe's own geometry

Computed from the table above, not recalled – each says which arithmetic produced it.

The hollow test only packs diodes 1-32, and this array has 64

calculate_reject_unified.m:465 packs diodes 1-32 whatever the probe's width. This probe is 64 diodes wide, so a particle imaged entirely beyond diode 32 gives the test two zero operands and is ruled hollow on no evidence. That verdict reaches auto_reject AND the Korolev correction, so it moves both acceptance and recorded size. Preserved deliberately; wide_hollow_fix in enhancements_uiops/ is the opt-in, default-off alternative, and v3.5's own rewrite is a DIFFERENT correction from ours (it also drops the middle-third scan restriction – 745 of 1,080 random particles disagree).

Computed from: constants.IMGPROC_CONFIG['PIP'].diodenum = 64

The array images 6.4 mm, and a size ladder must respect that

64 diodes at 0.1 mm is 6.4 mm across. That is not a hard ceiling on recorded size, and it would be an overclaim to say so: a particle that merely has its centre in the array (sa_method 0) or is sized through the Heymsfield & Parrish reconstruction (sa_method 2) can be recorded LARGER than the array it crossed. The bound that survives is a factor, not an equality – a centre-in particle reaches about twice the array width, not twenty times it. So the honest reading is: a bin above roughly 12.8 mm on this probe is beyond what any sizing convention here produces, and a ladder whose top lies there is a configuration error rather than a sparse flight. The upstream finding that the default 2D-S bin table became the HVPS one (recorded in the review of the upstream code) is exactly that: a 30 mm ladder handed to a 1.28 mm array, 23x its width, and the symptom was a well-formed file with almost nothing in it.

Computed from: constants.IMGPROC_CONFIG['PIP']: diodenum 64 x ds 0.1 mm = 6.4 mm

Chunked stage 3: supported

Timing family dmt is in CHUNKABLE_TIMINGS_V35, so --chunks splits stage 3 with no carried state and the result is byte-identical to a serial run.

Computed from: constants.IMGPROC_CONFIG['PIP'].timing = 'dmt'; CHUNKABLE_TIMINGS_V35 = ('dmt', 'pms', 'fast2dc'); PRIMABLE_TIMINGS_V35 = ('spec',)

What a person knows and a constant does not

Curated in probe_caveats.json (in scripts/). Every citation is re-checked against the real file each time this page is generated.

The SODA-2 engine reads the PIP through its DMT path, checked on a synthetic file only

PIP data arrive in DMT (PADS/PACS) format; SODA-2 rewrites probetype PIP to CIP (soda2_update_op.pro:49) and the port follows it, matching the original under GDL bit for bit on a synthetic 12-record fixture. No real PIP recording has been run through it here.

Source: docs/developer/COVERAGE_MATRIX.md

Reject code 't' is never emitted, on any probe

calculate_reject_unified.m:269 rejects on the tighter threshold (max_comp_img_ar) before :272 tests the looser one (max_edge_img_ar), so the second branch is unreachable and image_auto_reject never contains 116. The netCDF Description attribute at imgProc_sm.m:325-329 states the two thresholds the other way round. Both are preserved verbatim – this is a faithfully reproduced upstream defect, not a port bug. If you are tabulating reject codes, 't' is structurally absent rather than merely rare.

Trust the .call sidecar, not the filename

Every stage stamps its configuration into a .call sidecar and refuses an input that disagrees or carries no stamp. If you write products with your own script instead of arrayprobe run, you inherit this problem.

Ratios this probe appears in

None. No ratio measured so far has this probe on either side – which follows from the data held: a ratio needs two chains over the same raw, and there is no raw here to run two chains over.

Where to go next

Every probe x engine x mode cell, with its reasondocs/developer/COVERAGE_MATRIX.md
Which engine to usedocs/developer/TWO_ENGINES.md
The airspeed chain, which sets the sample volumedocs/developer/TAS.md
How the upstream code was reviewed, and what was founddocs/developer/UPSTREAM_REVIEW.md
All seven probes at a glanceThe seven probes

Generated, not hand-maintained, from arrayprobe.constants.IMGPROC_CONFIG, coverage_matrix.build_matrix() and the curated caveats in probe_caveats.json.