{"abstract":"The adapter reports an incorrect observer arrival while other fields remain valid.","category":"Astronomical coordinate conventions","checks":6,"contract":"A supplied timing adapter has observer position r projected onto source direction n, speed c>0, Einstein delay E, Shapiro delay S, and geocenter projection g. Barycentric arrival is t+r*n/c+E+S. This model composes explicit corrections only and does not calculate ephemerides or relativistic delays. Output fields are defined by: roemer_delay = d['r']*d['n']/d['c']; arrival = d['t']+d['r']*d['n']/d['c']+d['E']+d['S']; topocentric_residual = (d['r']-d['g'])*d['n']/d['c']; geocentric_arrival = d['t']+d['g']*d['n']/d['c']+d['E']+d['S']; observer_arrival = d['t']-d['r']*d['n']/d['c']-d['E']-d['S']; geometric_rate = d['n']/d['c']","contract_signature":"d","evaluation_group":"astro-barycentric-arrival-corrections","failed_approach":"A partial convention repair still uses d['t']+d['r']*d['n']/d['c']-d['E']-d['S']","family":"s3-astronomical-coordinate-conventions-barycentric-arrival-corrections-observer_arrival","id":"FA-56001","implementations":{"attempt":{"sha256":"a558ec273eddb17636b9c8d57665ca7332f6042829c9033924c672a9ec694ef1","source":"\"\"\"Failure Map reference implementation. Python standard library only.\"\"\"\nimport json\n\nN = 1\nobservations = []\ndef solve(d):\n    return {'roemer_delay': d['r']*d['n']/d['c'], 'arrival': d['t']+d['r']*d['n']/d['c']+d['E']+d['S'], 'topocentric_residual': (d['r']-d['g'])*d['n']/d['c'], 'geocentric_arrival': d['t']+d['g']*d['n']/d['c']+d['E']+d['S'], 'observer_arrival': d['t']+d['r']*d['n']/d['c']-d['E']-d['S'], 'geometric_rate': d['n']/d['c']}\ndef check(label, actual, expected):\n    observations.append({\"check\": label, \"actual\": actual, \"expected\": expected, \"passed\": actual == expected})\nfixtures = {1: [({'t': 100, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 108.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 105.0, 'observer_arrival': 92.0, 'geometric_rate': 0.5}), ({'t': 100, 'r': 8, 'n': 0, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 0.0, 'arrival': 104.0, 'topocentric_residual': 0.0, 'geocentric_arrival': 104.0, 'observer_arrival': 96.0, 'geometric_rate': 0.0}), ({'t': 100, 'r': -4, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 102.0, 'topocentric_residual': -3.0, 'geocentric_arrival': 105.0, 'observer_arrival': 98.0, 'geometric_rate': 0.5}), ({'t': 100, 'r': 8, 'n': 2, 'c': 4, 'E': 0, 'S': 0, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 104.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 101.0, 'observer_arrival': 96.0, 'geometric_rate': 0.5}), ({'t': 100, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 0}, {'roemer_delay': 4.0, 'arrival': 108.0, 'topocentric_residual': 4.0, 'geocentric_arrival': 104.0, 'observer_arrival': 92.0, 'geometric_rate': 0.5}), ({'t': 100, 'r': 8, 'n': -1, 'c': 4, 'E': 3, 'S': -2, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 99.0, 'topocentric_residual': -1.5, 'geocentric_arrival': 100.5, 'observer_arrival': 101.0, 'geometric_rate': -0.25})], 2: [({'t': 101, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 109.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 106.0, 'observer_arrival': 93.0, 'geometric_rate': 0.5}), ({'t': 101, 'r': 8, 'n': 0, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 0.0, 'arrival': 105.0, 'topocentric_residual': 0.0, 'geocentric_arrival': 105.0, 'observer_arrival': 97.0, 'geometric_rate': 0.0}), ({'t': 101, 'r': -4, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 103.0, 'topocentric_residual': -3.0, 'geocentric_arrival': 106.0, 'observer_arrival': 99.0, 'geometric_rate': 0.5}), ({'t': 101, 'r': 8, 'n': 2, 'c': 4, 'E': 0, 'S': 0, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 105.