-
1
-
-
0033338533
-
Optimization and transfer of vacuum squeezing from an optical parametric oscillator
-
P. K. Lam, T. C. Ralph, B. C. Buchler, D. E. McClelland, H.-A. Bachor, and J. Gao, "Optimization and transfer of vacuum squeezing from an optical parametric oscillator," J. Opt. B 1, 469-474 (1999).
-
(1999)
J. Opt. B
, vol.1
, pp. 469-474
-
-
Lam, P.K.1
Ralph, T.C.2
Buchler, B.C.3
McClelland, D.E.4
Bachor, H.-A.5
Gao, J.6
-
2
-
-
11144285012
-
Optimal optical measurement of small displacements
-
M. T. L. Hsu, V. Delaubert, P. K. Lam, and W. P. Bowen, "Optimal optical measurement of small displacements," J. Opt. B 6, 495-501 (2004).
-
(2004)
J. Opt. B
, vol.6
, pp. 495-501
-
-
Hsu, M.T.L.1
Delaubert, V.2
Lam, P.K.3
Bowen, W.P.4
-
3
-
-
0041663284
-
Quantum noise in laser-interferometer gravitational-wave detectors with a heterodyne readout scheme
-
A. Buonanno, Y. Chen, and N. Mavalvala, "Quantum noise in laser-interferometer gravitational-wave detectors with a heterodyne readout scheme," Phys. Rev. D 67, 122005 (2003).
-
(2003)
Phys. Rev. D
, vol.67
, pp. 122005
-
-
Buonanno, A.1
Chen, Y.2
Mavalvala, N.3
-
4
-
-
0038176789
-
Ground-based interferometric gravitational-wave detectors in the LISA epoch
-
D. Shoemaker, "Ground-based interferometric gravitational-wave detectors in the LISA epoch," Class. Quantum Grav. 20, S11-S22 (2003).
-
(2003)
Class. Quantum Grav
, vol.20
-
-
Shoemaker, D.1
-
5
-
-
84975659930
-
Noise in homodyne and heterodyne detection
-
H. Yuen and V. Chan, "Noise in homodyne and heterodyne detection," Opt. Lett. 8, 177-179 (1983).
-
(1983)
Opt. Lett
, vol.8
, pp. 177-179
-
-
Yuen, H.1
Chan, V.2
-
6
-
-
84893989640
-
-
Excess QN due to nonstationary shot noise can be avoided if the demodulation signal is the reciprocal waveform of the inverse of the modulation signal [7,8] or can be reduced by using an approximation of the reciprocal [9, Because minimum QN heterodyne schemes are technically challenging, homodyne detection is usually chosen
-
Excess QN due to nonstationary shot noise can be avoided if the demodulation signal is the reciprocal waveform of the inverse of the modulation signal [7,8] or can be reduced by using an approximation of the reciprocal [9]. Because minimum QN heterodyne schemes are technically challenging, homodyne detection is usually chosen.
-
-
-
-
7
-
-
0001252757
-
-
B. J. Meers and K. A. Strain, Modulation, signal, and quantum noise in interferometers, Phys. Rev. A 44, 4693-4703 (1991).
-
B. J. Meers and K. A. Strain, "Modulation, signal, and quantum noise in interferometers," Phys. Rev. A 44, 4693-4703 (1991).
-
-
-
-
8
-
-
0000105847
-
Nonstationary shot noise and its effect on the sensitivity of interferometers
-
T. M. Niebauer, R. Schilling, K. Danzmann, A. Rüdiger, and W. Winkler, "Nonstationary shot noise and its effect on the sensitivity of interferometers," Phys. Rev. A 43, 5022-5029 (1991).
-
(1991)
Phys. Rev. A
, vol.43
, pp. 5022-5029
-
-
Niebauer, T.M.1
Schilling, R.2
Danzmann, K.3
Rüdiger, A.4
Winkler, W.5
-
9
-
-
0027589446
-
Harmonic demodulation of nonstationary shot noise
-
M. B. Gray, A. J. Stevenson, H.-A. Bachor, and D. E. McClelland, "Harmonic demodulation of nonstationary shot noise," Opt. Lett. 18, 759 (1993).
-
(1993)
Opt. Lett
, vol.18
, pp. 759
-
-
Gray, M.B.1
Stevenson, A.J.2
Bachor, H.-A.3
McClelland, D.E.4
-
10
-
-
19644400841
-
Squeezing in the audio gravitational-wave detection band
-
K. McKenzie, N. Grosse, W. P. Bowen, S. E. Whitcomb, M. B. Gray, D. E. McClelland, and P. K. Lam, "Squeezing in the audio gravitational-wave detection band," Phys. Rev. Lett. 93, 161105 (2004).
-
(2004)
Phys. Rev. Lett
, vol.93
, pp. 161105
-
-
McKenzie, K.1
Grosse, N.2
Bowen, W.P.3
Whitcomb, S.E.4
Gray, M.B.5
McClelland, D.E.6
Lam, P.K.7
-
11
-
-
33645523461
-
Squeezed state generation for interferometric gravitational-wave detection
-
K. McKenzie, M. B. Gray, S. Goßler, P. K. Lam, and D. E. McClelland, "Squeezed state generation for interferometric gravitational-wave detection," Class. Quantum Grav. 23, S245-S250 (2006).
