#################### PYOTE 5.1.0  session started: Sat Apr 13 16:50:03 2024  ####################

filename: E:\ASTRONOMIA\1-Immagini CCD\Occultazioni\2024_04_12_(4446) Carolyn\Capture 2024-04-12T03_42_56Z\CarolynWithPymovie.csv

If the csv file came from PyMovie - columns with prefix: signal will be read.

==================== file header lines ====================
# PyMovie Version 4.0.5
# source: E:\ASTRONOMIA\1-Immagini CCD\Occultazioni\2024_04_12_(4446) Carolyn\Capture 2024-04-12T03_42_56Z.adv
#
# Aperture photometry was used to extract the lightcurves
#
# lunar background: False
# yellow mask = default: False
#
# aperture name: target
# ____ aperture size: 31
# ____ x,y: (167, 118) at frame 820
# ____ threshold: 1458
# ____ def mask radius: 3.2
# ____ color: green
# ____ joggable: False
# ____ auto textOut: False
# ____ thumbnail source: False
# ____ csv output order: 0
#
# aperture name: reference
# ____ aperture size: 31
# ____ x,y: (278, 275) at frame 820
# ____ threshold: 1489
# ____ def mask radius: 3.2
# ____ color: yellow
# ____ joggable: True
# ____ auto textOut: False
# ____ thumbnail source: False
# ____ csv output order: 1
#
# date at frame 0: 2024-04-12
#ADV-VERSION: 2
#ADVLIB-VERSION: 2.0
#ALTITUDE: 0
#BINNING-X: 2
#BINNING-Y: 2
#BITPIX: 16
#CAMERA-MODEL: QHY174M
#CAMERA-SENSOR-INFO: ADC bit depth : 12
#EFFECTIVE-PIXEL-SIZE-X: 11.720000267028809
#EFFECTIVE-PIXEL-SIZE-Y: 11.720000267028809
#FSTF-TYPE: ADV
#HEIGHT: 300
#LATITUDE: 46.23143816666666
#LONGITUDE: 9.024051666666667
#POSITION-REFERENCE: WGS84
#RECORDER-SOFTWARE: SharpCap
#RECORDER-SOFTWARE-VERSION: 4.1.11351.0
#WIDTH: 480
#
# Aperture photometry was used to extract the lightcurves
==================== end header lines ====================

At reading 00305: time delta to next reading = 0.6003 : likely 1 dropped readings
At reading 00639: time delta to next reading = 0.6003 : likely 1 dropped readings

========== Total dropped readings..... 2
========== Num duplicated readings.... 0
========== Number timestamp errors.... 0
========== Number of cadence errors... 2

timeDelta: 0.300144 seconds per reading
timestamp error rate: 0.244%

Home directory: C:\Users\stefa\AppData\Local\Packages\PythonSoftwareFoundation.Python.3.10_qbz5n2kfra8p0\LocalCache\local-packages\Python310\site-packages\pyoteapp

We found C:\Users\stefa\Documents\model-examples already present. Adding any new examples ...
Use min/max event to locate a "D and R" event has been selected

minEvent: 2  maxEvent: 9

Number of candidate solutions: 6516 (using event min/max entries)

New solver results...

Integer (non-subframe) solution...
sigB:14112.20  sigA:15652.58 B:63734.56 A:10719.00
in entryNum units: D: 458  R: 463

noise corr coefs: [1.00, 0.0873, 0.103, 0.0560, 0.0516]  (based on 816 points)  sigmaB: 12456.43

Subframe adjusted solution...
sigB:14112.20  sigA:11796.36 B:63734.56 A:4938.00
in entryNum units: D: 458  R: 462  D(subframe): 458.0000  R(subframe): 462.5638

in frameNum units: D: 458  R: 462  D(subframe): 458.0000  R(subframe): 462.5638

... end New solver results

Error bar report based on 100,000 simulations (units are readings)...

loDbar   @ .68 ci:  -0.2422
hiDbar   @ .68 ci:   0.2534
loDbar   @ .95 ci:  -0.6320
hiDbar   @ .95 ci:   0.5966
loDbar   @ .9973 ci:  -1.2993
hiDbar   @ .9973 ci:   1.2508

loDurBar @ .68 ci:  -0.3820
hiDurBar @ .68 ci:   0.3722
loDurBar @ .95 ci:  -0.8597
hiDurBar @ .95 ci:   0.8515
loDurBar @ .9973 ci:  -1.7845
hiDurBar @ .9973 ci:   1.6230

Timestamp validity check ...

From timestamps at D and R, calculated 4 reading blocks.  From reading blocks, calculated 4 blocks.

