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Averaged backscatter profile from Klett method

2023-05-25 00:00:00 ⇒ 00:59:29

2023-05-25 00:59:59 ⇒ 02:29:59

2023-05-25 02:40:59 ⇒ 03:40:29

2023-05-25 03:41:00 ⇒ 04:40:30

2023-05-25 04:41:00 ⇒ 05:40:29

2023-05-25 05:40:59 ⇒ 06:40:29

2023-05-25 06:41:00 ⇒ 07:40:30

2023-05-25 07:41:00 ⇒ 08:46:59

2023-05-25 08:47:30 ⇒ 09:47:00

2023-05-25 09:47:30 ⇒ 10:46:59

2023-05-25 10:47:29 ⇒ 11:46:59

2023-05-25 11:47:30 ⇒ 12:42:59

Averaged backscatter profile from Raman method

2023-05-25 00:00:00 ⇒ 00:59:29

2023-05-25 00:59:59 ⇒ 02:29:59

2023-05-25 02:40:59 ⇒ 03:40:29

2023-05-25 03:41:00 ⇒ 04:40:30

2023-05-25 04:41:00 ⇒ 05:40:29

2023-05-25 05:40:59 ⇒ 06:40:29

2023-05-25 06:41:00 ⇒ 07:40:30

2023-05-25 07:41:00 ⇒ 08:46:59

2023-05-25 08:47:30 ⇒ 09:47:00

2023-05-25 09:47:30 ⇒ 10:46:59

2023-05-25 10:47:29 ⇒ 11:46:59

2023-05-25 11:47:30 ⇒ 12:42:59

Averaged depolarization ratio profile with Bsc. from Klett method

2023-05-25 00:00:00 ⇒ 00:59:29

2023-05-25 00:59:59 ⇒ 02:29:59

2023-05-25 02:40:59 ⇒ 03:40:29

2023-05-25 03:41:00 ⇒ 04:40:30

2023-05-25 04:41:00 ⇒ 05:40:29

2023-05-25 05:40:59 ⇒ 06:40:29

2023-05-25 06:41:00 ⇒ 07:40:30

2023-05-25 07:41:00 ⇒ 08:46:59

2023-05-25 08:47:30 ⇒ 09:47:00

2023-05-25 09:47:30 ⇒ 10:46:59

2023-05-25 10:47:29 ⇒ 11:46:59

2023-05-25 11:47:30 ⇒ 12:42:59

Averaged depolarization ratio profile with Bsc. from Raman method

2023-05-25 00:00:00 ⇒ 00:59:29

2023-05-25 00:59:59 ⇒ 02:29:59

2023-05-25 02:40:59 ⇒ 03:40:29

2023-05-25 03:41:00 ⇒ 04:40:30

2023-05-25 04:41:00 ⇒ 05:40:29

2023-05-25 05:40:59 ⇒ 06:40:29

2023-05-25 06:41:00 ⇒ 07:40:30

2023-05-25 07:41:00 ⇒ 08:46:59

2023-05-25 08:47:30 ⇒ 09:47:00

2023-05-25 09:47:30 ⇒ 10:46:59

2023-05-25 10:47:29 ⇒ 11:46:59

2023-05-25 11:47:30 ⇒ 12:42:59