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Pre-Phase A Report - Lisa - Nasa

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58 Chapter 3 Experiment Description<br />

Shot noise limit. Single frequency laser light of significant power from a lightweight<br />

reliable system is best provided by a monolithic Nd:YAG laser pumped by laser diodes.<br />

With this type of laser up to 2 W of light is currently achievable. In order to obtain high<br />

reliability from such a system in a space environment it is reasonable to derate the laser<br />

by a factor of two and use only P = 1 W of output power. The laser system is described<br />

in detail in Section 3.1.5. Using this laser and taking into account the overall optical<br />

efficiency we find that shot noise limits the minimum detectable change 1 to<br />

δx =11×10 −12<br />

3<br />

λ<br />

1064 nm<br />

2 0.3W<br />

ɛPo<br />

1<br />

2 <br />

L<br />

5×10 9 m<br />

30 cm<br />

D<br />

2<br />

m/ √ Hz , (3.2)<br />

where L is the arm length, λ the wavelength and Po the power of the laser, the efficiency<br />

of the optical chain is ɛ, andD is the diameter of the transmitting and receiving optics.<br />

Thus with an optical chain with a realistic efficiency of ɛ =0.3 and a mirror of diameter<br />

of D ≈ 30 cm the target shot-noise performance can be achieved.<br />

3.1.5 Laser system<br />

Introduction. The laser system to be used in the LISA mission is a diode-laser-pumped<br />

monolithic miniature Nd:YAG ring laser which can generate a continuous diffractionlimited<br />

infra-red beam at 1064 µm ofupto2W.<br />

Diode-pumped solid-state lasers, operating in a single transverse mode, are well known<br />

as compact, reliable and highly efficient sources of stable radiation. In the case of the<br />

NPRO (Non Planar Ring Oscillator), TEM 00 mode operation is achieved by focussing the<br />

diode-laser beam into the crystal (see below). When the beamwidth of the diode laser<br />

radiation is smaller than the diameter of the TEM 00 mode in the absorption length of<br />

the pump radiation, the laser is forced to operate in a single transverse mode.<br />

Homogeneously broadened solid-state lasers oscillate on several longitudinal modes even<br />

at low output power because of the spatial hole-burning effect. To enforce single-frequency<br />

operation, resonator internal elements can be applied. However, the additional intracavity<br />

elements strongly reduce the efficiency and stability of the laser system. The monolithic<br />

Nd:YAG ring laser enables single-frequency operation at high output power without intracavity<br />

elements. Unidirectional and hence single-frequency oscillation is enforced by<br />

an intrinsic optical diode.<br />

The optical beam path in the crystal is determined by three total reflections and one<br />

reflection at the negatively curved front surface. The front surface is dielectrically coated,<br />

reflecting about 97 % of the 1064 nm laser radiation and highly transmitting the pump<br />

radiation at 808 nm (see Figure 3.4). The high frequency stability required for the LISA<br />

mission can only be achieved because of the high intrinsic stability of the NPRO (see<br />

Section 3.1.6). This stability results from the monolithic and compact design of the<br />

resonator and from the outstanding properties of host material YAG (Yttrium Aluminum<br />

Garnet Y3Al5O12). Low CTE (7×10−6 K−1 ) and low temperature dependence of the<br />

1The convention above and throughout this paper is that a ‘tilde’ over a quantity indicates that it is<br />

a linear spectral density, e.g. δx is the linear spectral density of δx.<br />

3-3-1999 9:33 Corrected version 2.08

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