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Astrophotography
Users
Search
Language
EN
English
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Mikhail Maslov
Overview
Photos
340
Rating
2509
Followers
19
Last seen
Nov 9, 2026 at 08:30
Contacts
Novosibirsk, Russia
Photos
Photos
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340 Photos
Telescope/Lens
Newtonian 1200mm f/4.0
smc PENTAX-DA* 300mm f/4 ED [IF] SDM Lens
Newtonian 1200mm f/2.8
smc PENTAX-DA* 300mm f/4.5 ED [IF] SDM Lens
Pentax smc PENTAX-FA 77mm f/1.8 Limited Lens
SMC Pentax FA 77 mm f/6.3 Limited
Newtonian 300mm f/4.5
300mm f/4.5 Lens
SMC Pentax FA 77 mm f/4.5 Limited
Celestron RASA 11
Camera
Pentax KP
Mount
Sky-Watcher AZ-EQ6
AZ-EQ6
Software
IRIS
Accessories
ASA Corrector-Reducer
Photos
Preview
Photo
Published
Views
Likes
Comments
C/2024 J3 ATLAS
Nov 9, 2026
25
6
0
161P/Hartley-IRAS
Nov 8, 2026
21
10
0
260P/McNaught
Sep 22, 2026
118
7
0
C/2024 R4 PanSTARRs
Sep 21, 2026
112
5
0
C/2024 G4 PanSTARRs
Sep 20, 2026
113
6
0
161P/Hartley-IRAS
Sep 17, 2026
218
6
0
260P/McNaught
Sep 16, 2026
105
6
0
C/2026 A2 Bok
Sep 11, 2026
169
5
0
C/2026 A2 Bok
Sep 2, 2026
148
8
0
C/2024 J3 ATLAS
Sep 1, 2026
150
5
0
C/2025 A6 Lemmon
Aug 31, 2026
202
14
1
169P/NEAT
Aug 29, 2026
176
7
0
78P/Gehrels
Aug 26, 2026
242
7
0
10P/Tempel 2
Aug 22, 2026
126
5
0
24P/Schaumasse
Aug 14, 2026
213
17
0
24P/Schaumasse
Aug 11, 2026
194
4
0
24P/Schaumasse
Aug 10, 2026
172
8
0
C/2025 R3 PanSTARRs
Apr 19, 2026
314
19
0
C/2024 E1 Wierzchos
Apr 18, 2026
370
5
0
C/2024 E1 Wierzchos
Apr 1, 2026
252
9
0
C/2022 QE78 ATLAS
Mar 27, 2026
366
8
0
3I/ATLAS
Mar 26, 2026
326
7
0
24P/Schaumasse
Mar 23, 2026
249
7
0
63P/Wild
Mar 22, 2026
266
5
0
C/2024 E1 Wierzchos
Mar 17, 2026
316
9
0
C/2024 E1 Wierzchos
Mar 16, 2026
464
7
0
C/2024 E1 Wierzchos
Mar 7, 2026
261
6
0
C/2025 J1 Borisov
Mar 4, 2026
276
8
0
C/2022 QE78 ATLAS
Feb 28, 2026
374
8
0
3I/ATLAS
Feb 19, 2026
280
10
0
240P/NEAT
Feb 15, 2026
427
15
0
240P/NEAT
Feb 6, 2026
462
8
0
C/2021 S3 PanSTARRs
Dec 31, 2025
565
6
0
