Engelhardsberg observatory
Comets By Designation (table is sortable)
info
Nr.
comet
last observed
thumbnail
observations
1
2P/Encke
2017
10
2
4P/Faye
04.09.2021
6
3
6P/d'Arrest
01.09.2021
3
4
7P/Pons-Winnecke
15.04.2021
3
5
8P/Tuttle
08.05.2021
1
6
9P/Tempel
2016
6
7
10P/Tempel
08.09.2021
5
8
11P/Tempel-Swift-Linear
14.11.2020
1
9
12P/Pons-Brooks
10.08.2023
2
10
14P/Wolf
2017
1
11
15P/Finlay
15.08.2021
6
12
16P/Brooks
2014
1
13
17P/Holmes
29.10.2021
6
14
19P/Borrelly
20.03.2022
4
15
21P/Giacobini-Zinner
18.09.2018
32
16
22P/Kopff
25.07.2022
6
17
24P/Schaumasse
22.02.2018
4
18
28P/Neujmin
15.08.2021
1
19
29P/Schwassmann-Wachmann
27.12.2022
11
20
30P/Reinmuth
2017
2
21
31P/Schwassmann-Wachmann
07.03.2019
1
22
32P/Comas-Sola
2015
7
23
33P/Daniel
2016
2
24
36P/Whipple
28.08.2019
1
25
37P/Forbes
20.08.2018
4
26
38P/Stephan-Oterma
27.02.2019
6
27
40P/Väisälä
2015
1
28
41P/Tuttle-Giacobini-Kresak
2017
10
29
43P/Wolf-Harrington
2016
2
30
44P/Reinmuth
05.09.2022
2
31
45P/Honda-Mrkos-Pajdusakova
2017
12
32
46P/Wirtanen
07.03.2019
5
33
47P/Ashbrook-Jackson
2017
4
34
48P/Johnson
15.08.2018
5
35
49P/Arend-Rigaux
29.03.2019
1
36
50P/Arend
2015
1
37
52P/Harrington/Abell
2014
3
38
53P/van Biesbroeck
2016
4
39
56P/Slaughter-Burnham
2016
4
40
57P/du Toit-Neujmin-Delporte
2015
1
41
59P/Kearns-Kwee
2017
1
42
60P/Tsuchinshan
30.03.2019
2
43
61P/Shajn-Schaldach
30.08.2022
3
44
62P/Tsuchinshan 1
19.02.2018
3
45
63P/Wild
2013
1
46
64P/Swift-Gehrels
18.09.2018
12
47
65P/Gunn
05.09.2018
3
48
66P/du Toit
13.08.2018
1
49
67P/Churyumov-Gerasimenko
02.03.2022
8
50
68P/Klemola
26.08.2019
5
51
70P/Kojima
23.03.2022
7
52
71P/Clark
2017
2
53
73P/Schwassmann-Wachmann 3
26.03.2022
5
54
74P/Smirnova-Chernykh
06.04.2018
5
55
76P/West-Kohoutek-Ikemura
04.12.2019
1
56
77P/Longmore
2016
3
57
78P/Gehrels 2
22.03.2020
7
58
81P/Wild
19.01.2023
11
59
84P/Giclas
2014
2
60
87P/Bus
24.03.2020
2
61
88P/Howell
26.05.2020
12
62
89P/Russell
2016
1
63
90P/Gehrels 1
2017
1
64
91P/Rusell
11.04.2020
1
65
93P/Lovas 1
2017
3
66
94P/Russell
09.02.2023
2
67
95P/Chiron
2016
3
68
98P/Takamizawa
2013
2
69
99P/Kowal 1
23.03.2022
3
70
100P/Hartley 1
27.03.2022
2
71
101P/Chernykh
30.11.2019
3
72
102P/Shoemaker
2013
3
73
103P/Hartley 2
24.08.2023
4
74
104P/Kowal 2
26.03.2022
6
75
105P/Singer Brewster
08.04.2018
2
76
106P/Schuster
2014
1
77
107P/Wilson-Harrington
07.08.2022
1
78
108P/Ciffreo
28.02.2022
5
79
110P/Hartley
