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Daily Reports (2026/10/6-13, NIKA2 run 81, Cryo run 93)

Observers on-site: Rémi, Giorgos, Mairi, Miren

AoD: Ioannis

Operators: Pedro, Sergio

Important

Focus offsets shall be measured on Ar1
Pointing offsets shall be measured on Ar2

Pool-Account usage: Accounting of observing times

Book-keeping of important scans

We ask you to please keep track of focus sequences (as much as possible), beam maps (always), and changes of sweep (until the new sweep DAFs are permanently installed). Thanks

Focus sequences

Please fill the Table with the Ar1,2,3 focus values as follows. At best, make one table per day.

Beam maps

Similarly, if any beam maps (total power) are taken:

Changes in sweep

Please keep track of sweep changes: it makes our life easier when building the DAFs/Kidpars.

October 6th, 2026, Tuesday

10:30-15:30 : 3/4 observers arrived at the telescope. Rémi planned to arrive later today. Weather horrible. Maintenance ongoing.

Antenna parked all day, clouds, wind, and rain.

October 7th, 2026, Wednesday

07:00LT: pointing and focus tests with old sweep (run92). Difference between Ar2 and Ar1 ~0.35 mm. Difference between Ar3 and Ar1 practically 0.

10:00 - 11:30LT: new sweep by M. Calvo. We now have new run93.ini files.

11:45LT Miren and Ioanns : starting NIKA2 observations to get beammaps for the new sweep. Back to run92 for pointing and focus on Mars. DAQ started, lost KIDs Ar1/Ar2/Ar3: 129/6/14; traces look fine. Opacity between 0.3 - 0.5. Peak-to-peak in Ar2 +/- 4-5 Jy/beam. Focus differences: Ar1 - Ar2 = -0.14 mm, Ar1 - Ar3 = 0.01 mm.

12:45LT: moving to run93 for beammaps. Lost KIDs Ar1/Ar2/Ar3: 21/8/30. To be understood if box I is lost or not. Beammap (20261007s30) focused on Ar1.

13h25LT: back to run92 for pointing and focus before another beammap. Lost KIDs Ar1/Ar2/Ar3: 140/7/15. Moving back to run93 for beammaps. Beammap (20261007s39) focused on Ar1.

14h30LT Miren and Mairi: focus tests with run92. Using the original focus script (with 0.4 mm step) starting from scan 20261007s80.

16h55LT: we try a mini pointing session making use of the sources in the PCCS catalogue provided by S. Berta (we have had to remove the "G" from the names in the end... 13 characters otherwise...) Opacity is ~ 0.35 (tau225 GHz), but a lot of clouds. We can not point, p2p fluctuations @Ar2 of +/- 20 Jy/beam.

19h00LT: We resume. Sky is stable (<5 Jy/beam) and tau around 0.3.

Summary:

Scan

Source

Azimuth

Elevation

tau_225GHz

Azimuth Corr.

Elevation Corr.

91

034.61+11.84

164

59

0.3

-5

-5

92

039.53+28.08

202

69

0.28

-3

-6

94

022.98+42.17

232

53

0.28

-3

-7

96

1641+399

285

71

0.28

-5

-8

104

039.28+62.77

274

43

0.26

-2.5

-7

109

1641+399

287

60

0.28

-4.5

-9

141

071.50+55.61

305

28

0.24

-2

-4.2

143

133.77+42.32

351

21

0.26

-0.5

-5

145

141.27+25.05

372

24

0.27

0

-2

147

W3OH

396

41

0.26

-2.8

-4.2

154

121.67-05.69

400

57

0.26

-6

-4

157

112.91-09.88

401

68

0.26

-6.5

-3

159

098.48-15.81

402

84

0.27

-8.7

-1

161

2200+420

307

81

0.24

-3

-4.3

Average

??

??

??

SD

??

??

??

October 8th, 2026, Thursday

00:30LT Miren: Stable (=/-2 Jy/beam) and good opacity (~ 0.25). Better beammaps are needed. We move to 0316+413 for first beammaps, waiting Uranus to be high.

01:00 - 07:00 LT, Rémi : stable weather, clear sky and opacity ~ 0.25 for the entire shift.

07:00 - 13:00 LT, Giorgos :

13:00 - 19:00 LT, Mairi : Taking over shift from Giorgos. Continuing test scans for project 092-26. One repetition completed (s112 and 113). Unstable sky (+/-10Jy/beam), waiting to see if improves before continuing.