C/2023 A3 Tsuchinshan-ATLAS
Dec 27, 2025
524
7
0
C/2022 E2 ATLAS
Dec 25, 2025
602
5
0
C/2022 E2 ATLAS
Dec 17, 2025
493
6
0
C/2021 S3 PanSTARRs
Dec 16, 2025
500
7
0
C/2023 A3 Tsuchinshan-ATLAS
Dec 14, 2025
426
12
0
C/2025 A6 Lemmon
Oct 26, 2025
539
11
1
C/2025 A6 Lemmon
Oct 26, 2025
478
9
0
C/2025 A6 Lemmon
Oct 23, 2025
777
5
0
C/2025 R2 SWAN
Oct 20, 2025
722
6
0
C/2025 A6 Lemmon
Oct 20, 2025
567
13
0
C/2025 A6 Lemmon
Oct 19, 2025
616
7
0
47P/Ashbrook-Jackson
Oct 19, 2025
605
2
0
C/2025 A6 Lemmon
Oct 18, 2025
744
6
0
C/2025 R2 SWAN
Oct 17, 2025
588
6
0
C/2023 R1 PanSTARRs
Oct 16, 2025
425
2
0
C/2025 A6 Lemmon
Oct 15, 2025
770
18
0
C/2023 A3 Tsuchinshan-ATLAS
Oct 7, 2025
487
5
0
C/2022 N2 PanSTARRs
Oct 5, 2025
925
6
0
C/2022 E2 ATLAS
Oct 4, 2025
969
4
0
47P/Ashbrook-Jackson
Oct 3, 2025
499
4
0
C/2023 C2 ATLAS
Oct 1, 2025
638
4
0
48P/Johnson
Sep 25, 2025
804
1
0
486P/Leonard
Sep 24, 2025
1,011
5
0
302P/Lemmon-PanSTARRs
Sep 23, 2025
828
3
0
C/2023 C2 ATLAS
Sep 22, 2025
902
5
0
C/2025 A6 Lemmon
Sep 20, 2025
873
8
0
C/2023 C2 ATLAS
Sep 19, 2025
1,042
8
0
C/2024 E1 Wierzchos
Sep 18, 2025
1,256
7
0
C/2023 R1 PanSTARRs
Sep 3, 2025
1,016
3
0
C/2025 K1 ATLAS
Sep 2, 2025
1,155
5
0
240P/NEAT
Sep 2, 2025
1,202
4
0
C/2022 N2 PanSTARRs
Aug 31, 2025
984
4
1
C/2025 K1 ATLAS
Aug 28, 2025
946
3
0
C/2022 E2 ATLAS
Jul 28, 2025
772
3
0
C/2022 N2 PanSTARRs
Jul 26, 2025
867
1
0
130p/Mcnaught-Hughes
Jul 18, 2025
826
5
0
253P/PanSTARRs
Jul 13, 2025
705
4
0
C/2022 E2 ATLAS
Jul 12, 2025
740
2
0
C/2021 S3 PanSTARRs
Jul 10, 2025
927
2
0
C/2022 QE78 ATLAS
Jul 9, 2025
1,076
3
0
487P/Siding Spring
Jul 8, 2025
726
5
0
C/2022 E2 ATLAS
Jul 7, 2025
747
5
0
130p/Mcnaught-Hughes
Jul 6, 2025
885
3
0
C/2021 S3 PanSTARRs
Jun 29, 2025
917
2
0
13P/Olbers
Jun 28, 2025
774
6
0
C/2023 H5 Lemmon
Jun 19, 2025
974
3
0
P/2023 S1
Jun 18, 2025
972
3
0
C/2022 QE78 ATLAS
Jun 17, 2025
834
2
0
496P/Hill
Jun 5, 2025
823
4
0
C/2021 G2 ATLAS
Jun 4, 2025
898
3
0
C/2024 N4 Sarneczky
May 27, 2025
945
3
0
C/2022 QE78 ATLAS
May 21, 2025
1,061
4
0
496P/Hill
May 16, 2025
1,040
3
0
