Introduction to general relativity this energy loss would be too small to be detectable, but this energy loss was observed in 1974 in a binary pulsar called PSR1913+16. In such a system, one of the orbiting stars is a pulsar. This has two consequences: a pulsar is an extremely dense object known as a neutron star, for which gravitational wave emission is much stronger than for ordinary stars. Also, a pulsar emits a narrow beam of electromagnetic radiation from its magnetic poles. As the pulsar rotates, its beam sweeps over the Earth, where it is seen as a regular series of radio pulses, just
Laser beam quality as shown in the figure. However, when a multimode beam is focused, Equation (3) becomes M cannot be determined from a single beam profile measurement. The ISO/DIS 11146 define that M should be calculated from a series of measurements as shown in the figure below. M is measured on real beams by focusing the beam with a fixed position lens of known focal length, and then measuring the characteristics of the beam waist and divergence. These measurements can be taken with a laser beam profiler. The multiple measurements ensure that the minimum beam diameter is found and enable a "curve