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 102.0, 'observer_arrival': 97.0, 'geometric_rate': 0.5}), ({'t': 101, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 0}, {'roemer_delay': 4.0, 'arrival': 109.0, 'topocentric_residual': 4.0, 'geocentric_arrival': 105.0, 'observer_arrival': 93.0, 'geometric_rate': 0.5}), ({'t': 101, 'r': 8, 'n': -1, 'c': 4, 'E': 3, 'S': -2, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 100.0, 'topocentric_residual': -1.5, 'geocentric_arrival': 101.5, 'observer_arrival': 102.0, 'geometric_rate': -0.25})], 3: [({'t': 102, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 110.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 107.0, 'observer_arrival': 94.0, 'geometric_rate': 0.5}), ({'t': 102, 'r': 8, 'n': 0, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 0.0, 'arrival': 106.0, 'topocentric_residual': 0.0, 'geocentric_arrival': 106.0, 'observer_arrival': 98.0, 'geometric_rate': 0.0}), ({'t': 102, 'r': -4, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 104.0, 'topocentric_residual': -3.0, 'geocentric_arrival': 107.0, 'observer_arrival': 100.0, 'geometric_rate': 0.5}), ({'t': 102, 'r': 8, 'n': 2, 'c': 4, 'E': 0, 'S': 0, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 106.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 103.0, 'observer_arrival': 98.0, 'geometric_rate': 0.5}), ({'t': 102, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 0}, {'roemer_delay': 4.0, 'arrival': 110.0, 'topocentric_residual': 4.0, 'geocentric_arrival': 106.0, 'observer_arrival': 94.0, 'geometric_rate': 0.5}), ({'t': 102, 'r': 8, 'n': -1, 'c': 4, 'E': 3, 'S': -2, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 101.0, 'topocentric_residual': -1.5, 'geocentric_arrival': 102.5, 'observer_arrival': 103.0, 'geometric_rate': -0.25})], 4: [({'t': 103, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 111.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 108.0, 'observer_arrival': 95.0, 'geometric_rate': 0.5}), ({'t': 103, 'r': 8, 'n': 0, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 0.0, 'arrival': 107.0, 'topocentric_residual': 0.0, 'geocentric_arrival': 107.0, 'observer_arrival': 99.0, 'geometric_rate': 0.0}), ({'t': 103, 'r': -4, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 105.0, 'topocentric_residual': -3.0, 'geocentric_arrival': 108.0, 'observer_arrival': 101.0, 'geometric_rate': 0.5}), ({'t': 103, 'r': 8, 'n': 2, 'c': 4, 'E': 0, 'S': 0, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 107.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 104.0, 'observer_arrival': 99.0, 'geometric_rate': 0.5}), ({'t': 103, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 0}, {'roemer_delay': 4.0, 'arrival': 111.0, 'topocentric_residual': 4.0, 'geocentric_arrival': 107.0, 'observer_arrival': 95.0, 'geometric_rate': 0.5}), ({'t': 103, 'r': 8, 'n': -1, 'c': 4, 'E': 3, 'S': -2, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 102.0, 'topocentric_residual': -1.5, 'geocentric_arrival': 103.5, 'observer_arrival': 104.0, 'geometric_rate': -0.25})], 5: [({'t': 104, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 112.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 109.0, 'observer_arrival': 96.0, 'geometric_rate': 0.5}), ({'t': 104, 'r': 8, 'n': 0, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 0.0, 'arrival': 108.0, 'topocentric_residual': 0.0, 'geocentric_arrival': 108.0, 'observer_arrival': 100.0, 'geometric_rate': 0.0}), ({'t': 104, 'r': -4, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 106.0, 'topocentric_residual': -3.0, 'geocentric_arrival': 109.0, 'observer_arrival': 102.0, 'geometric_rate': 0.5}), ({'t': 104, 'r': 8, 'n': 2, 'c': 4, 'E': 0, 'S': 0, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 108.