C/2021 S4 Tsuchinshan
May 14, 2025
937
2
0
P/2025 A5 ATLAS
May 13, 2025
839
2
0
496P/Hill
May 12, 2025
901
4
0
43P/Wolf-Harrington
May 8, 2025
1,041
3
0
C/2023 V1 Lemmon
May 6, 2025
849
4
0
C/2024 E1 Wierzchos
May 1, 2025
1,151
3
0
C/2023 H5 Lemmon
Apr 30, 2025
1,007
2
0
C/2024 B1 Lemmon
Apr 29, 2025
960
4
0
C/2025 F2 SWAN
Apr 28, 2025
1,023
5
0
P/2025 A5 ATLAS
Apr 27, 2025
926
5
0
C/2024 L5 ATLAS
Apr 25, 2025
961
3
0
C/2024 B1 Lemmon
Apr 23, 2025
996
4
0
C/2025 F2 SWAN
Apr 22, 2025
842
6
0
C/2024 E1 Wierzchos
Apr 21, 2025
1,064
3
0
32P/Comas Sola
Apr 20, 2025
871
6
0
29P/Schwassmann-Wachmann
Apr 17, 2025
1,120
3
0
C/2022 QE78 ATLAS
Apr 15, 2025
1,223
3
0
472P/NEAT-LINEAR
Apr 14, 2025
907
2
0
472P/NEAT-LINEAR
Mar 8, 2025
1,028
10
0
496P/Hill
Feb 11, 2025
1,180
4
0
C/2023 A3 Tsuchinshan-ATLAS
Feb 8, 2025
1,301
11
0
29P/Schwassmann-Wachmann
Feb 1, 2025
1,045
6
0
C/2022 QE78 ATLAS
Jan 30, 2025
1,360
7
0
C/2024 M1 ATLAS
Jan 28, 2025
1,114
8
0
C/2023 Q1 PanSTARRs
Jan 27, 2025
1,085
5
0
305P/Skiff
Jan 23, 2025
1,136
8
0
C/2023 H5 Lemmon
Jan 18, 2025
1,006
6
0
154P/Brewington
Jan 17, 2025
1,202
5
0
29P/Schwassmann-Wachmann
Jan 16, 2025
1,058
8
1
P/2023 S1
Jan 11, 2025
976
5
0
C/2022 QE78 ATLAS
Jan 6, 2025
1,506
12
1
C/2024 M1 ATLAS
Jan 6, 2025
1,178
4
0
487P/Siding Spring
Jan 4, 2025
1,029
8
0
276P/Vorobjov
Dec 31, 2024
1,398
7
0
333P/LINEAR
Dec 30, 2024
1,152
6
0
C/2024 J2 Wierzchos
Dec 28, 2024
1,013
8
0
C/2022 E2 ATLAS
Dec 19, 2024
1,096
7
0
472P/NEAT-LINEAR
Dec 9, 2024
1,092
9
0
C/2024 M1 ATLAS
Dec 5, 2024
1,228
6
0
C/2017 K2 PanSTARRs
Dec 5, 2024
1,133
7
0
487P/Siding Spring
Dec 4, 2024
1,074
4
0
C/2022 E2 ATLAS
Dec 4, 2024
1,203
7
0
C/2023 A3 Tsuchinshan-ATLAS
Nov 26, 2024
1,186
11
0
146P/Shoemaker-Linear
Nov 20, 2024
1,142
7
0
328P/LONEOS-Tucker
Nov 19, 2024
1,145
8
0
43P/Wolf-Harrington
Nov 12, 2024
1,312
7
0
C/2023 A3 Tsuchinshan-ATLAS
Nov 7, 2024
1,429
11
0
C/2023 A3 Tsuchinshan-ATLAS
Nov 5, 2024
1,108
8
0
C/2023 A3 Tsuchinshan-ATLAS
Nov 2, 2024
1,389
5
0
C/2023 Q1 PanSTARRs
Oct 31, 2024
1,029
6
0