26.03.2022
4
80
112P/Urata-Niijima
19.04.2020
3
81
114P/Wiseman-Skiff
22.03.2020
5
82
115P/Maury
20.08.2020
3
83
116P/Wild
26.03.2022
7
84
117P/Helin-Roman-Alu 1
18.03.2020
4
85
118P/Shoemaker-Levy 4
27.12.2022
4
86
119P/Parker-Hartley
27.12.2022
5
87
123P/West-Hartley
07.05.2019
6
88
124P/Mrkos
15.03.2020
5
89
125P/Spacewatch
2013
1
90
126P/Iras
14.08.2023
1
91
127P/Holm-Olmstead
24.08.2022
1
92
128P/Shoemaker-Holt 1
2016
1
93
129P/Shoemaker-Levy
14.08.2018
4
94
130P/McNaught-Hughes
13.08.2018
2
95
131P/Mueller
05.09.2018
1
96
132P/Helin-Roman-Alu 2
06.09.2021
3
97
133P/Elst-Pizzaro
02.09.2019
1
98
134P/Kowal-Vavrova
2014
6
99
136P/Mueller
2016
1
100
137P/Shoemaker-Levy
14.08.2018
4
101
139P/Vaisala-Oterma
2017
2
102
141P/Machholz
07.03.2021
2
103
143P/Kowal-Mrkos
08.04.2018
1
104
144P/Kushida
2016
2
105
145P/Shoemaker-Levy
2017
1
106
146P/Shoemaker-LINEAR
2016
1
107
149P/Mueller
29.03.2019
1
108
150P/Smirnova-Chernykh
2015
1
109
152P/Helin-Lawrence
13.04.2021
1
110
154P/Brewington
2014
8
111
155P/Shoemaker
15.03.2020
2
112
156P/Russell-LINEAR
07.03.2021
3
113
157P/Tritton
06.09.2022
2
114
158P/Kowal-LINEAR
2013
1
115
159P/LONEOS
2017
1
116
160P/LINEAR
21.01.2020
2
117
162P/Siding Spring
2016
1
118
164P/Christensen
27.02.2019
1
119
170P/Christensen
2014
2
120
171P/Spahr
18.09.2018
1
121
172P/Yeung
2016
1
122
173P/Mueller
28.12.2019
2
123
174P/Echeclus
2016
2
124
176P/LINEAR
2016
1
125
178P/Hug-Bell
2014
3
126
180P/NEAT
2016
2
127
183P/Korlevic-Juric
06.04.2018
1
128
184P/Lovas
2013
1
129
185P/Petriew
06.04.2018
2
130
187P/LINEAR
19.04.2018
1
131
188P/LINEAR-Mueller
2017
2
132
191P/McNaught
2014
1
133
193P/LINEAR-NEAT
12.09.2021
4
134
194P/Kowal
2016
1
135
199P/Shoemaker
03.04.2022
1
136
200P/Larsen
02.08.2018
1
137
201P/LONEOS
2015
2
138
203P/Korlevic
30.11.2019
2
139
204P/LINEAR-NEAT
18.01.2023
3
140
205P/Giacobini
2015
1
141
208P/McMillan
2016
1
142
209P/LINEAR
2014
8
143
210P/Christensen
25.04.2020
6
144
211P/Hill
21.02.2023
3
145
213P/Van Ness
2017
1
146
217P/LINEAR
2017
2
147
218P/LINEAR
2015
2
148
219P/LINEAR
2016
2
149
221P/LINEAR
2015
1
150
223P/Skiff
11.09.2018
2
151
226P/Pigott-LINEAR-Kowalski
2016
3
152
228P/LINEAR
01.01.2020
1
153
230P/LINEAR
2015
1
154
231P/LINEAR
31.03.2019
2
155
235P/LINEAR
04.04.2018
1
156
236P/LINEAR
2017
2
157
237P/LINEAR
2016
1
158
238P/Read
2016
1
159
239P/LINEAR
06.04.2019
1
160
240P/NEAT
27.02.2019
1
161