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 105.0, 'observer_arrival': 100.0, 'geometric_rate': 0.5}), ({'t': 104, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 0}, {'roemer_delay': 4.0, 'arrival': 112.0, 'topocentric_residual': 4.0, 'geocentric_arrival': 108.0, 'observer_arrival': 96.0, 'geometric_rate': 0.5}), ({'t': 104, 'r': 8, 'n': -1, 'c': 4, 'E': 3, 'S': -2, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 103.0, 'topocentric_residual': -1.5, 'geocentric_arrival': 104.5, 'observer_arrival': 105.0, 'geometric_rate': -0.25})]}\nfor i, (record, expected) in enumerate(fixtures[N]):\n    check('astronomical fixture %s' % i, solve(record), expected)\nprint(json.dumps({\"observations\": observations, \"passed\": all(x[\"passed\"] for x in observations)}, ensure_ascii=False))\nraise SystemExit(0 if all(x[\"passed\"] for x in observations) else 1)\n"},"broken":{"sha256":"825b4dc626d0147b274d67508d9ac3d3650f696e8f3361ed358dfabf89af6fcc","source":"\"\"\"Failure Map reference implementation. Python standard library only.\"\"\"\nimport json\n\nN = 1\nobservations = []\ndef solve(d):\n    return {'roemer_delay': d['r']*d['n']/d['c'], 'arrival': d['t']+d['r']*d['n']/d['c']+d['E']+d['S'], 'topocentric_residual': (d['r']-d['g'])*d['n']/d['c'], 'geocentric_arrival': d['t']+d['g']*d['n']/d['c']+d['E']+d['S'], 'observer_arrival': d['t']-d['r']*d['n']/d['c'], 'geometric_rate': d['n']/d['c']}\ndef check(label, actual, expected):\n    observations.append({\"check\": label, \"actual\": actual, \"expected\": expected, \"passed\": actual == expected})\nfixtures = {1: [({'t': 100, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 108.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 105.0, 'observer_arrival': 92.0, 'geometric_rate': 0.5}), ({'t': 100, 'r': 8, 'n': 0, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 0.0, 'arrival': 104.0, 'topocentric_residual': 0.0, 'geocentric_arrival': 104.0, 'observer_arrival': 96.0, 'geometric_rate': 0.0}), ({'t': 100, 'r': -4, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 102.0, 'topocentric_residual': -3.0, 'geocentric_arrival': 105.0, 'observer_arrival': 98.0, 'geometric_rate': 0.5}), ({'t': 100, 'r': 8, 'n': 2, 'c': 4, 'E': 0, 'S': 0, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 104.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 101.0, 'observer_arrival': 96.0, 'geometric_rate': 0.5}), ({'t': 100, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 0}, {'roemer_delay': 4.0, 'arrival': 108.0, 'topocentric_residual': 4.0, 'geocentric_arrival': 104.0, 'observer_arrival': 92.0, 'geometric_rate': 0.5}), ({'t': 100, 'r': 8, 'n': -1, 'c': 4, 'E': 3, 'S': -2, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 99.0, 'topocentric_residual': -1.5, 'geocentric_arrival': 100.5, 'observer_arrival': 101.0, 'geometric_rate': -0.25})], 2: [({'t': 101, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 109.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 106.0, 'observer_arrival': 93.0, 'geometric_rate': 0.5}), ({'t': 101, 'r': 8, 'n': 0, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 0.0, 'arrival': 105.0, 'topocentric_residual': 0.0, 'geocentric_arrival': 105.0, 'observer_arrival': 97.0, 'geometric_rate': 0.0}), ({'t': 101, 'r': -4, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 103.0, 'topocentric_residual': -3.0, 'geocentric_arrival': 106.0, 'observer_arrival': 99.0, 'geometric_rate': 0.5}), ({'t': 101, 'r': 8, 'n': 2, 'c': 4, 'E': 0, 'S': 0, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 105.