253P/PanSTARRs
Oct 29, 2024
1,014
4
0
190P/Mueller
Oct 28, 2024
1,053
5
0
C/2021 S3 PanSTARRs
Oct 22, 2024
1,118
9
1
C/2023 A3 Tsuchinshan-ATLAS
Oct 15, 2024
1,386
9
0
C/2019 T4 ATLAS
Aug 14, 2024
1,449
6
0
207P/NEAT
Aug 11, 2024
1,192
4
0
62P/Tsuchinshan
Aug 11, 2024
1,149
6
0
C/2021 S3 PanSTARRs
Aug 10, 2024
1,507
6
0
13P/Olbers
Jul 31, 2024
1,336
9
0
C/2023 A3 Tsuchinshan-ATLAS
Jun 18, 2024
1,319
6
0
207P/NEAT
Jun 17, 2024
1,426
10
0
227P/Catalina-LINEAR
May 24, 2024
1,139
5
0
C/2021 S3 PanSTARRs
May 23, 2024
1,299
8
0
62P/Tsuchinshan
May 20, 2024
1,203
4
0
207P/NEAT
May 14, 2024
1,308
5
0
144P/Kushida
May 10, 2024
1,383
5
0
12P/Pons-Brooks
May 8, 2024
1,277
4
0
62P/Tsuchinshan
May 3, 2024
1,326
5
0
144P/Kushida
Apr 23, 2024
1,877
8
0
103P/Hartley 2
Apr 18, 2024
1,388
7
0
12P/Pons-Brooks
Apr 17, 2024
1,341
12
0
12P/Pons-Brooks
Mar 13, 2024
1,781
17
0
12P/Pons-Brooks
Mar 9, 2024
1,316
9
0
12P/Pons-Brooks
Mar 9, 2024
1,245
6
0
144P/Kushida
Mar 8, 2024
1,312
4
0
103P/Hartley 2
Feb 25, 2024
1,321
4
0
12P/Pons-Brooks
Feb 24, 2024
1,759
7
0
65P/Gunn
Feb 24, 2024
1,532
4
0
C/2023 X1 Leonard
Feb 20, 2024
1,466
4
0
62P/Tsuchinshan
Feb 19, 2024
1,471
11
0
103P/Hartley 2
Feb 18, 2024
1,328
3
0
C/2017 K2 PanSTARRs
Feb 15, 2024
1,786
5
0
12P/Pons-Brooks
Feb 10, 2024
1,600
5
0
62P/Tsuchinshan
Feb 6, 2024
1,539
10
0
65P/Gunn
Feb 3, 2024
1,544
6
0
C/2023 X1 Leonard
Feb 2, 2024
1,351
6
0
227P/Catalina-LINEAR
Feb 2, 2024
1,250
3
0
C/2022 U3 Bok
Feb 1, 2024
1,496
4
0
C/2017 K2 PanSTARRs
Feb 1, 2024
1,481
4
0
62P/Tsuchinshan
Jan 30, 2024
1,461
5
0
62P/Tsuchinshan
Jan 29, 2024
1,310
6
0
62P/Tsuchinshan
Jan 28, 2024
1,348
8
0
C/2022 E2 ATLAS
Jan 22, 2024
1,237
5
0
12P/Pons-Brooks
Jan 22, 2024
1,474
9
0
12P/Pons-Brooks
Jan 19, 2024
1,447
6
0
310P/Hill
Jan 10, 2024
1,282
3
0
P/2023 S1
Jan 10, 2024
1,346
2
0
471P
Jan 9, 2024
1,496
4
0
C/2022 JK5 PanSTARRs
Jan 9, 2024
1,442
4
0
C/2023 H2 Lemmon
Jan 8, 2024
1,302
6
0
347P/PanSTARRs
Jan 7, 2024
1,613
2
0
C/2022 U1 Leonard
Jan 7, 2024
1,259
3
0
103P/Hartley 2
Jan 6, 2024
1,277
2