243P/NEAT
06.08.2018
1
162
244P/Scotti
2014
1
163
245P/WISE
14.08.2018
2
164
246P/NEAT
16.04.2020
8
165
247P/LINEAR
27.02.2019
1
166
249P/LINEAR
14.04.2020
4
167
250P/Larson
21.02.2018
1
168
252P/LINEAR
2016
3
169
257P/Catalina
2013
4
170
260P/McNaught
26.10.2019
7
171
261P/Larson
03.09.2019
3
172
263P/Gibbs
15.03.2023
3
173
266P/Christensen
22.03.2020
4
174
269P/Jedicke
2015
3
175
270P/Gehrels
2014
1
176
273P/Pons-Gambart
2013
1
177
274P/Tombaugh-Tenagra
27.02.2022
1
178
277P/LINEAR
14.11.2020
3
179
278P/McNaught
19.04.2020
2
180
279P/La Sagra
2016
1
181
282P
04.04.2021
1
182
284P/McNaught
02.09.2021
3
183
285P/LINEAR
01.09.2022
8
184
286P/Christensen
29.08.2022
3
185
288P
2016
1
186
289P/Blanpain
21.01.2020
3
187
290P/Jager
2014
5
188
291P/NEAT
2013
2
189
292P/Li
2013
1
190
293P/Spacewatch
2014
2
191
294P/LINEAR
2014
1
192
296P/Garradd
2014
2
193
297P/Beshore
2014
2
194
299P/Catalina-PANSTARRS
2016
1
195
302P/Lemmon-PANSTARRS
2016
1
196
303P/NEAT
2014
1
197
304P/Ory
21.08.2020
1
198
305P/Skiff
2014
2
199
307P/LINEAR
2014
1
200
312P/NEAT
21.08.2020
1
201
314P/Montani
2015
1
202
315P/LONEOS
2017
5
203
318P/McNaught-Hartley
2015
1
204
325P/Yang-Gao
02.07.2022
2
205
327P/Van Ness
06.09.2022
5
206
328P/LONEOS-Tucker
2015
1
207
329P/LINEAR-Catalina
2015
1
208
330P/Catalina
2016
1
209
332P/Ikeya-Murakami
2016
2
210
333P/LINEAR
2016
2
211
334P/NEAT
20.05.2018
1
212
337P/WISE
01.07.2022
2
213
338P/McNaught
2016
1
214
340P/Boattini
2016
1
215
341P/Gibbs
2016
1
216
343P/NEAT-LONEOS
2016
2
217
344P/Read
2016
1
218
345P/LINEAR
2016
1
219
346P/Catalina
2016
1
220
347P/PANSTARRS
2016
1
221
349P/Lemmon
2017
1
222
352P/Skiff
2017
2
223
355P/LINEAR-NEAT
2017
2
224
356P/WISE
2017
1
225
360P/WISE
2017
1
226
361P/Spacewatch
2017
2
227
362P/(457175)
2017
1
228
364P/PANSTARRS
27.03.2023
6
229
365P/LINEAR
04.04.2018
1
230
366P/LINEAR
07.04.2018
1
231
368P/NEAT
15.09.2018
3
232
369P/Hill
12.09.2018
1
233
370P/NEAT
18.09.2018
1
234
371P/LINEAR-Skiff
12.09.2018
1
235
373P/Rinner
06.04.2019
1
236
375P/Hill
31.03.2019
2
237
376P/Loneos
30.04.2019
3
238
377P/Scotti
23.03.2020
1
239
378P/McNaught
30.08.2022
1
240
379P/Spacewatch
23.04.2019
2
241
380P/PANSTARRS
30.04.2019
1
242
382P/Larson
07.08.2022
2
243
384P/Kowalski
28.12.2019
3
244
385P/Hill
30.11.2019
1
245
390P/Gibbs
21.01.2020
2
246
392P/LINEAR
30.11.2019
1
247
395P/Catalina-NEAT
14.11.2022
4
248
397P/Lemmon
21.08.2020
1
249
