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QUANTUM NONDEMOLITION MEASUREMENTS IN SYSTEMS ETC.
603
The system equations of motion are (fig. 1)
J~ + 0 9 2 2 -- --
2y(E1 sin (At + 9) + / ~ cos (At + 9)) +fg(t),
The action of the last cascade measuring device is modelled by gedanken state reduction of the system. There are difficulties in treating continuous approximate measurements this way. At the same time, the formal description of those measurements(~6) is cumbersome and nonobvious from the physical point of view. In our model we consider the whole measuring scheme: detector, meter and measuring device (fig. 1). The latter consists of three circulators, a homodyne detector and two degenerate parametric amplifiers (or four wave mixers) with different pump frequencies. According to the ideas of ref. (7-9) the homodyne detector measures the quadrature component of the readout system outgoing radiation, two degenerate parametric amplifiers (or four wave mixers) squeeze in a special way the vacuum fluctuations of the load and the circulators direct the fields into appropriate branches of the system. More concretely, the system outgoing field is directed through circulators C1, C2 and C3 into the load (absorber black-body with zero temperature) and dissipates in it. Zero fluctuations of the load enter through circulators C3 the degenerate parametric amplifier DPA2 with pump frequency 2(~o0+ 2A) and bandwidth A~<~ lzll, then get through circulators C3 and C2 into DPA1 with pump frequency 2~0 and bandwidth A~ ~< ]AI and then get through circulators C2 and C1 into the system.
IL NUOVO CIMENTO
VOL. 10 C, N. 6
Novembre-Dicembre 1987
Quantum Nondemolition Measurements in Systems with Nonstationary Squeezing of Quantum Noise.
V. V. KULAGIN and V. N. RUDENK0 Moscow State University, Department of Physics - 117234 Moscow, USSR
F~ q.1 ~- §
mh~o~)l~,
w h e r e ~ is the duration of external (gravitational) force; m, ~o~ are mass and resonant frequency of the W e b e r detector. Usually only two first cascades of antenna probe oscillator (detector) and readout system (meter) are considered in the quantum mechanics framework (24). (1) V. B. BRAGINSKY,V. P. MITROFANOV,V. I. PANOV: Systems with Small Dissipation, in Russian (Nauka, Moscow, 1981) (English translation: University of Chicago Press, Chicago, Ill., 1985). (2) C. M. CAVES, K. S. THORNE, R. W. P. DREVER, V. D. SANDBERG and M. ZIMMERMANN: Rev. Mod. Phys., 52, 341 (1980). (3) G. J. MILBURN, A. S. LANE and D. F. WALLS: Phys. Rev. A, 27, 2804 (1983). (4) V. V. DODONOV, V. V. KULAGIN, V. I. MAN'KO and V. N. RUDENKO: Experimental Tests of Gravitational Theories, ed. M.S.U., 1987 (to be published).
9 now is the arbitrary phase and we take for simplicity Itll--)0 but EL" Itll = const; EL is the input laser field. A system like (2) was considered earlier with Ebl, Eb2 to be a white stationary noise (1~,13). In our analysis Eb.a. is the squeezed noise with two points of squeezing: 090and ~Oo+ 2A. Let the back-action noise have the form (6) (lo) C. (11) C. (15) A. (~) A.
Eb.a. = Ebl COS090 t +/~b2 sin 090t
= E1 cos 090t +/i~2 sin ommutation relations(l~ The laser field inside the cavity has the form (5) Ep = E0 sin (09vt + 9),
Quantum nondemolition m e a s u r e m e n t s are the only possibility to increase the sensitivity of a W e b e r detector above the standard quantum limit (1,2) (1)
40 - I1 Nuovo Cimento C.
601
602
r
v.v.
= - r o ~t = i t o
KULAGIN and v. N. RUDENKO
1 2w o
12(wo+2A)
Fig. 1 -Gravitational antenna with measuring device. C1, C2, C3 are circulators; DPA1 and DPA2 are the narrow-bandwidth degenerate parametric amplifiers (or four wave mixers); LP is the laser pump; M1 and M2 are fixed and moving mirrors; HD is the homodyne detector; L is the load (absorber).
(5) A. BARCHIELLI, L. LANZ and G. M. PROSPERI: Found. Phys., 13, 779 (1983). (6) A. BARCHIELLI:P h y s . Roy. D, 32, 347 (1985). (7) B. YURKE and J. DENKER: Physica (Utrecht) B, 198, 1359 (1981). (8) B. YURKE and L. R. CORRUCCINI:Phys. Rev. A, 39, 895 (1984). (9) B. YURKE: J. Opt. Soc. Am. B, 2, 732 (1985).
/ ~ + ~E~ + 2~2 cos(At + 9) = 2~fl~b~, (2) E~. + ~fl~2 - 2flJ~ sin (At + 9) = 2~ Eb2, ~~o Eo 21 ' SEo Y=4mnt~' A=09p--oJo,
where E0 is the amplitude of the field inside optical resonator under the action of the ,,laser force, with mirrors fixed; S is the cross-section of the beam; M, 09~are the mass and frequency of the mechanical oscillator; l, 090 are the length and the eigenfrequency of the optical resonator; ~e, is the damping of the optical resonator due to the right mirror (with r0 < 1); )~ is the coordinate operator of the moving mirror; ~opis the frequency of the pump; fg(t) = F(t)/m, F(t) is the external (gravitational) force;/~,/~e and/~b~,/~b2 are the quadrature component operators of the measuring field/~ (3) and back-action field Eb.a. (4)