Timestamps appear valid @ D and R

================= 0.68 containment interval report =================

B: 63734.56  {+/- 494.20}  sigmaB: 14112.20

A: 4938.00  {+/- 6248.72}  sigmaA: 11796.36

magDrop report: percentDrop: 92.3  magDrop: 2.777  +/- 1.374  (0.68 ci)

snr: 4.17

D: 458.00 {+0.25,-0.25} (frame number)
D: [03:45:13.6892]  {+0.0744,-0.0744} seconds

R: 462.56 {+0.25,-0.25} (frame number)
R: [03:45:15.0590]  {+0.0744,-0.0744} seconds

Duration (R - D): 4.5638 {+0.3771,-0.3771} readings
Duration (R - D): 1.3698 {+0.1132,-0.1132} seconds

=============== end 0.68 containment interval report ===============

================= 0.95 containment interval report =================

B: 63734.56  {+/- 988.39}  sigmaB: 14112.20

A: 4938.00  {+/- 12497.45}  sigmaA: 11796.36

magDrop report: percentDrop: 92.3  magDrop: 2.777  +/- 2.748  (0.95 ci)

snr: 4.17

D: 458.00 {+0.61,-0.61} (frame number)
D: [03:45:13.6892]  {+0.1844,-0.1844} seconds

R: 462.56 {+0.61,-0.61} (frame number)
R: [03:45:15.0590]  {+0.1844,-0.1844} seconds

Duration (R - D): 4.5638 {+0.8556,-0.8556} readings
Duration (R - D): 1.3698 {+0.2568,-0.2568} seconds

=============== end 0.95 containment interval report ===============

================= 0.9973 containment interval report ===============

B: 63734.56  {+/- 1482.59}  sigmaB: 14112.20

A: 4938.00  {+/- 18746.17}  sigmaA: 11796.36

magDrop report: percentDrop: 92.3  magDrop: 2.777  too much noise; cannot calculate error bars

snr: 4.17

D: 458.00 {+1.28,-1.28} (frame number)
D: [03:45:13.6892]  {+0.3827,-0.3827} seconds

R: 462.56 {+1.28,-1.28} (frame number)
R: [03:45:15.0590]  {+0.3827,-0.3827} seconds

Duration (R - D): 4.5638 {+1.7038,-1.7038} readings
Duration (R - D): 1.3698 {+0.5114,-0.5114} seconds

=============== end 0.9973 containment interval report =============

D frame number: 458.00
D: 0.6800 containment intervals:  {+/- 0.25} (readings)
D: 0.9500 containment intervals:  {+/- 0.63} (readings)
D: 0.9973 containment intervals:  {+/- 1.30} (readings)

R frame number: 462.56
R: 0.6800 containment intervals:  {+/- 0.25} (readings)
R: 0.9500 containment intervals:  {+/- 0.63} (readings)
R: 0.9973 containment intervals:  {+/- 1.30} (readings)

Duration (R - D): 4.5638 readings
Duration: 0.6800 containment intervals:  {+/- 0.3771} (readings)
Duration: 0.9500 containment intervals:  {+/- 0.8556} (readings)
Duration: 0.9973 containment intervals:  {+/- 1.7038} (readings)

=============== Summary report for Excel file =====================

This light curve has not been block integrated.


This 'drop' has a zero probability of being an artifact of noise.
>>>> probability > 0.0000 indicates the 'drop' may be spurious (a noise artifact). Consult with an IOTA Regional Coordinator.
>>>> probability = 0.0000 indicates the 'drop' is unlikely to be a noise artifact, but does not prove that the 'drop' is due to an occultation
>>>> Consider 'drop' shape, timing, mag drop, duration and other positive observer chords before reporting the 'drop' as a positive.

All times are calculated/reported based on the assumption that timestamps are start-of-exposure times.

It is critical that you make appropriate time adjustments when timestamps are NOT start-of-exposure times.
If you use the North American Excel Spreadsheet report, all times will be properly corrected
for camera delay and reported start-of-exposure times.
For other users worldwide, use the appropriate corrections documented in the North American Spreadsheet report form - use
the documentation shown on the Corrections Tables tab.

magDrop report: percentDrop: 92.3  magDrop: 2.777  +/- 2.748  (0.95 ci)

snr: 4.17

D time: [03:45:13.6892]
D: 0.6800 containment intervals:  {+/- 0.0744} seconds
D: 0.9500 containment intervals:  {+/- 0.1844} seconds
D: 0.9973 containment intervals:  {+/- 0.3827} seconds

R time: [03:45:15.0590]
R: 0.6800 containment intervals:  {+/- 0.0744} seconds
R: 0.9500 containment intervals:  {+/- 0.1844} seconds
R: 0.9973 containment intervals:  {+/- 0.3827} seconds

Duration (R - D): 1.3698 seconds
Duration: 0.6800 containment intervals:  {+/- 0.1132} seconds
Duration: 0.9500 containment intervals:  {+/- 0.2568} seconds
Duration: 0.9973 containment intervals:  {+/- 0.5114} seconds

Enter D and R error bars for each containment interval in Excel spreadsheet without + or - sign (assumed to be +/-)

=========== end Summary report for Excel file =====================

Solution 'envelope' in the main plot drawn using 0.95 containment interval error bars



#################### Session ended: Sat Apr 13 16:52:26 2024  ####################