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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 |
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| * What is this? | |
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* 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) |
|
|
2019/08/28 07:54-09:07 |
1250981658 - 1250986038 |
FPMI |
(2) |
K1:GRD-LSC_FPMI_COCK_STATE_N=16 |
|
2019/08/29 07:43-08:46 |
1251067398 - 1251071178 |
FPMI |
(2) (Some bug) |
K1:GRD-LSC_FPMI_COCK_STATE_N=16 |
|
2019/08/30 05:12-08:43 |
1251144738 - 1251157398 |
SRMI |
(3) (4)(no opt gain and act eff) |
K1:GRD-LSC_SRFPMI_LOCK_STATE_N=2000 |
|
2019/08/31 06:43-10:00 |
1251236598 - 1251248418 |
SRMI |
(3) (4) |
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
- 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.