18:00 LT, SB. I've been processing the beam maps taken during the last night/morning with good weather and on Uranus and 0316+413. The result is good for Ar1. Ar3 is still downloading and I will then process it later tonight. And about Ar2... oh well, the beam is confirmed to be very elongated, even when supposedly "on focus". The position angle (PA) of the beam ellipse is rotating in AzEl, I guess as a function of Elevation. To give you an idea, here I include the sequence of Ar2 beam maps f.o.v., in the hope that this will help the instrument/hardware experts to figure out what is happening.

Ar2 f.o.v. of beam map 20261008s23 on Uranus Ar2 f.o.v. of beam map 20261008s38 on Uranus Ar2 f.o.v. of beam map 20261008s52 on Uranus Ar2 f.o.v. of beam map 20261008s63 on Uranus Ar2 f.o.v. of beam map 20261008s90 on Uranus Ar2 f.o.v. of beam map 20261008s98 on Uranus

CK: Beam are elongated in the central region and by ~90deg with elevation/PA. However, beams are about circular in the region around -150”/0”. Is the 2mm array offset relative to the radio axis ?

CK: As Array 2 was moved by 17mm, is it possible that Array 2 is now very far out of focus ? SB: yes I had this thought as well. It will be tested tonight

19:00 - 01:00 LT, Ioannis :

Extended focus test procedure:

Extended focus test after the new DAFs installation

23:00 LT, SB: the new NKFR and RPP DAFs for the new sweep are now installed and running at Pico. They are still preliminary (based on one scan only), but they're fine. From now on, we are not going to use the old sweep anymore. And from now on, the run number is N2R81 and cryo run 93. The first scan (permanently) obtained with the new sweep is 20261008s176. Below here comes the f.o.v. of the adopted beam maps used for the these N2R81 RPPs. Good night :-)

Ar2 f.o.v. of beam map 20261008s52 on Uranus Ar1 f.o.v. of beam map 20261008s90 on Uranus Ar3 f.o.v. of beam map 20261008s90 on Uranus

October 9th, 2026, Friday

01:00 - 07:00 LT, Rémi : opacity is very good over the shift, ~0.15. The stability is great. Some (relatively low) wind.

SB: the pointing must always be set on Ar2, no matter what focus is used for the beam maps (Ar1 or Ar2), because Ar2 is the only one with one KID exactly on the optical axis of the telescope+NIKA2 system. Please re-check what pointing has been used for these last beam maps. If it was Ar1, then they are not usable. Cfr. the notes in previous night/morning. [IM: Yes, we discussed this with Rémi and the plan was to always point on Ar2 last night. He can also confirm, if needed.]

Scan

Source

Azimuth

Elevation

tau_225GHz

Azimuth Corr.

Elevation Corr.

20261009s62

174.84+210.10

64.09

75.18

0.12

-12

-9.1

20261009s64

180.98+50.26

66.9

45.78

0.12

-5.5

-9.6

20261009s65

218.16+69.96

76.17

21.58

0.12

1.2

-9.6

20261009s66

243.98+08.93

146.34

22.51

0.11

2.2

-7.5

20261009s67

211.30+19.04

133.68

54.59

0.12

-4.8

-9.7

20261009s68

179.93+09.14

175.69

86.35

0.12

-8.4

-6.4

20261009s69

228.62-13.65

179.75

33

0.11

0.7

-6.8

20261009s71

184.72-12.78

231.47

62.88

0.12

-5.9

-11

20261009s73

169.15-39.71

255.82

34.38

0.12

0

-10.4

20261009s74

128.18-3052

294.27

22.62

0.11

2.5

-10.6

20261009s75

163.69+09.00

312.28

72.36

0.13

-6.3

-12.6

20261009s76

121.67-05.69

322.73

27.52

0.12

2.1

-9.8

20261009s77

146.02+11.93

332.32

55.87

0.10

-4.1

-12.8

20261009s78

174.84+20.10

331.47

84.7

0.12

-7.2

-10.7

20261009s79

120.90+19.21

351.16

33.70

0.11

0.

