Differences between revisions 23 and 38 (spanning 15 versions)
Revision 23 as of 2011-06-06 21:43:11
Size: 2017
Editor: KiwamuIzumi
Comment:
Revision 38 as of 2011-06-07 21:07:55
Size: 4285
Editor: KiwamuIzumi
Comment:
Deletions are marked like this. Additions are marked like this.
Line 12: Line 12:
[[BR]]
Line 13: Line 14:
[[BR]] <<Anchor(plantop)>>  <<Anchor(plantop)>>
Line 15: Line 16:
== Schnupp asymmetry measurement == == Schnupp asymmetry measurement and its adjustment ==
Line 17: Line 18:
  . {{{
 Schnupp asymmetry = 0.0342 [m] +/- XXX [mm]
}}}
 . The Schnupp asymmetry determines the reflectivity '' r ''and transmissivity '' t '' of the Michelson for the f1 and f2 sidebands when the carrier is kept in the dark condition. In the design ''' the f2 sideband should be critical coupling in the dual recycling cavity '''[#ref1 [1]] [#ref2 [2]]. To achieve the critical coupling we should adjust '' r '' and '' t'' properly.

 . According to a simulation the asymmetry should be within the precision of XXX mm to achieve more than 95 % of the power build up.
Line 18: Line 26:
 . Here is an instruction how to measure the Schnupp asymmetry.
Line 19: Line 28:
 . The result at the 40m was ... and the precision was +/- XXX mm. This implies us to fix the length of the asymmetry.

Line 21: Line 33:
== Cavity length measurements == ------
== PRC length measurement and its adjustment ==
Line 23: Line 36:
 . {{{ lprc = 6.7538 [m] +/- XXX [mm]
}}}
 . In order to successfully lock a power recycled interferometer with Fabry-Perot arms a technique broadly used is to choose the PRC length such that the sidebands are resonate in PRC. In our design the PRC length has been chosen to let both f1 and f2 sidebands resonate in PRC [#ref1 [1]] [#ref2 [2]].
Line 24: Line 41:
 . To measure the length of the recycling cavity,
Line 25: Line 44:
 .
Line 27: Line 47:
== Recycling gain measurements == ------
== SRC length measurement ==
=== Requirements ===
 . {{{ lsrc = 5.39915 [m] +/- XXX mm
 }}}
Line 29: Line 53:
 .
Line 30: Line 55:
 .
Line 33: Line 59:
------
== Recycling gain measurements ==
 . Since the recycling gain is related to loss in the recycling cavity,...
=== How to ===
 .
=== Results ===
 . {{{
 Carrirer = XX
 f1 sideband = YY
 f2 sideband = ZZ
}}}
[[BR]][[BR]]

------
== Beam spot position on BS ==
=== Requirements ===
{{{ off-centering < XXX mm
}}}
 . To get a clean AS signal

=== How to ===
=== results ===

[[BR]][[BR]]
------
Line 38: Line 89:
------
Line 44: Line 95:
------
Line 49: Line 101:
------
Line 55: Line 108:
------
Line 60: Line 114:
== Estimation of Suspensions' Position ==
=== Requirements ===
=== How to ===
=== Results ===
[[BR]][[BR]]
------
Line 68: Line 117:
Line 69: Line 119:
------
Line 72: Line 122:
 . {{{ Precision < 1 % (?)
}}}

 . When the DRMI is locked the MICH control signal is fed back to the BS actuator, but the actuation on BS intrinsically changes the PRC and SRC length as well as the MICH length ('' lx-ly''). This means the noise from MICH can be transferred to the PRC and SRC, resulting in the degradation of noise performance in the PRC and SRC [#ref3 [3]].
 . To avoid the coupling the MICH control should also actuate on PRM and SRM to minimize the coupling.
Line 75: Line 131:
[[BR]]
[[BR]]
------
= References =
<<Anchor(ref1)>>
[1] https://dcc.ligo.org/cgi-bin/private/DocDB/ShowDocument?docid=12213
Line 76: Line 138:
<<Anchor(ref2)>>
[2]

<<Anchor(ref3)>>
[3]
[[BR]]
[[BR]]

Interferometer Characterization at the 40m prototype

Goals

  • To help the DRMI commissioning that will be performed at LLO.

