Pre-Phase A Report - Lisa - Nasa
Pre-Phase A Report - Lisa - Nasa
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