398P/Boattini
07.03.2021
3
250
399P/PANSTARRS
2013
1
251
402P/LINEAR
28.02.2022
2
252
404P/Bressi
11.08.2021
1
253
405P/Lemmon
14.11.2020
2
254
407P/PANSTARRS-Fuls
14.04.2020
3
255
408P/Novichonok-Gerke
03.09.2021
2
256
409P/LONEOS-Hill
04.04.2021
2
257
413P/Larson
04.04.2021
2
258
415P/Tenagra
08.04.2021
1
259
418P/LINEAR
08.04.2021
1
260
425P/Kowalski
07.09.2021
1
261
433P/(248370)
15.08.2021
2
262
440P/Kobayashi
26.03.2022
3
263
442P/McNaught
02.09.2022
2
264
445P/Lemmon-PANSTARRS
01.09.2022
2
265
446P/McNaught
06.08.2022
1
266
452P/Sheppard-Jewitt
21.02.2023
1
267
453P/WISE-Lemmon
17.03.2023
1
268
465P/Hill
15.08.2023
1
269
6478 Gault (comet like asteroid)
30.03.2019
1
270
C/1975 V1 (West)
1976
1
271
C/2006 S3 (Loneos)
2015
6
272
C/2006 W3 (Christensen)
2009
1
273
C/2007 Q3 (SidingSpring)
2010
1
274
C/2008 S3 (Boattini)
2014
2
275
C/2009 F4 (McNaught)
2014
1
276
C/2009 K5 (McNaught)
2010
1
277
C/2010 S1 (LINEAR)
2014
7
278
C/2010 U3 (Boattini)
27.02.2019
3
279
C/2011 J2 (LINEAR)
2015
13
280
C/2011 KP36 (Spacewatch)
2016
5
281
C/2011 L4 (PANSTARRS)
2014
13
282
C/2011 R1 (McNaught)
2013
4
283
C/2012 A1 (PANSTARRS)
2013
1
284
C/2012 A2 (Linear)
2013
2
285
P/2012 B1 (PANSTARRS)
2014
1
286
P/2012 F2 (PANSTARRS)
2013
1
287
C/2012 F3 (PANSTARRS)
2015
3
288
C/2012 F6 (Lemmon)
2014
9
289
C/2012 J1 (Catalina)
2014
3
290
C/2012 K1 (PANSTARRS)
2014
17
291
C/2012 K6 (McNaught)
2014
5
292
C/2012 K8 (Lemmon)
2014
3
293
C/2012 LP26 (Palomar)
2016
4
294
C/2012 S1 (ISON)
2013
2
295
C/2012 S3 (PANSTARRS)
2013
4
296
C/2012 S4 (PANSTARRS)
2013
1
297
C/2012 U1 (PANSTARRS)
2013
1
298
C/2012 X1 (LINEAR)
2014
6
299
C/2013 A1 (Siding Spring)
2015
2
300
C/2013 C2 (Tenagra)
2014
2
301
C/2013 E1 (McNaught)
2014
1
302
C/2013 E2 (Iwamoto)
2013
2
303
C/2013 F2 (Catalina)
2014
2
304
C/2013 F3 (McNaught)
2013
1
305
C/2013 G1 (Kowalski)
2014
1
306
C/2013 G3 (PANSTARRS)
2014
3
307
C/2013 G5 (Catalina)
2013
1
308
C/2013 G8(PANSTARRS)
2014
1
309
C/2013 G9(Tenagra)
2014
1
310
C/2013 H1(La Sagra)
2013
1
311
C/2013 H2(Boattini)
2014
1
312
P/2013 J2 (McNaught)
2013
5
313
C/2013 P2 (PANSTARRS)
2014
1
314
C/2013 P3 (Palomar)
2014
1
315
C/2013 P4 (PANSTARRS)
2014
1
316
C/2013 R1 (Lovejoy)
2014
11
317
P/2013 R3 (Catalina-PANSTARRS)
2013
2
318
P/2013 T2 (Schwartz)
2013
1
319
C/2013 TW5
2015
4
320
C/2013 U1 (Catalina)
2013
1
321
C/2013 U2 (Holvorcem)
2015
3
322
C/2013 UQ4 (Catalina)
2014
9