-10.6

20261009s80

164.20+30.52

369.31

72.94

0.13

-8.3

-11.2

20261009s81

145.73+43.13

384.27

55.38

0.13

-6.5

-11.4

20261009s89

217.62+02.74

205.00

47.08

0.15

-3.4

-8.8

20261009s91

211.56+60.99

104.3

58.05

0.13

-7.2

-9.7

20261009s93

198.86+44.39

125.52

75.91

0.14

-10

-7.1

CK: At 2mm, is it possible that we are finding only a secondary maximum showing an elongated beam due to some astigmatism ? Do we need to scan the z-focus over a much wider range to find the main maximum, where the beam is 18" and circular ?

IM: I could run an even extended focus sequence for this but not sure of the system limitations (e.g. PaKo focus limits etc). I'll try to find out. CK: let's first discuss with the experts.

SB: at this point I do not think that's possible. Ioannis tested this, with a very broad focus range of +/- 2.4 mm centered on the Ar1 focus (see the PDF he produced and that is attached above). I might be wrong, but such a double peaked focus "variety" (mathematical entity) seems hard to understand to me. If you check the f.o.v. figure of Ar2 above (23:00 LT, yesterday), to me it seems that the "circular" beam is simply not in the center of the array, but it is on the left of the f.o.v. (e.g. Ar2 KID nr 440 in the figure). This tells me that some optical element is not well centered or well aligned. Two things have been "touched" in the last intervention: the dichroic and Ar2. Since there's not such an effect on Ar1 or Ar3, my guess is that it's not a dichroic issue, but rather the shims insterted below Ar2 might not be perfectly planar (e.g. they're thicker on one side that on the other). Or something happened to the Ar2 support in general. Does it make sense?

07:00 - 13:00 LT, Giorgos : Finished pointing session. Switched to polarization. Started project 090-26, 2 reps. Source 236.60+38.70 -> very weak.

IM: We tested the Planck catalog for both pointing sessions so far. Many of the targets are bright and therefore suitable for pointing calibrators. But it seems that there are several faint sources that are marginally good for pointing sources and only if the "f" option of the pointing script is used. In particular, source 236.60+38.70 reported above by Giorgos was not detected at all with a pointing. I think there should be some additional filtering of the Planck catalog, maybe based on NIKA2 observations.

CK: 236.60+38.70 is listed with 120mJy @ 1mm in Planck catalog. Obviously, we should exclude weak sources and sources which are extended relative to the 30m beam from a Planck-based pointing catalog.

---

SL: Replies to several of the observations, comments and question above.

- The 20"x25" beam mentioned by Rémi is extremely elliptic. But in the series of focus sequences, the best compromise beam is clearly much less elliptic than that, or even not at all. So I suppose the best compromise beam should be less or equal to 20" diameter circle.

- More precisely, about elongated beams at 2mm (Ar2), sizes, peak intensity, possible secondary maximum. The beam shape evolution on focus sequences show clearly an effect of astigmatism caused by an optical element which doesn't have a shape symmetric by revolution around its vertex, but has a 2 axes of symmetry. This is very well visible on the series of 3 focus sequences displayed above. Before the optimal "best compromise" focus, the beam is very elongated in one direction, and at some point at best focus for the perpendicular direction. Then it continues to improve in the 1st direction and starts slowly to degrade in the perpendicular direction. Then we reach the best compromise: circular (squarish on side lobes due to quadrupod) beam not optimal for neither directions but still good enough. Then optimal focus for the first direction, but still more degraded in the perpendicular direction, creating an elongated beam in the direction perpendicular to the one before the best compromise. So, when there's a lot of astigmatism, the best compromise beam is in all cases worse than when there's no astigmatism. In other words, with the strong astigmatism visible in the 3 series of focus, it's certain we can't have 18" or lower circular FWHM. The best compromise beam must be a bit larger than that, even with perfect RPP. Now, is 21" FWHM too big in these conditions? If we assume RPP is not perfect... I don't know...
In all cases there's no other better maximum out of the sequence I just described.

- The preliminary 2mm RPP have been computed with not so good beam maps, so the grid is possibly not regular, while in reality, given the KIDs real positions, it should be regular. Few arcsec error position on many pixels enlarge the beam on maps by few arcsec. If we want a better idea of the real optical beam size, look at the beam profile in the pointing cross scans. I bet that when we are at best focus this is 18" or even less, isn't it? This remark on the RPP is possibly not true anymore since the Oct 8 23:00 entry from SB (tbc).

