1 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo Current status (ELiTES and Geometry of payload) KAGRA(LCGT) cryogenic payload.

Slides:



Advertisements
Similar presentations
9 th /July/2013 Amaldi 10 C3 15:24~15:42 N.KIMURA/KEK Progress on the Cryogenic System for the Interferometric Cryogenic Gravitational Wave Telescope,
Advertisements

11 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo Current status (Experiments in Toshiba, Susupension model, Sapphire fibers,
April 27th, 2006 Paola Puppo – INFN Roma ILIAS Cryogenic payloads and cooling systems (towards a third generation interferometer) part II: the Vibration.
1 Kazuhiro Yamamoto, Dan Chen, Hiroki Tanaka, Takahiro Miyamoto Institute for Cosmic Ray Research (ICRR) the University of Tokyo KAGRA face to face meeting.
11 K. Yamamoto, R. Takahashi, T. Sekiguchi, Y. Sakakibara, C. Tokoku, M. Kamiizumi, U. Iwasaki, T. Uchiyama, S. Miyoki, M. Ohashi, T. Akutsu A, H. Ishizaki.
Cryo-payload Kazuhiro Yamamoto Institute for Cosmic Ray Research
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo Current status (ELiTES and IMPEX sapphire fiber) KAGRA(LCGT) cryogenic payload.
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research (ICRR) the University of Tokyo KAGRA face to face meeting University of Toyama, Toyama, Japan 1 August.
Design study for ET 3rd generation Gravitational Wave Interferometer Work Package 2 Suspension, Thermal noise and Cryogenics Piero Rapagnani
LCGT Cryogenics Status Report KEK T.Suzuki.
11111 K. Yamamoto A, T. Miyamoto A, H. Tanaka A, T. Uchiyama A, S. Zeidler B, A. Hagiwara C, N. Kimura C, R. Kumar C, T. Kume C, I. Murakami C, T. Suzuki.
111 K. Yamamoto, R. Takahashi, T. Sekiguchi, Y. Sakakibara, C. Tokoku, M. Kamiizumi, U. Iwasaki, E. Hirose, T. Uchiyama, S. Miyoki, M. Ohashi, T. Akutsu.
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research (ICRR) the University of Tokyo ELiTES first collaboration meeting Sanjo conference hall, the University.
11111 K. Yamamoto, R. Takahashi A, H. Tanaka, T. Miyamoto, K. Ono, T. Sekiguchi, Y. Sakakibara, M. Kamiizumi, E. Hirose, A. Khalaidovski, R. Kumar, T.
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research (ICRR) the University of Tokyo KAGRA face to face meeting Institute for Cosmic Ray Research, Kashiwa,
Simulation for KAGRA cryogenic payload: vibration via heat links and thermal noise Univ. Tokyo, D1 Takanori Sekiguchi.
1 K. Yamamoto, R. Takahashi, T. Sekiguchi, T. Uchiyama, H. Ishizaki A, A. Takamori B, R. DeSalvo C, E. Majorana D, LCGT collaboration ICRR, NAO A,ERI B,
LCGT Technical Review Suspension Point Interferometer for Parasitic Noise Reduction and an Additional IFO S.Miyoki (ICRR, Univ. of TOKYO)
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research (ICRR) the University of Tokyo KAGRA face to face meeting University of Toyama, Toyama, Japan 1 August.
External forces from heat links in cryogenic suspensions D1, ICRR, Univ. Tokyo Takanori Sekiguchi GWADW in Hawaii.
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo Current status KAGRA(LCGT) cryogenic payload meeting 8 February 2012.
11 K. Yamamoto and KAGRA collaboration Institute for Cosmic Ray Research the University of Tokyo Current status of KAGRA Cryogenic 16 May 2012 Gravitational-Wave.
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo Bulk materials, coating materials for KAGRA ELiTES WP2 meeting 15 June 2012.
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo Report from sub-groups Cryogenic Cryogenic payload 4 August 2011.
ELiTES European Community - Japan Scientist exchange program.
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research (ICRR) the University of Tokyo KAGRA face to face meeting University of Toyama, Toyama, Japan 3 August.
Cryogenic Payload Issues