323
C/2013 US10 (Catalina)
2016
10
324
C/2013 V1 (Boattini)
2014
8
325
C/2013 V2 (Borisov)
2015
6
326
C/2013 V3 (Nevski)
2014
3
327
C/2013 V4 (Catalina)
2016
9
328
C/2013 V5 (Oukaimeden)
2014
5
329
P/2013 W1 (PANSTARRS)
2013
1
330
C/2013 X1 (PANSTARRS)
2015
5
331
C/2013 Y2 (PANSTARRS)
2014
1
332
P/2014 A2 (Hill)
2014
1
333
C/2014 A4 (SONEAR)
2016
7
334
C/2014 AA52 (Catalina)
2014
1
335
C/2014 B1 (Schwartz)
08.04.2018
4
336
C/2014 C3 (NEOWISE)
2014
2
337
P/2014 D2 (Catalina-PANSTARRS)
2014
2
338
C/2014 E2 (Jacques)
2014
12
339
C/2014 F1 (Hill)
2014
1
340
C/2014 F2 (Tenagra)
2015
2
341
C/2014 G3 (PANSTARRS)
2014
1
342
C/2014 H1 (Christensen)
2014
1
343
P/2014 L2 (NEOWISE)
2014
4
344
P/2014 L3 (Hill)
2014
2
345
C/2014 M3 (Catalina)
2014
1
346
P/2014 M4 (PANSTARRS)
2014
1
347
P/2014 MG4 (Spacewatch-PANSTARRS)
2014
1
348
C/2014 N3 (NEOWISE)
2015
5
349
C/2014 OE4 (PANSTARRS)
12.07.2018
6
350
C/2014 Q1 (PANSTARRS)
2014
2
351
C/2014 Q2 (Lovejoy)
2016
16
352
C/2014 Q3 (Borisov)
2014
6
353
C/2014 R1 (Borisov)
2015
1
354
C/2014 R3 (PANSTARRS)
18.05.2018
3
355
C/2014 R4 (Gibbs)
2014
1
356
C/2014 S2 (PANSTARRS)
2016
11
357
C/2014 W2 (PANSTARRS)
2016
8
358
C/2014 W9 (PANSTARRS)
2015
1
359
C/2014 W11 (PANSTARRS)
2015
2
360
P/2014 X1 (Elenin)
2015
3
361
C/2014 Y1 (PANSTARRS)
2015
3
362
C/2015 C1 (TOTAS-GIBBS)
2015
2
363
C/2015 C2 (SWAN)
2015
2
364
C/2015 D3 (PANSTARRS)
2015
1
365
C/2015 ER61 (PANSTARRS)
2017
4
366
C/2015 F2 (Polonia)
2015
1
367
C/2015 F3 (SWAN)
2015
2
368
C/2015 F4 (Jacques)
2015
2
369
C/2015 F5 (SWAN-Xingming)
2015
3
370
C/2015 G2 (MASTER)
2015
1
371
C/2015 GX (PANSTARRS)
2015
1
372
C/2015 H2 (PANSTARRS)
11.09.2018
1
373
C/2015 K1 (MASTER)
2015
1
374
C/2015 LC2 (PANSTARRS)
2016
1
375
C/2015 M3 (PANSTARRS)
2015
1
376
C/2015 O1 (PANSTARRS)
01.07.2018
7
377
C/2015 T2 (PANSTARRS)
2017
1
378
C/2015 T4 (PANSTARRS)
2015
1
379
P/2015 TP200 (LINEAR)
2016
2
380
C/2015 V1 (PANSTARRS)
2017
4
381
C/2015 V2 (Johnson)
2017
21
382
C/2015 V3 (PANSTARRS)
2015
1
383
C/2015 VL62 (Lemmon-Yeung-PanSTARRS )
2017
6
384
C/2015 W1 (Gibbs)
2016
1
385
P/2015 W2 (Catalina)
2015
1
386
C/2015 WZ (PANSTARRS)
2016
3
387
C/2015 X4 (Elenin)
2015
1
388
C/2015 X7 (ATLAS)
2017
3
389
C/2015 X8 (NEOWISE)
2015
1
390
C/2015 XY1 (Lemmon)
06.02.2018
2
391
C/2015 Y1 (LINEAR)
2016
1
392
C/2015 YG1 (NEOWISE)
2016
1
393
C/2016 A1 (PANSTARRS)
06.04.2018
4
394
C/2016 A8 (LINEAR)
2016
5
395
