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Averaged backscatter profile from Klett method

2022-11-30 00:00:15 ⇒ 01:00:50

2022-11-30 01:01:21 ⇒ 02:02:06

2022-11-30 02:02:37 ⇒ 03:03:12

2022-11-30 03:03:43 ⇒ 04:04:16

2022-11-30 04:04:46 ⇒ 05:04:47

2022-11-30 05:05:18 ⇒ 05:59:46

2022-11-30 06:00:17 ⇒ 07:00:39

2022-11-30 07:01:09 ⇒ 08:01:44

2022-11-30 08:02:14 ⇒ 09:02:35

2022-11-30 09:03:05 ⇒ 10:03:23

2022-11-30 10:03:54 ⇒ 11:04:17

2022-11-30 11:04:47 ⇒ 11:52:57

Averaged backscatter profile from Raman method

2022-11-30 00:00:15 ⇒ 01:00:50

2022-11-30 01:01:21 ⇒ 02:02:06

2022-11-30 02:02:37 ⇒ 03:03:12

2022-11-30 03:03:43 ⇒ 04:04:16

2022-11-30 04:04:46 ⇒ 05:04:47

2022-11-30 05:05:18 ⇒ 05:59:46

2022-11-30 06:00:17 ⇒ 07:00:39

2022-11-30 07:01:09 ⇒ 08:01:44

2022-11-30 08:02:14 ⇒ 09:02:35

2022-11-30 09:03:05 ⇒ 10:03:23

2022-11-30 10:03:54 ⇒ 11:04:17

2022-11-30 11:04:47 ⇒ 11:52:57

Averaged depolarization ratio profile with Bsc. from Klett method

2022-11-30 00:00:15 ⇒ 01:00:50

2022-11-30 01:01:21 ⇒ 02:02:06

2022-11-30 02:02:37 ⇒ 03:03:12

2022-11-30 03:03:43 ⇒ 04:04:16

2022-11-30 04:04:46 ⇒ 05:04:47

2022-11-30 05:05:18 ⇒ 05:59:46

2022-11-30 06:00:17 ⇒ 07:00:39

2022-11-30 07:01:09 ⇒ 08:01:44

2022-11-30 08:02:14 ⇒ 09:02:35

2022-11-30 09:03:05 ⇒ 10:03:23

2022-11-30 10:03:54 ⇒ 11:04:17

2022-11-30 11:04:47 ⇒ 11:52:57

Averaged depolarization ratio profile with Bsc. from Raman method

2022-11-30 00:00:15 ⇒ 01:00:50

2022-11-30 01:01:21 ⇒ 02:02:06

2022-11-30 02:02:37 ⇒ 03:03:12

2022-11-30 03:03:43 ⇒ 04:04:16

2022-11-30 04:04:46 ⇒ 05:04:47

2022-11-30 05:05:18 ⇒ 05:59:46

2022-11-30 06:00:17 ⇒ 07:00:39

2022-11-30 07:01:09 ⇒ 08:01:44

2022-11-30 08:02:14 ⇒ 09:02:35

2022-11-30 09:03:05 ⇒ 10:03:23

2022-11-30 10:03:54 ⇒ 11:04:17

2022-11-30 11:04:47 ⇒ 11:52:57