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 102.0, 'observer_arrival': 97.0, 'geometric_rate': 0.5}), ({'t': 101, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 0}, {'roemer_delay': 4.0, 'arrival': 109.0, 'topocentric_residual': 4.0, 'geocentric_arrival': 105.0, 'observer_arrival': 93.0, 'geometric_rate': 0.5}), ({'t': 101, 'r': 8, 'n': -1, 'c': 4, 'E': 3, 'S': -2, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 100.0, 'topocentric_residual': -1.5, 'geocentric_arrival': 101.5, 'observer_arrival': 102.0, 'geometric_rate': -0.25})], 3: [({'t': 102, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 110.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 107.0, 'observer_arrival': 94.0, 'geometric_rate': 0.5}), ({'t': 102, 'r': 8, 'n': 0, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 0.0, 'arrival': 106.0, 'topocentric_residual': 0.0, 'geocentric_arrival': 106.0, 'observer_arrival': 98.0, 'geometric_rate': 0.0}), ({'t': 102, 'r': -4, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 104.0, 'topocentric_residual': -3.0, 'geocentric_arrival': 107.0, 'observer_arrival': 100.0, 'geometric_rate': 0.5}), ({'t': 102, 'r': 8, 'n': 2, 'c': 4, 'E': 0, 'S': 0, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 106.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 103.0, 'observer_arrival': 98.0, 'geometric_rate': 0.5}), ({'t': 102, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 0}, {'roemer_delay': 4.0, 'arrival': 110.0, 'topocentric_residual': 4.0, 'geocentric_arrival': 106.0, 'observer_arrival': 94.0, 'geometric_rate': 0.5}), ({'t': 102, 'r': 8, 'n': -1, 'c': 4, 'E': 3, 'S': -2, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 101.0, 'topocentric_residual': -1.5, 'geocentric_arrival': 102.5, 'observer_arrival': 103.0, 'geometric_rate': -0.25})], 4: [({'t': 103, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 111.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 108.0, 'observer_arrival': 95.0, 'geometric_rate': 0.5}), ({'t': 103, 'r': 8, 'n': 0, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 0.0, 'arrival': 107.0, 'topocentric_residual': 0.0, 'geocentric_arrival': 107.0, 'observer_arrival': 99.0, 'geometric_rate': 0.0}), ({'t': 103, 'r': -4, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 105.0, 'topocentric_residual': -3.0, 'geocentric_arrival': 108.0, 'observer_arrival': 101.0, 'geometric_rate': 0.5}), ({'t': 103, 'r': 8, 'n': 2, 'c': 4, 'E': 0, 'S': 0, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 107.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 104.0, 'observer_arrival': 99.0, 'geometric_rate': 0.5}), ({'t': 103, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 0}, {'roemer_delay': 4.0, 'arrival': 111.0, 'topocentric_residual': 4.0, 'geocentric_arrival': 107.0, 'observer_arrival': 95.0, 'geometric_rate': 0.5}), ({'t': 103, 'r': 8, 'n': -1, 'c': 4, 'E': 3, 'S': -2, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 102.0, 'topocentric_residual': -1.5, 'geocentric_arrival': 103.5, 'observer_arrival': 104.0, 'geometric_rate': -0.25})], 5: [({'t': 104, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 112.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 109.0, 'observer_arrival': 96.0, 'geometric_rate': 0.5}), ({'t': 104, 'r': 8, 'n': 0, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': 0.0, 'arrival': 108.0, 'topocentric_residual': 0.0, 'geocentric_arrival': 108.0, 'observer_arrival': 100.0, 'geometric_rate': 0.0}), ({'t': 104, 'r': -4, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 106.0, 'topocentric_residual': -3.0, 'geocentric_arrival': 109.0, 'observer_arrival': 102.0, 'geometric_rate': 0.5}), ({'t': 104, 'r': 8, 'n': 2, 'c': 4, 'E': 0, 'S': 0, 'g': 2}, {'roemer_delay': 4.0, 'arrival': 108.0, 