0
62P/Tsuchinshan
Jan 5, 2024
1,423
3
0
C/2022 U1 Leonard
Jan 5, 2024
1,515
4
0
29P/Schwassmann-Wachmann
Jan 4, 2024
1,329
4
0
170P/Christensen
Jan 3, 2024
1,518
4
0
103P/Hartley 2
Jan 3, 2024
1,308
6
0
C/2017 K2 PanSTARRs
Jan 2, 2024
1,440
4
0
62P/Tsuchinshan
Jan 2, 2024
1,452
4
0
C/2021 S4 Tsuchinshan
Jan 1, 2024
1,505
4
0
32P/Comas Sola
Jan 1, 2024
1,758
3
0
144P/Kushida
Dec 31, 2023
1,515
4
0
C/2021 X1 Maury-Attard
Dec 31, 2023
1,232
4
0
12P/Pons-Brooks
Dec 30, 2023
1,334
3
0
62P/Tsuchinshan
Dec 30, 2023
1,508
5
0
103P/Hartley 2
Dec 28, 2023
1,415
5
0
62P/Tsuchinshan
Dec 28, 2023
1,619
6
0
29P/Schwassmann-Wachmann
Dec 27, 2023
1,431
6
0
C/2017 K2 PanSTARRs
Dec 26, 2023
1,490
5
0
144P/Kushida
Dec 26, 2023
1,440
5
0
12P/Pons-Brooks
Dec 24, 2023
1,414
13
0
C/2019 U5 PanSTARRs
Nov 3, 2023
1,472
6
0
C/2019 T4 ATLAS
Nov 1, 2023
1,512
10
0
C/2022 U4 Bok
Oct 31, 2023
1,536
7
0
103P/Hartley 2
Oct 31, 2023
1,572
7
0
103P/Hartley 2
Oct 30, 2023
1,366
7
0
103P/Hartley 2
Oct 30, 2023
1,525
11
0
170P/Christensen
Oct 29, 2023
1,548
6
0
310P/Hill
Oct 29, 2023
1,751
6
0
465P/Hill
Oct 28, 2023
1,483
6
0
32P/Comas Sola
Oct 27, 2023
1,551
5
0
62P/Tsuchinshan
Oct 27, 2023
1,532
4
0
C/2022 S4 Lemmon
Oct 26, 2023
1,430
4
0
71P/Clark
Oct 26, 2023
1,346
4
0
117P/Helin-Roman-Alu
Oct 25, 2023
1,753
4
0
C/2022 JK5 PanSTARRs
Oct 25, 2023
1,445
4
0
C/2023 E1 ATLAS
Oct 24, 2023
1,502
5
0
C/2023 R1 PanSTARRs
Oct 24, 2023
1,503
4
0
170P/Christensen
Oct 23, 2023
1,308
6
0
C/2022 S2 Lemmon
Oct 23, 2023
1,623
6
0
C/2021 X1 Maury-Attard
Oct 22, 2023
1,573
10
0
126P/IRAS
Oct 22, 2023
1,461
8
0
P/2023 KF3
Oct 21, 2023
1,567
4
0
12P/Pons-Brooks
Oct 21, 2023
1,528
6
0
2P/Encke
Oct 20, 2023
1,385
8
0
103P/Hartley 2
Oct 20, 2023
1,543
9
0
126P/IRAS
Oct 19, 2023
1,603
7
0
C/2020 V2 ZTF
Oct 17, 2023
1,548
8
0
C/2022 A2 PanSTARRs
Oct 16, 2023
1,744
10
0
103P/Hartley 2
Oct 16, 2023
1,402
9
0
C/2023 H2 Lemmon
Oct 15, 2023
1,649
12
0
126P/IRAS
Oct 15, 2023
1,736
6
0
103P/Hartley 2
Oct 13, 2023
1,744
11
0
C/2023 E1 ATLAS
Oct 12, 2023
1,558
7
0
