This contribution is part of the special series of Inaugural Articles by members of the National Academy of Sciences elected on April 25, 2006. Contributed by V. B. Braginsky, November 29, 2006 (sent for review October 30, 2006) It is reasonable to regard the experiments performed by C. Coulomb and H. Cavendish in the end of the 18th century as the beginning of laboratory experimental physics. These outstanding scientists have measured forces (accelerations) produced by electric charges and by gravitational ''charges'' on probe masses that were attached to torque balance. Among the variety of different research programs and projects existing today, experiments with probe masses are still playing an important role. In this short review, the achieved and planned sensitivities of very challenging LIGO (Laser Interferometer Gravitational wave Observatory) and LISA (Laser Interferometer Space Antennae) projects are described, and a list of nonsolved problems is discussed as well. The role of quantum fluctuations in high precision measurements is also outlined. Apart from these main topics, the limitations of sensitivity caused by cosmic rays and the prospects of clock frequency stability are presented.gravitational waves ͉ measurement
I. Classical and Quantum Limitations of Sensitivity in the Experiments with Probe MassesI n the simplest classical ''case,'' when a probe mass (PM) m p is coupled with a heat-bath by means of friction H, the FluctuationDissipation Theorem (FDT) gives the limit for detectable value of AC accelerationwhere T is the heat-bath temperature, k B is the Boltzmann constant, and ⌬f is the bandwidth of force acting on the PM F ϭ m p ⅐a PM . Equation 1 is valid when the parameter H does not depend on frequency and if the time interval (averaging time) is equal to Ӎ (⌬f ) Ϫ1 . If PM is in the absolute vacuum (no mechanical contact with the entourage-envelope), then the remaining fluctuating force acting on PM is the AC component of thermal radiation pressure F THERM from the entourage if T Ͼ 0. This effect is a classical one (i.e., it exists due to fluctuations of envelope temperature in thermal equilibrium). This small effect will be discussed in Section III.Simple calculations [almost 40 years old (1)] give another limit for the detectable force F ϭ m p ⅐a PM , which acts on PM. This limit is of quantum origin; it depends on the chosen observable of the measuring device (meter). If PM is a part of the mechanical oscillator whose eigenfrequency is m , and if F ϭ F 0 sin m t during time interval , then using an optical Fabry-Perot resonator pumped by a laser as a continuous monitor of the coordinate, it is possible to measure the amplitude (1)
[2]The term ''Standard Quantum Limit'' (SQL) was coined by K. S. Thorne. This limit can be obtained only provided that laser pumping power in the meter is equal to the optimal value:where R is the mirrors reflectivity, c is the speed of light, and optic is the laser frequency. If W is smaller or higher than W optim , then the variance of output signal w...