-
(2006)
Class. Quantum Grav
, vol.23
-
-
McKenzie, K.1
Gray, M.B.2
Goßler, S.3
Lam, P.K.4
McClelland, D.E.5
-
12
-
-
33745782110
-
Coherent control of vacuum squeezing in the gravitational-wave detection band
-
H. Vahlbruch, S. Chelkowski, B. Hage, A. Franzen, K. Danzmann, and R. Schnabel, "Coherent control of vacuum squeezing in the gravitational-wave detection band," Phys. Rev. Lett. 97, 011101 (2006).
-
(2006)
Phys. Rev. Lett
, vol.97
, pp. 011101
-
-
Vahlbruch, H.1
Chelkowski, S.2
Hage, B.3
Franzen, A.4
Danzmann, K.5
Schnabel, R.6
-
13
-
-
84894004667
-
-
It has been brought to our attention that scattered light noise may also limit homodyne detector sensitivity at low frequencies [14, We have not characterized this noise source experimentally
-
It has been brought to our attention that scattered light noise may also limit homodyne detector sensitivity at low frequencies [14]. We have not characterized this noise source experimentally.
-
-
-
-
14
-
-
34547501269
-
-
Max-Planck-Institut für Gravitationsphysik (Albert-Einstein-Institute, Callinstrasse 38, 30167, Hannover, Germany personal communication
-
H. Vahlbruch, Max-Planck-Institut für Gravitationsphysik (Albert-Einstein-Institute), Callinstrasse 38, 30167, Hannover, Germany (personal communication, 2006).
-
(2006)
-
-
Vahlbruch, H.1
-
15
-
-
84950787091
-
A mode selector to suppress fluctuations in laser beam geometry
-
A. Rüdiger, R. Schilling, L. Schnupp, W. Winkler, H. Billing, and K. Maischberger, "A mode selector to suppress fluctuations in laser beam geometry," Opt. Acta 28, 641-658 (1981).
-
(1981)
Opt. Acta
, vol.28
, pp. 641-658
-
-
Rüdiger, A.1
Schilling, R.2
Schnupp, L.3
Winkler, W.4
Billing, H.5
Maischberger, K.6
-
16
-
-
0020764924
-
Laser phase and frequency stabilization using an optical resonator
-
R. W. P. Drever, J. L. Hall, F. V. Kowalski, J. Hough, G. M. Ford, A. J. Munley, and H. Ward, "Laser phase and frequency stabilization using an optical resonator," Appl. Phys. B 31, 97-105 (1983).
-
(1983)
Appl. Phys. B
, vol.31
, pp. 97-105
-
-
Drever, R.W.P.1
Hall, J.L.2
Kowalski, F.V.3
Hough, J.4
Ford, G.M.5
Munley, A.J.6
Ward, H.7
-
17
-
-
0000321301
-
Photodetector designs for low-noise, broadband, and high-power applications
-
M. B. Gray, D. A. Shaddock, C. C. Harb, and H.-A. Bachor, "Photodetector designs for low-noise, broadband, and high-power applications," Rev. Sei. Instrum. 69, 3755-3762 (1998).
-
(1998)
Rev. Sei. Instrum
, vol.69
, pp. 3755-3762
-
-
Gray, M.B.1
Shaddock, D.A.2
Harb, C.C.3
Bachor, H.-A.4
-
18
-
-
84893987994
-
-
B. Lantz, D. Shoemaker, and J. Kerman, Spatial uniformity of silicon photodiodes, LIGO document T952007 (1999), http://www.ligo. caltech.edu/docs/T/T952014-00.pdf.
-
B. Lantz, D. Shoemaker, and J. Kerman, "Spatial uniformity of silicon photodiodes," LIGO document T952007 (1999), http://www.ligo. caltech.edu/docs/T/T952014-00.pdf.
-
-
-
-
19
-
-
84893988424
-
Photodiodes for Initial and Advanced LIGO
-
LIGO document () G980022-00-D
-
P. Csatorday, A. Marin, and M. Zucker, "Photodiodes for Initial and Advanced LIGO," LIGO document (1998) G980022-00-D, http://www.ligo.caltech. edu/docs/G980022-00-D.
-
(1998)
-
-
Csatorday, P.1
Marin, A.2
Zucker, M.3
-
20
-
-
0000463298
-
Sur une propriété nouvelle des ondes lumineuses
-
L. G. Gouy, "Sur une propriété nouvelle des ondes lumineuses," C. R. Acad. Sci. Paris 110, 1251 (1890).
-
(1890)
C. R. Acad. Sci. Paris
, vol.110
, pp. 1251
-
-
Gouy, L.G.1
-
21
-
-
84893998633
-
-
This fit was normalized to maximum value of the experimental data
-
This fit was normalized to maximum value of the experimental data.
-
-
-
-
22
-
-
84894001389
-
-
If the distances were not matched, the QPD might measure the beam when it has a Guoy phase different from that at the homodyne photodetectors and therefore might measure a different contribution of tilt and offset
-
If the distances were not matched, the QPD might measure the beam when it has a Guoy phase different from that at the homodyne photodetectors and therefore might measure a different contribution of tilt and offset.
-
-
-
-
23
-
-
84894004177
-
-
Subtracting the electronic noise below 10 Hz may be misleading, since electronic noise becomes the dominant noise source here.
-
Subtracting the electronic noise below 10 Hz may be misleading, since electronic noise becomes the dominant noise source here.
-
-
-
|