12P/Pons-Brooks
Oct 7, 2023
1,572
5
0
237P/LINEAR
Oct 6, 2023
1,405
8
0
103P/Hartley 2
Oct 2, 2023
1,593
4
0
C/2022 A2 PanSTARRs
Sep 27, 2023
1,562
7
0
C/2020 V2 ZTF
Sep 26, 2023
1,713
6
0
2P/Encke
Sep 26, 2023
1,586
7
0
C/2023 E1 ATLAS
Sep 23, 2023
1,559
7
0
C/2023 H2 Lemmon
Sep 22, 2023
1,963
12
0
C/2022 A2 PanSTARRs
Sep 13, 2023
1,563
9
0
C/2020 R7 ATLAS
Sep 13, 2023
1,630
5
0
C/2023 Tsuchinshan-ATLAS
Sep 12, 2023
1,627
8
0
C/2020 F2 ATLAS
Sep 11, 2023
1,505
7
0
C/2023 E1 ATLAS
Sep 11, 2023
1,429
8
0
C/2020 V2 ZTF
Sep 8, 2023
1,566
8
0
103P/Hartley 2
Sep 7, 2023
1,636
6
0
C/2022 A2 PanSTARRs
Sep 6, 2023
1,437
11
0
C/2023 E1 ATLAS
Sep 6, 2023
1,662
11
0
103P/Hartley 2
Sep 5, 2023
1,558
10
0
126P/IRAS
Sep 4, 2023
1,588
10
0
12P/Pons-Brooks
Sep 3, 2023
1,352
8
0
237P/LINEAR
Sep 1, 2023
1,450
8
0
2P/Encke
Sep 1, 2023
1,599
9
0
C/2023 P1 Nishimura
Aug 29, 2023
1,782
11
0
C/2022 A2 PanSTARRs
Aug 29, 2023
1,777
9
0
C/2020 R7 PanSTARRS
Aug 25, 2023
1,425
8
0
C/2022 L2 ATLAS
Aug 25, 2023
1,455
9
0
C/2023 A3 Tsuchinshan-ATLAS
Aug 24, 2023
1,801
8
0
C/2019 T4 ATLAS
Aug 24, 2023
1,503
9
0
C/2023 E1 ATLAS
Aug 11, 2023
1,633
9
0
C/2022 W3 Leonard
Aug 11, 2023
1,562
8
0
81P/Wild
Aug 10, 2023
1,647
4
0
364P/PanSTARRs
Aug 9, 2023
1,472
6
0
77P/Longmore
Aug 9, 2023
1,405
5
0
C/2022 E2 ATLAS
Aug 8, 2023
1,604
5
0
364P/PanSTARRs
Aug 7, 2023
1,917
7
0
211P/Hill
Aug 7, 2023
1,429
4
0
402P/LINEAR
Aug 6, 2023
1,461
7
0
65P/Gunn
Aug 6, 2023
1,529
7
0
118P/Shoemaker-Levy
Aug 5, 2023
1,436
6
0
C/2022 E3 ZTF
Aug 5, 2023
1,535
6
0
C/2019 T4 ATLAS
Aug 4, 2023
1,769
6
0
C/2019 T4 ATLAS
Aug 4, 2023
1,412
7
0
263P/Gibbs
Aug 3, 2023
1,456
7
0
C/2022 U4 Bok
Jul 22, 2023
1,436
6
0
C/2023 A1 Leonard
Jul 22, 2023
1,533
6
0
C/2022 E2 ATLAS
Jul 21, 2023
1,393
5
0
C/2022 W3 Leonard
Jul 21, 2023
1,526
6
0
C/2019 T4 ATLAS
Jul 19, 2023
1,468
5
0
263P/Gibbs
Jul 18, 2023
1,584
3
0
C/2022 U4 Bok
Jul 18, 2023
1,525
4
0
P/2023 B1 PanSTARRs
Jul 17, 2023
1,521
3
0
C/2022 U2 ATLAS
Jul 16, 2023
1,462
6
0
C/2019 U5
Jul 14, 2023
1,565
6
0
C/2020 S4 PanSTARRs