- The dichroic is totally transparent for the 1 mm beams, so any optical effect it has affects only Ar2, not Ar1 and Ar3!
- But, the dichroic is closer to the cold pupil than to an image surface, which means that even a local distortions on it will affect a very large fraction of the image. In that context, it looks quite complicated that it creates distorted beams on some part of the image and not distorted beams on other parts. That's why I think that the beam shape inhomogeneities visible on the series of beam maps reduced and posted by SB, with elliptic beams on a portion of the Array 2 and more circular beams elsewhere, is probably not a dichroic issue!
- Now, regarding the hypothesis of asymmetries induced by shims not perfectly planar, this is even more unlikely to me. Indeed, the shims have been checked, at most their planarity error is few 10s microns (an probably less in reality), which is totally negligible in terms of beam distortion, by far!

- With a downward residual distortion of the dichroic as we have now, and the fact that the dichroic is tilted, Zemax shows that this creates astigmatism for the reflected beam. So, the hypothesis that the astigmatism visible on Ar2 is caused by the dichroic, doesn't seem totally ruled out yet. But there's several elements that can help figuring out whether it's the dichroic or something else that creates the distortion we see these days on the 2mm beams:
-- The dichroic induced astigmatism is invariant with elevation. So in Nasmyth coordinates, whatever the elevation of the source, the directions of the ellipses before and after the best compromise focus are always the same. Visibly it's not the case on the beam maps...
-- The telescope astigmatism, created by the distortion of M1 with gravity, depends on elevation. It is almost 0 near 45-50° elevation, it appears with a major axis in one direction at higher elevation, and perpendicular to this direction at lower elevation, stronger and stronger when you get further away from 45-50° elevation. So, in Nasmyth the directions of the ellipses vary with elevation, and they are inverted when you pass the 45-50° limit. In other words, the 2 directions of ellipses you see on each side of the best compromise focus, are inverted at lower elevation with respect to the high elevation. On the beam maps we see the rotation with elevation, but do we see the inversion of ellipses direction when we pass the 45-50° limit? It's not clear to me yet...
-- According to my simulation, the astigmatic aberration spot created by the dichroic distortion should stay significantly smaller than the diffraction spot, which means the ellipticity shouldn't be very strong. Besides, the best compromise beam in the simulation is still smaller than the ellipse minor axis at the best focus of each astigmatic direction. In other words, the max beam intensity is at the best compromise focus, not a max a bit before the best compromise and another max a bit after the best compromise.
-- This dichroic astigmatism shouldn't be localized on the image ; it should be everywhere. Though, the direction of the ellipses is not totally uniform, there's should be an axis of symmetry passing by the center of the array, and ellipses slightly tilted on both parts of this axis. But that doesn't correspond to what we see on the maps.
- I don't know yet if, with a dichroic distortion upward there's the same kind of astigmatism. It's possibly not symmetrical. If it is symmetrical, we should have seen this effect before the intervention, but from my recollection this was not the case. I will check with simulations of course.

- We have a focus difference between array 2 and the 1 mm arrays; this means the dichroic distortion is not 1.5 mm amplitude at the center as I targeted when I put the 17 mm shims. So, first of all for the simulations, I need to figure out the distortion we have. Assuming that, based on the shape of the beam we estimate for now Ar1-Ar2 ~ -0.8 mm (for the distance between best 1mm focus, and best compromise round 2 mm beam), I will compute it. Once it's done, I'll try to quantify better everything I said above.

- When the dichroic is distorted, the position of the center of the membrane along the optical axis is not at the designed position. So with the tilt, this shifts the optical axis on the array by the same value as the distortion amplitude (to 1st order). in other word, the projection of the center of the array on sky should be different than the position of the center of the 1mm arrays (for an illustration of this effect, see the Zemax screenshot on https://publicwiki.iram.es/DailyReportsNika2Run81#Friday.2C_2nd_October_2026). That's why I'm a bit surprised that after the good beam maps reduction, Stefano finds the same pointing for all 3 arrays within 1-2 arcsec...

