Quantum noise of non-ideal Sagnac speed meter interferometer with asymmetries

The speed meter concept has been identified as a technique that can potentially provide laser-interferometric measurements at a sensitivity level which surpasses the standard quantum limit (SQL) over a broad frequency range. As with other sub-SQL measurement techniques, losses play a central role in speed meter interferometers and they ultimately determine the quantum noise limited sensitivity that can be achieved. So far in the literature, the quantum noise limited sensitivity has only been derived for lossless or lossy cases using certain approximations (for instance that the arm cavity round trip loss is small compared to the arm cavity mirror transmission). In this article we present a generalized, analytical treatment of losses in speed meters that allows accurate calculation of the quantum noise limited sensitivity of Sagnac speed meters with arm cavities. In addition, our analysis allows us to take into account potential imperfections in the interferometer such as an asymmetric beam splitter or differences of the reflectivities of the two arm cavity input mirrors. Finally, we use the examples of the proof-of-concept Sagnac speed meter currently under construction in Glasgow and a potential implementation of a Sagnac speed meter in the Einstein Telescope to illustrate how our findings affect Sagnac speed meters with metre- and kilometre-long baselines.

[1]  S. Leavey,et al.  Design of a speed meter interferometer proof-of-principle experiment , 2014, 1405.2783.

[2]  Yanbei Chen,et al.  Quantum limits of interferometer topologies for gravitational radiation detection , 2013, 1305.3957.

[3]  L. Barsotti,et al.  Realistic filter cavities for advanced gravitational wave detectors , 2013, 1305.1599.

[4]  A. Freise,et al.  Realistic polarizing Sagnac topology with DC readout for the Einstein Telescope , 2013, 1303.5236.

[5]  F. Khalili,et al.  Quantum Measurement Theory in Gravitational-Wave Detectors , 2012, Living Reviews in Relativity.

[6]  F. Khalili,et al.  QND measurements for future gravitational-wave detectors , 2009, 0910.0319.

[7]  S. Bose,et al.  Sensitivity studies for third-generation gravitational wave observatories , 2010, 1012.0908.

[8]  R. DeSalvo,et al.  A xylophone configuration for a third-generation gravitational wave detector , 2009, 0906.2655.

[9]  H. Lück,et al.  Review of quantum non-demolition schemes for the Einstein Telescope , 2009 .

[10]  H. Müller-Ebhardt On quantum effects in the dynamics of macroscopic test masses , 2009 .

[11]  S. Danilishin Sensitivity limitations in optical speed meter topology of gravitational-wave antennas , 2003, gr-qc/0312016.

[12]  Yanbei Chen Sagnac interferometer as a speed-meter-type, quantum-nondemolition gravitational-wave detector , 2002, gr-qc/0208051.

[13]  A. Matsko,et al.  Noise in gravitational-wave detectors and other classical-force measurements is not influenced by test-mass quantization , 2001, gr-qc/0109003.

[14]  Yanbei Chen,et al.  Practical speed meter designs for quantum nondemolition gravitational-wave interferometers , 2002, gr-qc/0208049.

[15]  P. Purdue Analysis of a quantum nondemolition speed-meter interferometer , 2002 .

[16]  Berkeley,et al.  Conversion of conventional gravitational-wave interferometers into quantum nondemolition interferometers by modifying their input and/or output optics , 2000, gr-qc/0008026.

[17]  F. Khalili,et al.  Dual-resonator speed meter for a free test mass , 1999, gr-qc/9906108.

[18]  V. Braginsky,et al.  Gravitational wave antenna with QND speed meter , 1990 .

[19]  Schumaker,et al.  New formalism for two-photon quantum optics. I. Quadrature phases and squeezed states. , 1985, Physical review. A, General physics.

[20]  Reza Mansouri,et al.  General Relativity and Gravitation: A Centennial Perspective , 2015 .

[21]  H. Callen,et al.  Irreversibility and Generalized Noise , 1951 .