Jul 13, 2023
1,346
5
0
180P/NEAT
Jul 13, 2023
1,417
4
0
29P/Schwassmann-Wachmann
Jul 12, 2023
1,359
4
0
C/2022 U2 ATLAS
Jul 12, 2023
1,520
4
0
C/2022 A2 PanSTARRs
Jun 30, 2023
1,580
10
0
C/2022 U2 ATLAS
Jun 26, 2023
1,688
13
0
C/2022 A2 PanSTARRs
Jun 23, 2023
1,429
10
0
C/2020 V2 ZTF
Jun 23, 2023
1,552
5
0
C/2020 V2 ZTF
Jun 21, 2023
1,466
6
0
C/2022 U2 ATLAS & C/2022 E3 ZTF
Mar 4, 2023
1,706
10
0
C/2021 Y1 ATLAS
Oct 23, 2022
1,666
15
0
C/2021 Y1 ATLAS
Sep 26, 2022
1,799
16
0
Mars and the Pleiades
Aug 31, 2022
1,899
15
1
C/2017 K2 PanSTARRs
Jun 21, 2022
1,779
9
0
C/2017 K2 PanSTARRs
Jun 18, 2022
1,939
13
0
C/2017 K2 PanSTARRs
Jun 16, 2022
1,916
4
0
C/2017 K2 PanSTARRs
Jun 15, 2022
2,132
7
0
C/2017 K2 PanSTARRs
Jun 10, 2022
1,965
7
0
C/2020 K1 PanSTARRs
Jun 9, 2022
1,897
5
0
C/2020 O2 Amaral
Jun 7, 2022
1,823
8
0
C/2017 K2 PanSTARRs
May 29, 2022
2,072
9
1
C/2021 A1 Leonard
Mar 6, 2022
2,183
5
0
4P/Faye
Dec 7, 2021
2,024
3
0
C/2019 L3 ATLAS
Dec 6, 2021
2,034
7
0
C/2021 A1 Leonard
Dec 6, 2021
2,164
10
0
C/2021 A1 Leonard
Dec 5, 2021
2,186
14
0
C/2021 A1 Leonard
Dec 3, 2021
2,356
23
0
C/2021 A1 Leonard
Dec 3, 2021
2,220
14
0
C/2021 A1 Leonard
Dec 2, 2021
2,215
14
0
C/2021 A1 Leonard
Dec 1, 2021
2,064
9
0
4P/Faye
Dec 1, 2021
2,086
8
0
397P/Lemmon
Feb 5, 2021
2,213
6
0
277P/LINEAR and P/2020 U2 PanSTARRs
Jan 29, 2021
2,498
10
0
156P/Russell-LINEAR and M33
Jan 28, 2021
2,272
12
0
84P/Giclas
Jan 26, 2021
2,854
9
0
C/2019 L3 ATLAS
Jan 26, 2021
2,613
9
0
C/2020 M3 ATLAS and the Capella star
Jan 18, 2021
2,471
8
0
C/2020 M3 ATLAS
Jan 9, 2021
2,410
12
0
C/2018 N2 ASASSN
Jan 8, 2021
2,004
1
0
C/2020 M3 ATLAS
Jan 6, 2021
2,335
13
0
C/2020 M3 ATLAS and Bellatrix
Dec 25, 2020
2,628
6
0
C/2020 M3 ATLAS near IC 410 and IC 405
Dec 17, 2020
2,407
10
0
C/2020 M3 ATLAS near IC 410
Dec 12, 2020
2,131
6
0
C/2020 M3 ATLAS near Bellatrix
Dec 1, 2020
2,051
6
0
C/2020 Q1 Borisov near the Crescent Nebula NGC 6888
Oct 18, 2020
2,054
3
0
P/2020 M2 Lemmon near IC 405 the Flaming Star Nebula
Oct 16, 2020
2,886
12
0
No matching photos.