1 Cryogenic payload 1111 (1)ELiTES WP1 (Cryogenic payload) meeting : 13th of April, 25th of May WP2 meting (Cryogenic mirror): 2nd of May, 15th of June.
2009/6/25Amaldi 8 in NewYork City1 Thermal-noise-limited underground interferometer CLIO Kazuhiro Agatsuma and CLIO Collaborators Institute for Cosmic.
External forces from heat links in cryogenic suspensions D1, ICRR, Univ. Tokyo Takanori Sekiguchi.
Defining the volumes and functions of the cryogenic suspension Discussion guidance Kashiwa October JGW-G
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo Current status KAGRA(LCGT) cryogenic payload meeting 7 March2012.
111 Kazuhiro Yamamoto Institute for Cosmic Ray Research, the University of Tokyo Cryogenic interferometer technologies 19 May 2014 Gravitational Wave Advanced.
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research The University of Tokyo KAGRA external review (Cryogenic payload) 18 April 2012.
GWADW2011 Elba/Italy, 23/May/2011 N. KIMURA and Y. SAKAKIBARA Present Design of LCGT Cryogenic Payload - Status of Cryogenic Design - N. KIMURA*, Y. SAKAKIBARA**,
11 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo Current status (Toshiba, 1/4 cryostat, Sapphire fibers, ELiTES meeting,
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo LCGT internal review (Cryogenic payload) 30 January 2012.
11 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo Current status (Toshiba, ELiTES, Baffle, Brittleness of Maraging, Cryogenic.
11 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo Current status (ELiTES meeting, Guests, Toshiba, Sapphire fibers) KAGRA.
1 Cryogenic payload is not a simple system. We need cryostat to test cryogenic payload performance. 1/4 cryostat will be prepared in Kashiwa campus. 1/4.
Michele Punturo INFN Perugia and EGO 11st ELiTES meeting.
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo LCGT internal review (Cryogenic payload) 30 January 2012.
E. Majorana (INFN – Rome) ELiTES 3 rd General Meeting Hongo Campus – Tokyo – 9-10 Feb., 2015 Cryogenic platform with vertical suspension: a practical approach.
Lessons from CLIO Masatake Ohashi (ICRR, The University of TOKYO) and CLIO collaborators GWADW2012 Hawaii 2012/5/16.
ELiTES ELiTES 3 rd general meeting Interlacing workpackages February 5-7, 2015, Hongo Campus, The University of Tokyo E. Majorana (INFN) ET-LCGT Interferometric.
Status of the cryogenic payload system for baseline KAGRA Rahul Kumar 1, K. Craig 2, K. Yamamoto 2, H. Tanaka 2, T. Miyamoto 2,T. Kajita 2, T. Suzuki 1,
ELiTES 4 th General Meeting Michele Punturo EGO and INFN.
1 Kazuhiro Yamamoto Institute for Cosmic Ray Research (ICRR) the University of Tokyo KAGRA face to face meeting Institute for Cosmic Ray Research, The.
Vibration measurements at KAGRA site
Cryogenic development in KAGRA
Performance test of KAGRA cryostat at site
Overview of the 20K configuration
Pros and cons of cryogenics for Einstein Telescope and Cosmic Explorer
Performance test of KAGRA cryostat at site
Radiation shield vibration measurement at KAGRA site
Status of KAGRA Cryogenics II
Vibration measurements at KAGRA site
External forces from heat links in cryogenic suspensions
Cryogenic Payload Modeling: Vibration via Heat Links
Institute for Cosmic Ray Research The university of Tokyo
Institute for Cosmic Ray Research The University of Tokyo
(Toshiba, 1/4 cryostat, Sapphire fibers, ET meeting, Jena)
Informal meeting of cryogenic payload
Development of vibration isolation systems for LCGT VII
Report from sub-groups Cryogenic Cryogenic payload
Development of vibration isolation systems for LCGT VI
Development of vibration isolation systems for LCGT VI
(Toshiba, 1/4 cryostat, Sapphire fibers, ET meeting, Jena)
Fast cooling of interferometer payload
Cryogenic Payload Modeling: Vibration via Heat Links
Presentation transcript:

1 Kazuhiro Yamamoto Institute for Cosmic Ray Research The university of Tokyo Current status (ELiTES and Geometry of payload) KAGRA(LCGT) cryogenic payload meeting 25 April 2012

2 ELiTES What is the ELiTES ? Grant for collaboration between KAGRA and ET European 7th Framework Programme Marie Curie action (Mar Feb. 2016) European people can visit Japan for KAGRA. For example, Luca Naticchioni will stay on this autumn (at least, one month).

3 ELiTES ELiTES consists of four Working Packages. WP1: Cryogenic payload (E. Majorana) WP2: Cryogenic mirror (R. Nawrodt) Fibers to suspend mirror (In KAGRA, it is included in Crygenic) WP3: Cooling system (K. Somiya) WP4: Organization

4 ELiTES WP1: Cryogenic payload (E. Majorana) Discussion has already started. The first meeting was held on 13th of April. Every month meeting General meeting : 2-3 Aug ? in Japan

5 WP1 structure Task 1.1: Seismic attenuation for underground interferometers  document; month 24; Nikhef, UniSannio, ICRR-UT MARCH 2014 Activities of this task already started are promising in view of the milestone. Task 1.2: Payload design, interface with seismic attenuator  document; month 48; Physics–unirm1, ICRR-UT MARCH 2016 Activities of this task started already but they have to be re-aligned. Task 1.3: Auxiliary attenuation systems for thermal links  document; month 36; Physics–unirm1, ICRR-UT SEPT 2015 Task 1.4: Actuators, sensors and mirror control at room and low temperature  document; month 48; Physics–unirm1, ICRR-UT MARCH 2016 Activities related to this task are progressing in Japan will be reported in May, in order to focus and coordinate KAGRA/ET common efforts. ELiTES

6 WP2: Cryogenic mirror (R. Nawrodt) Mirror, Coating, Fibers to suspend mirror The first meeting will be held on 2nd or 4th of May.

7 ELiTES WP3: Cooling system (K. Somiya) Reduction of cooling and warming time, Radiation shield, Baffles, Mirror contamination and so on

8 ELiTES Mailing lists for WP1,2,3 have already been made. Since the announce was sent, please subscribe to join them. If you did not receive the annouce , let me know.

9 ELiTES Ettore Majorana is here. If you have questions, please ask him now.

10 Geometry of payload (a)Original idea Cold 300 K Cold 300 K (b)Hot platform Platform MirrorRecoil mass Intermediate mass Recoil mass for intermediate mass

11 Geometry of payload Cold 300 K (b)Hot platform Advantage Control and adjustment system at room temperature Initial cooling time is shorter ? Mirror temperature is the same ? Y.Sakakibara calculated.

12 Geometry of payload (a)Original idea Cold 300 K

13 Geometry of payload (b)Hot platform Cold 300 K

14 Geometry of payload (b)Hot platform Cold 300 K

15 Geometry of payload (b)Hot platform Above 150 K (Until 15th day), heat transfer is dominated by radiation. In the best case, it takes 20 days (maybe).

16 Geometry of payload (b)Hot platform Cold 300 K

17 Geometry of payload (b)Hot platform Cold 300 K

18 Geometry of payload (b)Hot platform Cold 300 K External vibration T. Sekiguchi’s calculation Vibration isolation should be better. bKAGRA 3* m/rtHz at 80Hz 3.6* m/rtHz at 30Hz 1.5* m/rtHz at 10Hz

19 Geometry of payload Cold 300 K (b)Hot platform Thermal noise Vertical spring must be cooled (thermal noise).

20 Geometry of payload (b’)Cold platform Cold 300 K Although the platform is cooled, the heat links are connected to intermediate recoil mass, not platform. Heat links between intermediate mass and its recoil mass are not necessary (probably). In this case, this has smaller vibration via heat link than original idea (a) does.

21 Geometry of payload Cold 300 K (b’)Cold platform Temperature change after start of laser operation 20 heat links

22 Geometry of payload (a)Original idea Cold 300 K (c)LIGO (like)

23 Geometry of payload (c)LIGO (like) Advantage : Smaller thermal noise of recoil mass stage Disadvantage : The distance between IM and IMR could be changed when the actuators of the mirror work. This is the problem (for example, the efficiency of the actuators for IM could be changed). Recoil mass Mirror IM IMR

24 Geometry of payload (a)Original idea Cold 300 K (b)Hot platform Cold 300 K Advantage of (b) Control and adjustment system at room temperature Short initial cooling Note Vertical spring at cryogenic temperature and vibration isolation along heat link are necessary (even in original idea (a)).

25 Geometry of payload (a)Original idea Cold 300 K Cold 300 K (b’)Cold platform In the case without heat links between intermediate mass and its recoil mass Smaller vibration via heat link Mirror temperature is enough low if heat load is not so large. (b’) is better than (a) ?

26 Geometry of payload (a)Original idea Cold 300 K (c)LIGO (like) Advantage Smaller thermal noise Disadvantage : The distance between IM and IMR could be changed when the actuators of the mirror work. This is the problem (for example, the efficiency of the actuators for IM could be changed).

27 Geometry of payload There is no reason to adopt original idea (a). (b)Hot platform : Control and adjustment system at room temperature and short initial cooling (b’)Cold platform : Smaller vibration via heat link (c)LIGO (like) : Smaller thermal noise of recoil mass Details of actuators are necessary for discussion.

28 Geometry of payload Please give your opinion