'topocentric_residual': 3.0, 'geocentric_arrival': 105.0, 'observer_arrival': 100.0, 'geometric_rate': 0.5}), ({'t': 104, 'r': 8, 'n': 2, 'c': 4, 'E': 3, 'S': 1, 'g': 0}, {'roemer_delay': 4.0, 'arrival': 112.0, 'topocentric_residual': 4.0, 'geocentric_arrival': 108.0, 'observer_arrival': 96.0, 'geometric_rate': 0.5}), ({'t': 104, 'r': 8, 'n': -1, 'c': 4, 'E': 3, 'S': -2, 'g': 2}, {'roemer_delay': -2.0, 'arrival': 103.0, 'topocentric_residual': -1.5, 'geocentric_arrival': 104.5, 'observer_arrival': 105.0, 'geometric_rate': -0.25})]}\nfor i, (record, expected) in enumerate(fixtures[N]):\n    check('astronomical fixture %s' % i, solve(record), expected)\nprint(json.dumps({\"observations\": observations, \"passed\": all(x[\"passed\"] for x in observations)}, ensure_ascii=False))\nraise SystemExit(0 if all(x[\"passed\"] for x in observations) else 1)\n"}},"limitations":"Explicitly stipulated finite algebraic adapter; no standards conformance, physical accuracy, or production-library claim. Inputs are the documented finite valid model domain. This reproducer isolates one failure mechanism. Results cover the supplied fixtures. Variants within a family share a test contract and should remain grouped when constructing evaluation splits. Related mechanisms with a shared evaluation_group must also remain together; these controlled models are not independent production incidents.","method":"Deterministic executable model with adversarial boundary fixtures.","provenance":{"created_by":"Failure Map","dependencies":"Python standard library","family":"s3-astronomical-coordinate-conventions-barycentric-arrival-corrections-observer_arrival","generated_at":"2026-09-29T14:46:03.074236+00:00","license":"CC0-1.0","python":"3.12.14","seed":1,"split":"open-access"},"relevance":"Catalog, detector, sky-coordinate, and spectroscopy adapters must preserve the association between numeric coordinates and their declared reference conventions.","root_cause":"Inverse arrival-time adapter removes only geometric delay. Faulty expression: d['t']-d['r']*d['n']/d['c']","sha256":"11c90a3b30585ee4ebb3afbd81449eb59a29cb7891b9bd531b7dde7e42aef7b7","title":"Barycentric arrival corrections: Inverse arrival-time adapter removes only geometric delay · case 01","variant":1,"variant_policy":"Five numbered records share a model and may reuse boundary fixtures.","verified":true,"visibility":"public","verification":{"attempt":{"elapsed_ms":43.088,"exit_code":1,"observations":[{"actual":{"arrival":108.0,"geocentric_arrival":105.0,"geometric_rate":0.5,"observer_arrival":100.0,"roemer_delay":4.0,"topocentric_residual":3.0},"check":"astronomical fixture 0","expected":{"arrival":108.0,"geocentric_arrival":105.0,"geometric_rate":0.5,"observer_arrival":92.0,"roemer_delay":4.0,"topocentric_residual":3.0},"passed":false},{"actual":{"arrival":104.0,"geocentric_arrival":104.0,"geometric_rate":0.0,"observer_arrival":96.0,"roemer_delay":0.0,"topocentric_residual":0.0},"check":"astronomical fixture 1","expected":{"arrival":104.0,"geocentric_arrival":104.0,"geometric_rate":0.0,"observer_arrival":96.0,"roemer_delay":0.0,"topocentric_residual":0.0},"passed":true},{"actual":{"arrival":102.0,"geocentric_arrival":105.0,"geometric_rate":0.5,"observer_arrival":94.0,"roemer_delay":-2.0,"topocentric_residual":-3.0},"check":"astronomical fixture 2","expected":{"arrival":102.0,"geocentric_arrival":105.0,"geometric_rate":0.5,"observer_arrival":98.0,"roemer_delay":-2.0,"topocentric_residual":-3.0},"passed":false},{"actual":{"arrival":104.0,"geocentric_arrival":101.0,"geometric_rate":0.5,"observer_arrival":104.0,"roemer_delay":4.0,"topocentric_residual":3.0},"check":"astronomical fixture 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