- Another thing that seems a bit neglected now, and might seem disconnected, but is possibly not: the radio alignment. As I wrote in the the Oct 7 NIKA2 meeting minutes, 9 mm radio axis offset offset with respect to the cryostat window center is really a lot. We should double check that. If this is confirmed, that means the "tirant" of the cold M7-M8 assembly are not at the optimal elongation. Since we can't open the cryostat to correct that (for now), the only other way then to avoid spillover on M1, is to put closer the optical/laser axis to the radio axis. To do that, one needs to move the M6 back screws accordingly.
- But first of all the radio alignment must be double checked. Doing it with a hot load in front of a very good, stable and low opacity sky is better than with a cold load on vertex closed 300K background. Sorry, this will take a couple of hours of good sky, but this is important.
- If you find out that optical axis has to be moved to match better the radio axis, and so if you do move M6 screws indeed, the consequence of course is that all the pointing parameters with change... as well as the geometry...

Sorry for the slightly scarring information/reflections...

---

13:00 - 19:00 LT, Mairi : Finished rep for 90-26. Switching to TP and performing repetition for project 092-26. 18:00 LT, switching to polarimetry. Switching to project 084-25, calib scan on 3C286 for IP characterisation. Setting off rep of AFGL2591 and handing over to Miren.

19:00 - 01:00 LT, Miren: Using 3C454 for IP characterisation calib_1scan. Opacity ~ 0.25.

Changed to nikas-26 for a few focus tests. When focus optimised for A1, A2 beam elongated: ~ 17.5" x 33".

22 LT: Back to project 084-25 for two more repetitions on AFGL2591. Opacity ~0.2 and stable (+/- 2 Jy/beam @ A2). Stability improving reaching +/- 0.5 Jy/beam @ A2.

00:35 LT: a skydip under project nikas-26 (20261009s259). Neptune is now available for IP calib_1scans. A fourth repetition on AFGL2591.

October 10th, 2026, Saturday

01:00 - 07:00, Rémi: stable conditions. Reasonable opacity ~0.2-0.3. A bit of reasonable wind.

07:00 - 13:00, Giorgos:Weather stayed stable, opacity around 0.3. Continued with the calibration from Uranus to ALFORI and then Mars.Did a skydip. Started project 090-26.

13:00 - 20:30, Mairi: Bracketing 090-26 IP observations with Mars and 3C286. Switching to TP. Tau increasing. Starting project 093-26, tau around 0.5. Onset of fog 15:30 LT, stopping to see if weather improves. Restarting at 17:00 LT, again with 093-26.

20:30 - 01:00, Ioannis: Continue with 093-26 observations while we wait for the opacity to drop and sky to stabilize better. Around midnight, sky stability looks good (+/- 1.5 Jy/beam) and opacity is relatively low, so I start with 084-25. IP scan on Neptune and another repetition of AFGL2591.

October 11th, 2026, Sunday

01:00 - 07:00, Rémi: opacity ~0.35. Very stable: starting shift with +/- 3 Jy/beam over a ~7mn scan at 45deg elevation, with slow variations. No wind at all.

07:00 - 13:00, Giorgos: opacity 0.35-0.5. Stable sky. Continued from Uranus to ALFORI and then mars to finish calibration and then started project 090-26.Finished project 090-26, switched to TP and started project 093-26.

13:00 - 19:00, Mairi: continuing with 093-26. Patchy cloud, observing in regions where the sky is clear. Opacity increasing, rising to 0.6-0.7, stop at 16:00LT. Remi takes over at 17:30LT to run some tests to make use of the poor weather conditions.

19:00 - 01:00, Ioannis: Bad weather, high opacity and unstable atmosphere throughout the shift. Remi did a test for project 094-26 at the beginning but other than that shift was lost due to adverse weather.

October 12th, 2026, Monday

01:00 - 07:00, Rémi: opacity ~ 0.7-0.8. Only EMIR observations this night.

07:00 - 13:00, Giorgos:

13:00 - 19:00, Mairi: Ioannis starts the shift by carrying out some focus tests. I take over at 14:30LT. Focussing on Mars at low elevation, Remi points out that the shape of the beam in array 1 looks similar to what we are seeing in array 2 with the cross like pattern when in focus (focus sequence s158-162). SB: it looks good and normal to me

height="250" height="250" height="250"

For the remainder of the shift continue with 093-26.

19:00 - 01:00, Miren: Opacity around 0.65, trying several pointings on nikas-26 before continuing with 093-26 or moving to EMIR. Large pointing corrections.

20h30 LT: Opacity not decreasing, so we move to EMIR 3 mm backup projects. Starting with 053-26.

October 13th, 2026, Tuesday