Differences between revisions 25 and 29 (spanning 4 versions)
⇤ ← Revision 25 as of 2019-09-01 06:17:21 →
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Editor: TakaakiYokozawa
Comment:
← Revision 29 as of 2019-09-02 15:51:03 → ⇥
Size: 2646
Editor: chihiro.kozakai
Comment:
Deletions are marked like this. Additions are marked like this.
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|| 2019/08/28 07:54-09:07 || 1250981658 - 1250986038 || FPMI || (2) || [[http://klog.icrr.u-tokyo.ac.jp/osl/?r=10168|10168]] ||                                     ||
|| 2019/08/29 07:43-08:46 || 1251067398 - 1251071178 || FPMI || (2) (Some bug) || [[http://klog.icrr.u-tokyo.ac.jp/osl/?r=10184|10184]] ||                                     ||		 || 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_FPMI_LOCK_STATE_N=16 ||
|| 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 ||
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== Summary of the morning run ==

|| Time (JST) || Time (GPS) || IFO config || Main channel || klog || Memo ||
|| 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]] || Silent run ||
|| 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]] || Silent run ||
|| 2019/08/29 07:43-08:46 || 1251067398 - 1251071178 || FPMI || K1:CAL-CS_PROC_DARM_DISPLACEMENT_DQ (Some bug) || [[http://klog.icrr.u-tokyo.ac.jp/osl/?r=10184|10184]] || Silent run ||
|| 2019/08/30 05:12-08:43 || 1251144738 - 1251157398 || SRMI || K1:CAL-CS_PROC_(MICH/SRCL)_DISPLACEMENT_DQ || [[http://klog.icrr.u-tokyo.ac.jp/osl/?r=10214|10214]] || Silent run ||
=== 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_DQ
   * --(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 gain and actuator efficiency
  * (4) K1:CAL-CS_PROC_SRCL_DISPLACEMENT_DQ
   * First optical gain and actuator efficiency by Ogaki-san and Yamat-san 2019/08/30
Line 63: Line 35:
 * state flag
  * guardian state flag
Line 64: Line 39:
  * What is this?
Line 67: Line 41:


 * klog
  * Information related to the run is summarized here

 * Memo
  * What is this?
  * 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

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_FPMI_LOCK_STATE_N=16

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

1251067398 - 1251071178

FPMI

(2) (Some bug)

10184

K1:GRD-LSC_FPMI_LOCK_STATE_N=16

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

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

1251236598 - 1251248418

SRMI

(3) (4)

10238

K1:GRD-LSC_SRFPMI_LOCK_STATE_N=17

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_DQ

      • 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
  • 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)