Differences between revisions 1 and 32 (spanning 31 versions)
Revision 1 as of 2019-08-28 10:22:18
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Revision 32 as of 2019-09-03 18:47:16
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Summary of the morning run == Summary of the morning run ==
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|| Date || GPSTime || IFO config || Main channel || klog ||
|| 2019/08/27 02:09-09:26 || 1250874558 - 1250900778 || Yarm cavity || K1:CAL-CS_PROC_XARM_FREQUENCY_DQ || [[http://klog.icrr.u-tokyo.ac.jp/osl/?r=10135|10135]] ||
|| 2019/08/28 07:54-09:07 || 1250981658 - 1250986038 || FPmi || K1:CAL-CS_PROC_DARM_DISPLACEMENT_DQ || [[http://klog.icrr.u-tokyo.ac.jp/osl/?r=10168|10168]] ||
|| Time (JST) || Time (GPS) || IFO config || Main channel || klog || state flag || Duty Cycle ||
|| 2019/08/27 02:09-09:26 || 1250874558 - 1250900778 || Yarm cavity || (1) || [[http://klog.icrr.u-tokyo.ac.jp/osl/?r=10135|10135]] || || ||
|| 2019/08/28 07:54-09:07 || 1250981658 - 1250986038 || FPMI || (2) || [[http://klog.icrr.u-tokyo.ac.jp/osl/?r=10168|10168]] || K1:GRD-LSC_LOCK_SIMPLE_STATE_N=16 || 100% ||
|| 2019/08/29 07:43-08:46 || 1251067398 - 1251071178 || FPMI || (2) (Some bug) || [[http://klog.icrr.u-tokyo.ac.jp/osl/?r=10184|10184]] || K1:GRD-LSC_FPMI_LOCK_STATE_N=16 || 100% ||
|| 2019/08/30 05:12-08:43 || 1251144738 - 1251157398 || SRMI || (3) (4)(no opt gain and act eff) || [[http://klog.icrr.u-tokyo.ac.jp/osl/?r=10214|10214]] || K1:GRD-LSC_SRFPMI_LOCK_STATE_N=2000 || 64.7% ||
|| 2019/08/31 06:43-10:00 || 1251236598 - 1251248418 || SRMI || (3) (4) || [[http://klog.icrr.u-tokyo.ac.jp/osl/?r=10238|10238]] || K1:GRD-LSC_SRFPMI_LOCK_STATE_N=17 || 100% ||


=== Note for beginner ===

 * Time
  * JST or GPS time

 * IFO config = Interferometer configuration
  * Yarm cavity : Lock the Yarm cavity by feedback to the IMC length (Almost frequency noise evaluated by Yarm length)
  * FPMI : Fabry-Perot Michelson interferometer. The h-of-t signal is calculated from DARM displacement

 * Main channel
  * We should analyze this channel as h(t) channel
  * (1) K1:CAL-CS_PROC_XARM_FREQUENCY_DQ
   * Unit is Hz, because of calculating the IR laser frequency noise
   * Even though Yarm lock, the channel name is XARM. The same strategy to keep the cavity.
  * (2) K1:CAL-CS_PROC_DARM_DISPLACEMENT_DQn
   * --(DARM displacement [nm or m] there are still some bugs in the online model, I will summarize later)-- Fixed(Due to the fail of the filter)
  * (3) K1:CAL-CS_PROC_MICH_DISPLACEMENT_DQ
   * Ogaki-san and cal team sometimes update the optical efficiency and actuator efficiency
  * (4) K1:CAL-CS_PROC_SRCL_DISPLACEMENT_DQ
   * First opt gain and act eff measurement 2019/08/30

 * klog
  * Information related to the run is summarized here

 * state flag = guardian state flag
  * When this state flag and K1:MIF-WE_ARE_DOING_NOTHING = 0 are satisfied, we should analyze data.

 * Memo
  * In the future, we want to do the calibration line injection, PEM injection, add the excitation and check the noise, hardware injection, and so on.
  * We will write following information.

Summary of the morning run

Time (JST)

Time (GPS)

IFO config

Main channel

klog

state flag

Duty Cycle

2019/08/27 02:09-09:26

1250874558 - 1250900778

Yarm cavity

(1)

10135

2019/08/28 07:54-09:07

1250981658 - 1250986038

FPMI

(2)

10168

K1:GRD-LSC_LOCK_SIMPLE_STATE_N=16

100%

2019/08/29 07:43-08:46

1251067398 - 1251071178

FPMI

(2) (Some bug)

10184

K1:GRD-LSC_FPMI_LOCK_STATE_N=16

100%

2019/08/30 05:12-08:43

1251144738 - 1251157398

SRMI

(3) (4)(no opt gain and act eff)

10214

K1:GRD-LSC_SRFPMI_LOCK_STATE_N=2000

64.7%

2019/08/31 06:43-10:00

1251236598 - 1251248418

SRMI

(3) (4)

10238

K1:GRD-LSC_SRFPMI_LOCK_STATE_N=17

100%

Note for beginner

  • Time
    • JST or GPS time
  • IFO config = Interferometer configuration
    • Yarm cavity : Lock the Yarm cavity by feedback to the IMC length (Almost frequency noise evaluated by Yarm length)
    • FPMI : Fabry-Perot Michelson interferometer. The h-of-t signal is calculated from DARM displacement
  • Main channel
    • We should analyze this channel as h(t) channel
    • (1) K1:CAL-CS_PROC_XARM_FREQUENCY_DQ
      • Unit is Hz, because of calculating the IR laser frequency noise
      • Even though Yarm lock, the channel name is XARM. The same strategy to keep the cavity.
    • (2) K1:CAL-CS_PROC_DARM_DISPLACEMENT_DQn
      • DARM displacement [nm or m] there are still some bugs in the online model, I will summarize later Fixed(Due to the fail of the filter)

    • (3) K1:CAL-CS_PROC_MICH_DISPLACEMENT_DQ
      • Ogaki-san and cal team sometimes update the optical efficiency and actuator efficiency
    • (4) K1:CAL-CS_PROC_SRCL_DISPLACEMENT_DQ
      • First opt gain and act eff measurement 2019/08/30
  • klog
    • Information related to the run is summarized here
  • state flag = guardian state flag
    • When this state flag and K1:MIF-WE_ARE_DOING_NOTHING = 0 are satisfied, we should analyze data.
  • Memo
    • In the future, we want to do the calibration line injection, PEM injection, add the excitation and check the noise, hardware injection, and so on.
    • We will write following information.

KAGRA/Subgroups/DET/RUN/MORNINGRUN2019 (last edited 2019-11-21 14:05:15 by chihiro.kozakai)