P/2016 BA14 (PANSTARRS)
2016
1
396
C/2016 B1 (NEOWISE)
2017
1
397
C/2016 C1 (PANSTARRS)
2016
1
398
P/2016 G1 (PANSTARRS)
2016
1
399
C/2016 KA (Catalina)
2016
1
400
C/2016 K1 (LINEAR)
2016
2
401
C/2016 M1 (PANSTARRS)
21.05.2018
13
402
C/2016 N4 (Master)
20.05.2018
5
403
C/2016 N6 (PANSTARRS)
18.04.2018
8
404
P/2016 P2 (PANSTARRS)
2016
1
405
C/2016 Q2 (PANSTARRS)
31.05.2021
2
406
C/2016 Q4 (Kowalski)
2016
1
407
C/2016 R2 (PANSTARRS)
02.07.2019
11
408
C/2016 T1 (Matheny)
2016
1
409
C/2016 T2 (Matheny)
2016
2
410
C/2016 T3 (PANSTARRS)
06.02.2018
2
411
C/2016 U1 (NEOWISE)
2016
2
412
C/2016 VZ18 (PANSTARRS)
2017
5
413
C/2016 X1 (Lemmon)
2016
1
414
C/2017 AB5 (PANSTARRS)
06.02.2018
1
415
C/2017 D2 (Barros)
2017
1
416
C/2017 D3 (ATLAS)
19.02.2018
1
417
C/2017 E3 (PANSTARRS)
18.04.2018
2
418
C/2017 E4 (Lovejoy)
2017
1
419
C/2017 K2 (PANSTARRS)
21.07.2022
36
420
C/2017 K4 (ATLAS)
16.07.2018
2
421
C/2017 K6 (Jacques)
19.02.2018
1
422
C/2017 M4 (ATLAS)
05.08.2018
7
423
C/2017 M5 (TOTAS)
14.08.2018
3
424
C/2017 O1 (ASASSN)
06.04.2018
6
425
C/2017 S3 (PANSTARRS)
03.08.2018
15
426
P/2017 S5 (ATLAS)
2017
1
427
C/2017 S6 (Catalina)
2017
1
428
C/2017 S7 (Lemmon)
2017
1
429
C/2017 T1 (Heinze)
2017
2
430
C/2017 T2 (PANSTARRS)
26.05.2020
24
431
C/2017 T3 (ATLAS)
2017
1
432
C/2017 U7 (PANSTARRS)
01.09.2021
2
433
C/2017 W2 (Leonard)
06.02.2018
1
434
P/2017 W3 (Gibbs)
08.04.2018
1
435
C/2018 A1 (PANSTARRS)
06.02.2018
1
436
C/2018 A3 (ATLAS)
23.08.2019
2
437
C/2018 A6 (Gibbs)
04.04.2018
2
438
C/2018 B1 (Lemmon)
03.03.2018
1
439
P/2018 C1 (Lemmon-Read)
18.02.2018
1
440
C/2018 C2 (Lemmon)
08.04.2018
1
441
C/2018 DO4 (Lemmon)
27.10.2019
1
442
C/2018 EF9 (Lemmon)
20.05.2018
1
443
C/2018 F1 (Grauer)
07.04.2018
1
444
C/2018 F4 (PANSTARRS)
18.04.2018
1
445
P/2018 H2 (PANSTARRS)
02.06.2018
1
446
C/2018 K1 (Weiland)
20.06.2018
1
447
C/2018 KJ3 (Lemmon)
14.08.2018
1
448
C/2018 L2 (ATLAS)
04.12.2018
2
449
P/2018 L4 (PANSTARRS)
03.07.2018
1
450
P/2018 L5 (Leonard)
18.07.2018
1
451
C/2018 M1 (Catalina)
13.07.2018
1
452
C/2018 N1 (NEOWISE)
08.09.2018
3
453
C/2018 N2 (ASASSN)
30.11.2019
8
454
P/2018 P3 (PANSTARRS)
11.09.2018
1
455
P/2018 P4 (PANSTARRS)
04.09.2018
1
456
C/2018 P5 (PANSTARRS)
08.09.2018
1
457
C/2018 R3 (Lemmon)
07.04.2019
1
458
C/2018 U1 (Lemmon)
08.05.2021
6
459
C/2018 V1 (Machholz-Fujikawa-Iwamoto)
04.12.2018
1
460
C/2018 W2 (Africano)
03.09.2019
11
461
C/2018 X2 (Fitzsimmons)