Motivations

  • In the aLIGO schedule a DRMI test will start on May 2011 at LLO. Prior to the DRMI test we, the 40m lab, should help their commissioning to make the things smooth and hence allow to finish the commissioning in the shortest time. Moreover any commissioning tests that will be performed at LLO should be well predicted and tested at the 40m so that the people at the site can easily pass through all the commissioning tests and possibly can spend time for a real trouble shooting (commissioning) to fix unexpected issues.

  • So for this purpose some recipes must be prepared by the 40m lab. Each recipe includes descriptions about how to make a commissioning test, how to estimate important parameters and the results at the 40m. Additionally some useful scripts must be developed at the 40m.

BR BR

BR


DRMI Characterization Plan at the 40m

Schnupp asymmetry measurement and its adjustment

Requirement

  •  Schnupp asymmetry = 0.0342 [m] +/- XXX [mm]
  • The Schnupp asymmetry determines the reflectivity r and transmissivity t of the Michelson for the f1 and f2 sidebands when the carrier is kept in the dark condition. In the design the f2 sideband should be critical coupling in the dual recycling cavity [#ref1 [1]] [#ref2 [2]]. To achieve the critical coupling we should adjust r and t properly.

  • According to a simulation the asymmetry should be within the precision of XXX mm to achieve more than 95 % of the power build up.

How to

  • Here is an instruction how to measure the Schnupp asymmetry.

Results

  • The result at the 40m was ... and the precision was +/- XXX mm. This implies us to fix the length of the asymmetry.

BRBR


PRC length measurement and its adjustment

Requirements

  • {{{ lprc = 6.7538 [m] +/- XXX [mm]

}}}

  • In order to successfully lock a power recycled interferometer with Fabry-Perot arms a technique broadly used is to choose the PRC length such that the sidebands are resonate in PRC. In our design the PRC length has been chosen to let both f1 and f2 sidebands resonate in PRC [#ref1 [1]] [#ref2 [2]].

How to

  • To measure the length of the recycling cavity,

Results

BRBR


SRC length measurement

Requirements

  • {{{ lsrc = 5.39915 [m] +/- XXX mm }}}

How to

Results

BRBR


Recycling gain measurements

  • Since the recycling gain is related to loss in the recycling cavity,...

How to

Results

  •  Carrirer    = XX
     f1 sideband = YY
     f2 sideband = ZZ

BRBR


Beam spot position on BS

Requirements

{{{ off-centering < XXX mm }}}

  • To get a clean AS signal

How to

results

BRBR


Reflectivity check

How to

Results

BRBR


Sensing matrix check

How to

Results

BRBR


Calibration of Actuator responses

How to

Results

BRBR


f2a filter adjustment

Requirement

How to

Results

BRBR


IFO modeling

How to

Results

BRBR


Locking procedure

How to

BRBR


MICH actuator decoupling

Requirements

  • {{{ Precision < 1 % (?)

}}}

  • When the DRMI is locked the MICH control signal is fed back to the BS actuator, but the actuation on BS intrinsically changes the PRC and SRC length as well as the MICH length ( lx-ly). This means the noise from MICH can be transferred to the PRC and SRC, resulting in the degradation of noise performance in the PRC and SRC [#ref3 [3]].

  • To avoid the coupling the MICH control should also actuate on PRM and SRM to minimize the coupling.

How to

BR BR BR BR


References

[1] https://dcc.ligo.org/cgi-bin/private/DocDB/ShowDocument?docid=12213

[2]

[3] BR BR [#plantop back to top]

Interferometer_Characterization (last edited 2012-03-11 03:31:49 by KiwamuizumiATligoDOTorg)