07.03.2019
1
462
C/2018 Y1 (Iwamoto)
30.04.2019
5
463
P/2019 A2 (ATLAS)
29.03.2019
1
464
C/2019 B1 (Africano)
07.03.2019
1
465
P/2019 B2 (Groeller)
07.03.2019
1
466
C/2019 C1 (ATLAS)
22.03.2020
2
467
C/2019 D1 (Flewelling)
05.07.2019
6
468
C/2019 F1 (ATLAS-Africano)
19.04.2020
4
469
C/2019 F2 (ATLAS)
23.04.2019
1
470
C/2019 H1 (NEOWISE)
08.05.2019
1
471
C/2019 J2 (Palomar)
30.06.2019
2
472
C/2019 J3 (ATLAS)
02.07.2019
1
473
C/2019 K4 (Ye)
23.08.2019
4
474
C/2019 K5 (Young)
28.12.2019
3
475
A/2019 K6
16.04.2020
1
476
C/2019 K7 (Smith)
15.04.2021
5
477
C/2019 K8 (ATLAS)
31.08.2019
2
478
C/2019 L1 (PANSTARRS)
01.08.2019
1
479
C/2019 L2 (NEOWISE)
29.06.2019
1
480
C/2019 L3 (ATLAS)
20.03.2022
16
481
P/2019 LD2 (ATLAS)
07.09.2021
1
482
P/2019 LM4 (Palomar)
18.05.2020
2
483
P/2019 M2 (ATLAS)
01.08.2019
1
484
C/2019 M3 (ATLAS)
31.07.2019
1
485
C/2019 N1 (ATLAS)
15.05.2020
6
486
C/2019 O3 (Palomar)
29.08.2022
5
487
2I/2019 Q4 (Borisov)
31.10.2019
1
488
C/2019 S4 (Lemmon)
01.04.2020
1
489
C/2019 T2 (Lemmon)
21.08.2020
2
490
C/2019 T3 (ATLAS)
02.09.2022
8
491
C/2019 T4 (ATLAS)
28.03.2023
3
492
P/2019 T6 (PANSTARRS)
30.11.2019
1
493
C/2019 U5 (PANSTARRS)
27.03.2023
11
494
C/2019 U6 (Lemmon)
05.11.2020
6
495
C/2019 V1 (Borisov)
30.11.2019
1
496
P/2019 X1 (Pruyne)
16.01.2020
1
497
C/2019 Y1 (ATLAS)
18.05.2020
22
498
C/2019 Y4 (ATLAS)
15.05.2020
22
499
C/2020 A2 (Iwamoto)
19.03.2020
3
500
C/2020 B3 (Rankin)
22.03.2020
1
501
C/2020 F2 (ATLAS)
22.02.2023
3
502
C/2020 F3 (NEOWISE)
20.08.2020
7
503
C/2020 F5 (NEOWISE)
24.08.2022
2
504
C/2020 F8 (ATLAS)
19.05.2020
1
505
P/2020 G1 (PIMENTEL)
19.04.2020
1
506
C/2020 H2 (Pruyne)
11.05.2020
1
507
C/2020 H3 (Wierzchos)
19.05.2020
1
508
C/2020 H6 (ATLAS)
02.06.2022
7
509
C/2020 H7 (Lemmon)
28.05.2020
1
510
C/2020 H8 (PANSTARRS)
27.05.2020
1
511
C/2020 J1 (ATLAS)
07.03.2022
3
512
C/2020 K1 (PANSTARRS)
02.09.2022
12
513
C/2020 K3 (Leonard)
18.06.2020
1
514
C/2020 K7 (PANSTARRS)
21.07.2020
1
515
C/2020 K8 (Catalina-ATLAS)
19.06.2020
1
516
P/2020 K9 (Lemmon-PANSTARRS)
20.08.2020
1
517
C/2020 M3 (ATLAS)
14.11.2020
1
518
C/2020 M5 (ATLAS)
22.03.2022
5
519
C/2020 N1 (PANSTARRS)
06.11.2020
2
520
C/2020 O2 (Amaral)
08.08.2021
1
521
C/2020 P3 (ATLAS)
07.03.2021
2
522
C/2020 PV6 (PANSTARRS)
01.09.2021
3
523
C/2020 R2 (PANSTARRS)
05.09.2021
1
524
C/2020 R4 (ATLAS)
30.05.2021
6
525
C/2020 R7 (ATLAS)
27.02.2023
1
526
C/2020 S3 (Erasmus)
14.08.2021
1
527
C/2020 S4 (PANSTARRS)
18.01.2023
4
528
P/2020 S6 (Leonard)
14.11.2020
1
529
C/2020 S8 (Lemmon)
08.05.2021
5
530
C/2020 T2 (Palomar)
30.05.2021
8
531
P/2020 U2 (PANSTARRS)
07.03.2021
1
532
C/2020 U4 (PANSTARRS)
14.11.2022
4
533
C/2020 U5 (PANSTARRS)
21.08.2022
3
534
C/2020 V2 (ZTF)
24.08.2023
14
535
P/2020 V4 (Rankin)
19.02.2022
1
536
P/2020 WJ5 (Lemmon)
21.03.2023
1
537
C/2020 Y2 (ATLAS)
20.04.2021
1
538
C/2020 Y3 (ATLAS)
07.03.2021
1
539
C/2021 A1 (Leonard)
30.05.2021
3
540
C/2021 A2 (NEOWISE)
07.03.2021
1
541
C/2021 A4 (NEOWISE)
06.03.2021
1
542
C/2021 A9 (PANSTARRS)
27.03.2022
1
543
C/2021 C1 (Rankin)
08.03.2021
1
544
C/2021 C3 (Catalina)
08.03.2021
1
545
C/2021 D1 (SWAN)
30.03.2021
2
546
C/2021 D2 (ZTF)
23.02.2022
4
547
C/2021 E3 (ZTF)
03.09.2021
2
548
C/2021 F1 (Lemmon-PANSTARRS)
03.03.2022
2
549
C/2021 K1 (ATLAS)
04.09.2021
1
550
C/2021 L3 (Borisov)
09.03.2022
1
551
P/2021 N2 (Fuls)
08.09.2021
2
552
C/2021 O3 (PANSTARRS)
05.09.2021
3
553
C/2021 P4 (PANSTARRS)
02.06.2022
7
554
C/2021 Q3 (ATLAS)
01.09.2021
1
555
C/2021 Q4 (FULS)
05.09.2022
3
556
P/2021 Q5 (ATLAS)
08.09.2021
1
557
C/2021 QM45 (PANSTARRS)
06.09.2022
2
558
C/2021 S4 (Tsuchinshan)
08.02.2023
1
559
C/2021 S1 (ATLAS)
28.02.2022
2
560
C/2021 T4 (Lemmon)
12.12.2022
3
561
C/2021 U5 (Catalina)
26.03.2022
1
562
P/2021 V2 (Fuls)
17.03.2023
1
563
C/2021 X1 (Maury-Attard)
15.08.2023
1
564
C/2021 Y1 (ATLAS)
17.12.2022
3
565
C/2022 A2 (PANSTARRS)
14.08.2023
4
566
C/2022 A3 (Lemmon-ATLAS)
19.01.2023
1
567
P/2022 C2 (PANSTARRS)
22.03.2022
2
568
P/2022 D1 (PANSTARRS)
27.03.2022
1
569
C/2022 E3 (ZTF)
09.02.2023
15
570
C/2022 J2 (Bok)
17.12.2022
1
571
C/2022 L1 (Catalina)
28.08.2022
4
572
C/2022 L2 (ATLAS)
10.08.2023
3
573
P/2022 L3 (ATLAS)
12.12.2022
6
574
C/2022 N1 (Attard-Maury)
19.07.2022
1
575
C/2022 P1 (NEOWISE)
03.09.2022
3
576
P/2022 P2 (ZTF)
05.09.2022
1
577
C/2022 P3 (ZTF)
08.02.2023
1
578
C/2022 Q2 (ATLAS)
14.11.2022
1
579
C/2022 R3 (Leonard)
16.12.2022
2
580
C/2022 S4 (Lemmon)
15.08.2023
1
581
C/2022 U1 (Leonard)
15.08.2023
2
582
C/2022 U2 (ATLAS)
09.02.2023
4
583
C/2022 U3 (Bok)
13.11.2022
1
584
C/2022 U4 (Bok)
27.03.2023
4
585
C/2022 W2 (ATLAS)
08.02.2023
1
586
C/2022 W3 (Leonard)
07.02.2023
1
587
C/2023 A1 (Leonard)
26.02.2023
2
588
P/2023 B1 (PANSTARRS)
27.03.2023
3
589
C/2023 E1 (ATLAS)
23.08.2023
4
590
C/2023 H2 (Lemmon)
10.08.2023
1
591
C/2023 P1 (Nishimura)
24.08.2023
3